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<strong>National</strong> <strong>Superconducting</strong><br />

Cyclotron Laboratory<br />

at Michigan State University<br />

2008<br />

<strong>Graduate</strong> Studies


<strong>NSCL</strong><br />

Welcome<br />

I have enjoyed working in nuclear science for most of<br />

my life. It has been a fabulous journey and the field has<br />

made enormous advances since my student days 40<br />

years ago. Yet, nuclear science today seems more dynamic<br />

and more interesting to me than it seemed then.<br />

Breakthrough technologies will allow us to address important<br />

questions that seemed out of reach even a decade<br />

ago.<br />

Konrad Gelbke, <strong>NSCL</strong> Director<br />

• Largest university campus-based nuclear science<br />

laboratory in the United States<br />

• Training ground for 10% of all U.S. nuclear science<br />

doctoral students<br />

• <strong>Graduate</strong> program in nuclear physics ranked No. 2<br />

by U.S. News and World Report<br />

• <strong>NSCL</strong> graduate students complete their Ph.D.s 1.5<br />

years faster than the national average<br />

• World-leading facility for the production and study<br />

of rare isotopes<br />

• <strong>National</strong> Science Foundation-funded user facility,<br />

with 700 users from 35 countries<br />

• Opportunities for hands-on research and meaningful<br />

scholarly collaboration<br />

Many of these questions center around rare isotopes,<br />

unstable nuclei that play an important if fleeting role in<br />

the cosmos. For decades, inadequate knowledge of<br />

important nuclear properties has limited understanding<br />

of astrophysical processes that forge the elements<br />

– and, hence, the atoms we and the visible world are<br />

made of. However, thanks to technology developed at<br />

<strong>NSCL</strong> and other world-leading laboratories, and investments<br />

in more capable accelerator facilities, the next<br />

generation of nuclear scientists will have at their disposal<br />

an impressive arsenal of tools. The result will be pathbreaking<br />

exploration of a large and so far unexplored<br />

part of the nuclear landscape – the terra incognita of<br />

rare isotopes – that will provide critical tests of our best<br />

theories and shed light on the astrophysical processes<br />

that formed the elements in our solar system.<br />

<strong>NSCL</strong> and other labs around the world are developing<br />

state-of-the-art tools for experimenters and theorists –<br />

powerful accelerators, sensitive detectors, advanced<br />

computer hardware and software – that will push the<br />

bounds of basic science and, at the same time, provide<br />

outstanding education and research opportunities<br />

for graduate students and postdoctoral researchers.<br />

Rare isotope research has important cross-disciplinary<br />

linkages to other fields of science such as astrophysics,<br />

biomedicine, national and international security,<br />

energy, materials science and quantum information<br />

processing.<br />

In short, the future of nuclear science is bright, and<br />

Michigan State University’s graduate program in nuclear<br />

and accelerator science offers attractive prospects<br />

for a future science career.<br />

Konrad Gelbke, Director<br />

02<br />

www.nscl.msu.edu


<strong>NSCL</strong><br />

Table of Contents<br />

02 Welcome<br />

03 Table of Contents<br />

04 Nuclear Science at MSU<br />

05 <strong>Graduate</strong> <strong>Student</strong> Life<br />

06 Lab Facilities<br />

07 Lab History & Future Plans<br />

08 Careers in Nuclear Science<br />

09 Admissions<br />

10 Faculty<br />

11 Faculty Profiles<br />

39 <strong>NSCL</strong> in the News<br />

40 Michigan State University<br />

42 Lansing Area<br />

43 Maps<br />

45 Useful Links<br />

www.nscl.msu.edu<br />

03


<strong>NSCL</strong><br />

Nuclear Science at MSU<br />

To probe the mysteries of an atom’s nucleus<br />

is to seek answers to some of the most fundamental<br />

of questions about how the elements<br />

were formed and what keeps nuclei together.<br />

Nuclear science pursues these big questions<br />

by colliding and examining the tiniest of particles.<br />

In collisions at half the speed of light, new<br />

isotopes are created in a billionth of a trillionth<br />

of one second. To do this, scientists need particle<br />

accelerators, state-of-the-art computers,<br />

and specially designed equipment.<br />

Research at <strong>NSCL</strong> concentrates on the study<br />

of exotic nuclei, one of the current frontiers in<br />

nuclear science. Compared to the more familiar<br />

stable nuclei, these exotic nuclei have<br />

large excesses of either protons or neutrons<br />

and tend to decay quickly, sometimes within<br />

fractions of seconds. Experimental groups use<br />

the world leading capabilities of cyclotrons at<br />

<strong>NSCL</strong> to produce exotic nuclei through fragmentation<br />

of accelerated stable nuclei that<br />

bombard a solid target. The exotic fragments<br />

are transported to the experimental stations<br />

within hundreds of nanoseconds, where a<br />

wide range of experiments can be carried out<br />

using state-of-the art equipment. Some experiments<br />

determine the existence of a particular<br />

nucleus for the first time, while others stop<br />

the nuclei to study their decay or to measure<br />

their mass. Yet other experiments<br />

have the exotic nuclei bombard<br />

another target and study the ensuing<br />

nuclear reactions<br />

revealing information<br />

about the internal structure<br />

of the nucleus, or the behavior of nuclear<br />

matter during the extreme temperatures and<br />

densities encountered in a nuclear collision.<br />

Already such experiments have revealed<br />

many surprising properties of exotic nuclei<br />

and many more remain to be discovered.<br />

<strong>NSCL</strong> theorists are working closely with experimentalists<br />

to interpret these results and to<br />

use exotic nuclei as probes to uncover hidden<br />

aspects of the nuclear force that holds<br />

together all atomic nuclei. Understanding this<br />

force and building a nuclear theory that can<br />

predict the properties of nuclei is one of the<br />

ultimate goals in nuclear science.<br />

Exotic nuclei also play an important role in astrophysics.<br />

They are created in stellar explosions<br />

such as X-ray bursts and supernovae, and<br />

they might exist inside neutron stars. Often the<br />

decays of exotic nuclei are intermediate steps<br />

in the astrophysical processes that created the<br />

elements in nature. Many <strong>NSCL</strong> groups work<br />

at the intersection of nuclear physics and astrophysics<br />

to address<br />

open questions<br />

raised<br />

by astron<br />

o m i c a l<br />

observations<br />

concerning<br />

the<br />

origin of the<br />

elements, the nature of stellar explosions, and<br />

the properties of neutron stars. This research<br />

combines <strong>NSCL</strong> experiments, nuclear theory,<br />

astrophysical models, and observations.<br />

04<br />

www.nscl.msu.edu


<strong>NSCL</strong><br />

<strong>Graduate</strong> <strong>Student</strong> Life<br />

<strong>Graduate</strong> students at <strong>NSCL</strong> have outstanding<br />

opportunities to do research at a national<br />

laboratory located on the campus of a major<br />

research university. The strong interaction<br />

between the experimental and theoretical<br />

scientists and the frequent visitors and users<br />

of the facility creates an open and academically<br />

stimulating atmosphere. <strong>NSCL</strong> is widely<br />

recognized for its cutting-edge research in<br />

nuclear science, nuclear astrophysics, accelerator<br />

physics and engineering, as evidenced<br />

by a large number of publications in highquality<br />

refereed journals and invited talks at<br />

national and international conferences. Most<br />

graduate students are financially supported<br />

with research assistantships when working on<br />

thesis projects. Exceptional students can be<br />

awarded an <strong>NSCL</strong> fellowship.<br />

As the premier rare isotope<br />

facility in the U.S.<br />

for the next decade,<br />

<strong>NSCL</strong> is a high national<br />

priority, as expressed<br />

in the number-one<br />

recommendation in<br />

the 2002 Long Range<br />

Plan of the DOE/NSF<br />

Nuclear Science Advisory<br />

Committee. Experimental<br />

and theoretical<br />

insight gained at <strong>NSCL</strong> will be highly<br />

relevant for the next generation rare isotope<br />

facility.<br />

<strong>Graduate</strong> students in experimental nuclear<br />

science will be involved in all aspects of performing<br />

an experiment at <strong>NSCL</strong>: writing a proposal<br />

which will be reviewed by an external<br />

Program Advisory Committee, designing the<br />

experiment, setting up the hardware and electronics,<br />

writing data acquisition and analysis<br />

code, analyzing and interpreting the results,<br />

and finally writing a manuscript for a peer-reviewed<br />

journal. Theory students have access<br />

to world experts<br />

who frequently<br />

visit the laboratory<br />

and collaborate<br />

closely<br />

with local faculty.<br />

The Joint<br />

Institute for Nuclear<br />

Astrophysics<br />

offers the unique opportunity to work on<br />

the interface between nuclear physics and<br />

astrophysics.<br />

Our graduate students routinely present their<br />

new results at important national or international<br />

conferences. This provides exposure to<br />

senior colleagues and helps in finding new job<br />

opportunities after graduation.<br />

<strong>Graduate</strong> students take an active part in the<br />

organization and daily business of <strong>NSCL</strong>, and<br />

are represented on most laboratory committees.<br />

<strong>NSCL</strong> graduate students administer<br />

their own office space, furniture, and desktop<br />

computers. The graduate students meet<br />

weekly and organize their own seminar series.<br />

They also contribute to many of<br />

the outreach activities offered<br />

through <strong>NSCL</strong> and participate in<br />

the governance process<br />

of the College of Natural<br />

Science and the Council<br />

of <strong>Graduate</strong> <strong>Student</strong>s.<br />

www.nscl.msu.edu<br />

05


<strong>NSCL</strong><br />

Lab Facilities<br />

Imagination, creativity and scientific knowledge<br />

are the lifeblood of nuclear physics research,<br />

but the equipment is the skeleton that<br />

brings form and substance to science. <strong>NSCL</strong><br />

has been at the forefront of developing technology<br />

that makes nuclear science a reality.<br />

Beams of atomic nuclei are made in the ion<br />

source and accelerated in the K500 and<br />

K1200 cyclotrons. The rare isotopes, which are<br />

our specialty,<br />

are selected<br />

by the A1900<br />

fragment separator.<br />

When the<br />

beam of rare<br />

isotopes hits<br />

the target, the<br />

reaction products<br />

are measured with special detectors.<br />

For example, the S800 spectrograph<br />

can identify the exotic<br />

fragments produced and<br />

measure their energies. Protons<br />

and light atomic nuclei are detected<br />

in various charged particle<br />

detectors, including the<br />

high-resolution silicon strip detector<br />

array HiRA. Neutrons are<br />

studied with the<br />

neutron emission<br />

ratio observer NERO and<br />

the modular neutron array<br />

MoNA. Gamma-rays<br />

are detected in the segmented<br />

germanium array SeGA. The rare isotopes<br />

can also be stopped and their properties<br />

studied with the low energy beam ion trap<br />

LEBIT or the beta counting system BCS.<br />

<strong>NSCL</strong> has complete electronics and mechanical<br />

engineering departments and a modern<br />

machine shop equipped with a variety of<br />

CNC machines capable of building complex<br />

parts for experimental equipment.<br />

If you need something for your research project,<br />

the purchasing department at <strong>NSCL</strong> is<br />

there to help. Purchasing approval, placement<br />

of an order, and receiving are all handled<br />

in-house – saving a lot of time.<br />

<strong>Graduate</strong> students will work on personal desktop<br />

computers and have access to the <strong>NSCL</strong><br />

linux clusters, as well as to MSU’s high performance<br />

computing center. <strong>Student</strong>s also benefit<br />

from strong<br />

<strong>National</strong> and<br />

International<br />

Collaborations,<br />

for example<br />

the<br />

Joint Institute<br />

for Nuclear<br />

Astrophysics<br />

(JINA), the<br />

Mesoscopic<br />

Theory Center (MTC), and the Exotic Femto<br />

Systems Overseas Laboratory of the University<br />

of Tokyo are located at <strong>NSCL</strong>. In addition,<br />

<strong>NSCL</strong> theorists are members of the Universal<br />

Nuclear Energy Density Functional (UNEDF)<br />

SciDAC project, and the Center of Excellence<br />

for Radioactive Ion Beam Studies for Stewardship<br />

Science.<br />

06<br />

www.nscl.msu.edu


<strong>NSCL</strong><br />

Lab History & Future Plans<br />

Nuclear physics research began at Michigan<br />

State University in 1958. In the decades that<br />

followed, MSU became known, both in the<br />

United States and worldwide, for its innovations<br />

in nuclear science and associated crossdisciplinary<br />

research. Major contributions<br />

have been made in the fields of nuclear structure,<br />

nuclear astrophysics, heavy-ion reaction<br />

mechanisms, accelerator physics, beam dynamics<br />

and experimental techniques.<br />

<strong>NSCL</strong> also is the source of innovations that improve<br />

lives. A medical cyclotron built by the<br />

laboratory in the 1980s was used to treat cancer<br />

patients at Harper University Hospital in<br />

Detroit for more than 15 years. More recently,<br />

<strong>NSCL</strong> technology and design concepts were<br />

used in a new, higher-powered medical cyclotron<br />

built by Varian Medical Systems. The<br />

collaboration agreement, an example of<br />

technology transfer that returns benefits to<br />

the university, will bring<br />

more advanced nuclear<br />

therapy to cancer<br />

patients in several<br />

countries.<br />

Over the years, <strong>NSCL</strong><br />

has evolved into the<br />

largest campus-based<br />

nuclear science facility<br />

in the country. Today,<br />

the laboratory<br />

has 300 employees, including 28 faculty and<br />

about 100 students, half of them in doctoral<br />

programs. MSU awards approximately 10 percent<br />

of the nation’s nuclear science doctorates<br />

and, according to U.S. News & World Report,<br />

is ranked second to MIT in nuclear physics<br />

graduate education. The laboratory also offers<br />

several programs designed to give undergraduates<br />

meaningful, hand-on research<br />

experiences. Several dozen undergrads participate<br />

in such programs annually.<br />

In December 2006, <strong>NSCL</strong> released plans for the<br />

Isotope Science Facility, a capability upgrade<br />

that would provide the nuclear science re-<br />

search community<br />

with<br />

significantly<br />

i n c r e a s e d<br />

i n t e n s i t i e s<br />

and varieties<br />

of worldclass<br />

beams<br />

of rare isotopes<br />

well into the 21 st century. Top administrators<br />

from the laboratory and university are<br />

continuing to work with the science community,<br />

lawmakers and senior officials at federal<br />

agencies to make the case for the laboratory<br />

upgrade — a logical continuation of decades<br />

of research and education accomplishments<br />

by <strong>NSCL</strong> faculty, students and users.<br />

Meanwhile, in ongoing day-to-day operations,<br />

<strong>NSCL</strong> is laying the groundwork for a future in<br />

which it serves the anticipated requirements<br />

of the U.S. rare isotope research community;<br />

extends the frontiers of nuclear science;<br />

and enhances the nation’s<br />

workforce as it trains the next generation<br />

of science and<br />

technology professionals.<br />

www.nscl.msu.edu<br />

07


<strong>NSCL</strong><br />

Careers in Nuclear Science<br />

Your success as a graduate student is important<br />

to us. Our graduates are in high demand,<br />

and they are the best testimony to the quality<br />

of our highly ranked graduate education<br />

program.<br />

As a nuclear or accelerator physicist, engineer,<br />

or nuclear chemist educated at <strong>NSCL</strong>,<br />

you are well positioned to pursue a variety<br />

of career paths. You are expertly trained to<br />

do research in a university,<br />

at a national<br />

laboratory, or in an<br />

industrial setting. You<br />

are well qualified to<br />

teach in a small college<br />

or a large university.<br />

You can pursue<br />

science policy or<br />

specialize in business.<br />

You can work for the<br />

U.S. Patent Office or<br />

on Wall Street or at<br />

Mayo Clinic. If you are not sure which direction<br />

to take, we have a large network of <strong>NSCL</strong><br />

alumni who will gladly speak with you about<br />

their professions.<br />

<strong>NSCL</strong> graduates now occupy many important<br />

positions in universities, national laboratories,<br />

and the private sector, making<br />

valuable contributions to society<br />

in many different areas. For example,<br />

recent <strong>NSCL</strong><br />

graduates now work on<br />

cancer therapy, airport<br />

Career Placement<br />

of <strong>NSCL</strong> Ph.D.s<br />

1996-2007<br />

anti-terrorist safety, environmental protection,<br />

weapons safeguards, national security, nuclear<br />

fusion, and radiation safety of space travel.<br />

Others have chosen careers where they apply<br />

their problem solving and goal-oriented<br />

team-work skills in diverse areas of the economy,<br />

including car manufacturing, electronics,<br />

computing, and finance.<br />

The Statistical Research Center of the American<br />

Institute of Physics disseminates data on<br />

education and employment in physics and<br />

related fields. For example, the center publishes<br />

reports on common career paths, workforce<br />

dynamics, and salaries and employment<br />

prospects. The reports and additional<br />

statistical data can be found at:<br />

http://www.aip.org/statistics/<br />

08<br />

www.nscl.msu.edu


<strong>NSCL</strong><br />

Admissions<br />

<strong>NSCL</strong> is committed to<br />

providing the highest<br />

quality graduate education<br />

in nuclear science,<br />

nuclear astrophysics,<br />

accelerator physics,<br />

and related instrumentation<br />

technologies. The<br />

degree requirements<br />

and curricula differ, depending<br />

on whether you<br />

matriculate in the Department<br />

of Chemistry,<br />

Department of Physics & Astronomy, or the<br />

College of Engineering. We refer you to the<br />

corresponding departments for application<br />

procedures and admission, course and degree<br />

requirements.<br />

Based on your background, the <strong>Graduate</strong><br />

Advisors in each department will put together<br />

an individual curriculum for you. <strong>Student</strong>s accepted<br />

into the graduate program at <strong>NSCL</strong><br />

receive teaching or research assistantships.<br />

At <strong>NSCL</strong>, your first contact<br />

point is the Associate<br />

Director for Education<br />

who will discuss<br />

with you the various<br />

options and opportunities<br />

for research topics.<br />

He will continue to<br />

serve as contact between<br />

you, <strong>NSCL</strong> and<br />

your respective department<br />

for the duration<br />

of your thesis studies.<br />

member. <strong>NSCL</strong> faculty<br />

can serve as the direct<br />

thesis supervisor as they<br />

have either joint or adjunct<br />

appointments<br />

at one of the departments.<br />

The research<br />

environment at <strong>NSCL</strong><br />

is very collaborative<br />

and the connection<br />

between individual research<br />

groups is very<br />

strong. For example,<br />

within a collaboration a professor in the Department<br />

of Physics & Astronomy can supervise<br />

a chemistry student and vice versa.<br />

After you choose your area of research you<br />

will form your guidance committee which will<br />

meet with you at least once a year to ensure<br />

a satisfactory progress towards your degree.<br />

All <strong>NSCL</strong> graduate students actively participate<br />

in Research Discussion, Nuclear Seminars,<br />

Departmental Colloquia, and the daily<br />

laboratory business. Essential to a doctoral<br />

degree is that you develop and then demonstrate<br />

the ability to conduct vital, independent<br />

research. To become an independent<br />

researcher you will need to develop a set of<br />

proficiencies. After you advance<br />

to Ph.D. candidacy it usually takes<br />

two to four years to complete the<br />

original research that<br />

forms the basis for your<br />

dissertation.<br />

<strong>Graduate</strong> students at <strong>NSCL</strong> will perform their<br />

research under the guidance of a faculty<br />

www.nscl.msu.edu<br />

09


<strong>NSCL</strong><br />

Faculty<br />

Wolfgang Bauer<br />

Theoretical Nuclear Physics<br />

Abigail Bickley<br />

Nuclear Chemistry<br />

Scott Bogner<br />

Theoretical Nuclear Physics<br />

Georg Bollen<br />

Experimental Nuclear Physics<br />

Alex Brown<br />

Theoretical Nuclear Physics<br />

Edward Brown<br />

Theoretical Nuclear Astrophysics<br />

Pawel Danielewicz<br />

Theoretical Nuclear Physics<br />

Marc Doleans<br />

Accelerator Physics & Engineering<br />

Alexandra Gade<br />

Experimental Nuclear Physics<br />

Thomas Glasmacher<br />

Experimental Nuclear Physics<br />

Bill Lynch<br />

Experimental Nuclear Physics<br />

Paul Mantica<br />

Nuclear Chemistry<br />

Felix Marti<br />

Accelerator Physics & Engineering<br />

Wolfgang Mittig<br />

Experimental Nuclear Physics<br />

Dave Morrissey<br />

Nuclear Chemistry<br />

Filomena Nunes<br />

Theoretical Nuclear Physics<br />

Hendrik Schatz<br />

Experimental Nuclear Astrophysics<br />

Brad Sherrill<br />

Experimental Nuclear Physics<br />

Krzysztof Starosta<br />

Experimental Nuclear Physics<br />

Andreas Stolz<br />

Experimental Nuclear Physics<br />

Michael Thoennessen<br />

Experimental Nuclear Physics<br />

Betty Tsang<br />

Experimental Nuclear Physics<br />

John Vincent<br />

Accelerator Physics & Engineering<br />

Thomas Wangler<br />

Accelerator Physics & Engineering<br />

Gary Westfall<br />

Experimental Nuclear Physics<br />

Richard York<br />

Accelerator Physics & Engineering<br />

Remco Zegers<br />

Experimental Nuclear Physics<br />

Vladimir Zelevinsky<br />

Theoretical Nuclear Physics<br />

10<br />

www.nscl.msu.edu


Wolfgang Bauer<br />

University Distinguished Professor and<br />

Chairperson, Department of Physics and Astronomy<br />

Theoretical Nuclear Physics<br />

Selected Publications<br />

M.S., Physics,<br />

University Giessen,<br />

1985<br />

PhD, Physics,<br />

University Giessen,<br />

1987<br />

Joined <strong>NSCL</strong><br />

in October 1988<br />

bauer@pa.msu.edu<br />

Zipf’s Law in Nuclear Multifragmentation<br />

and Percolation Theory, K. Paech, W. Bauer,<br />

and S. Pratt, Phys. Rev. C 76, 054603 (2007)<br />

The Nuclear and Many-Body Physics of Supernova<br />

Explosions, T. Strother and W. Bauer,<br />

Int. J. Mod. Phys. E 16, 1073 (2007)<br />

Fragmentation and the Nuclear Equation<br />

of State, W. Bauer, Nucl. Phys. A787, 595c<br />

(2007)<br />

Cancer Detection on a Cell-by-Cell Basis Using<br />

a Fractal Dimension Analysis, W. Bauer<br />

and Ch.D. Mackenzie, Heavy Ion Physics 14,<br />

39 (2001)<br />

Common Aspects of Phase Transitions of<br />

Molecules, Nuclei, and Hadronic Matter, W.<br />

Bauer, Nucl. Phys. A681, 441 (2001)<br />

I am a theoretical physicist and work mainly on phase<br />

transitions in nuclear systems, on transport theory for<br />

heavy ion collisions, and on the determination of the<br />

nuclear equation of state. Much of my work is in close<br />

connection with experimentally accessible observables,<br />

and I have enjoyed many collaborations with<br />

my experimental colleagues from <strong>NSCL</strong> and around<br />

the world. Approximately one half of my roughly 120<br />

publications in peer-reviewed journals are collaborations<br />

with experimentalists.<br />

During the last few years I have found out that many<br />

advances in one particular field of science can be<br />

applied in an interdisciplinary way. One<br />

example is my application of algorithms<br />

developed in my work on nuclear fragmentation<br />

to the detection of cancer<br />

cells in human bodies. Another example<br />

is the application of our methods to solve<br />

the transport problem for heavy ion collisions<br />

to the dynamics of supernova explosions.<br />

This project is still ongoing and first<br />

results look very promising.<br />

I have also worked on chaos, non-linear<br />

dynamics, and self-organized criticality.<br />

All of these areas of study have applications<br />

to nuclear physics, but also to a great<br />

range of other systems, from molecules to<br />

traffic flow, and from the stock market to<br />

the weather.<br />

Finally, I am interested in research on teaching and<br />

learning. Here I have a long-standing collaboration<br />

that has produced the LON-CAPA course management<br />

and learning system, which is now in use at over<br />

<strong>NSCL</strong><br />

100 universities, colleges, and high schools around<br />

the country and in several other countries around the<br />

world.<br />

For the near future I am planning on a continuation of<br />

the work on nuclear fragmentation, as well as the transport<br />

problem for supernova explosions. In addition, I<br />

have become interested in the physics of double β decay<br />

and the hunt for a neutrino-less double-β decay<br />

mode, which would overthrow the standard model of<br />

particle physics. I am also continuing my practice of<br />

tight collaborations with my experimental colleagues<br />

at <strong>NSCL</strong>, by working on the physics case for a time projection<br />

chamber experiment for the next upgrade of<br />

the accelerator complex at <strong>NSCL</strong>.<br />

Using transport theories and models of phase transitions<br />

to determine the nuclear matter phase diagram.<br />

www.nscl.msu.edu<br />

11


d Rapidiare<br />

et al.,<br />

32002.<br />

mentum,<br />

N) = 200<br />

Rev. Lett.<br />

y for the<br />

3, 285.<br />

r Midra-<br />

GeV, B.B.<br />

CHEMISTRY RESEARCH FACULTY<br />

ransverse<br />

sqrt(s_<br />

Rev. Lett.<br />

le to Parlisions<br />

at<br />

Rev. C70<br />

propperatween<br />

nd the<br />

tate of<br />

ces red<br />

neuict<br />

the<br />

ental<br />

nergy.<br />

16<br />

Abigail A. Bickley<br />

ASSISTANT<br />

PROFESSOR<br />

(b. 1978)<br />

B.A., 2000,<br />

Dartmouth College;<br />

Ph.D., 2004, University of<br />

Maryland, College Park;<br />

Research Associate,<br />

University of Colorado<br />

at Boulder, 2004-07.<br />

517-355-9672<br />

Ext. 480<br />

Nuclear Equation of State<br />

SELECTED PUBLICATIONS<br />

J/Psi Production vs. Transverse Momentum and Rapidity<br />

in p+p Collisions at sqrt(s) = 200 GeV, A. Adare et al.,<br />

” hep-ex/0611020, Phys. Rev. Lett. 2007, 98, 232002.<br />

J/Psi Production vs. Centrality, Transverse Momentum,<br />

and Rapidity in Au+Au Collisions at sqrt(s_NN) = 200<br />

GeV, A. Adare, et al., nucl-ex/0611020, Phys. Rev. Lett.<br />

2007, 98, 232201.<br />

Quarkonium Production in PHENIX, A. Bickley for the<br />

PHENIX Collaboration, Nucl. Phys. 2007, A783, 285.<br />

Charged Antiparticle to Particle Ratios Near Midrapidity<br />

in p+p Collisions at sqrt(s_NN) = 200 GeV, B.B.<br />

Back, et al., Phys. Rev. C71 2005, 021901(R).<br />

Centrality Dependence of Charged Hadron Transverse<br />

Momentum Spectra in Au+Au Collisions from sqrt(s_<br />

Selected Publications<br />

J/Psi Production vs. Transverse Momentum<br />

and Rapidity in p+p Collisions at √(s)<br />

= 200 GeV, A. Adare et al., Phys. Rev.<br />

Lett. 98, 232002 (2007)<br />

J/Psi Production vs. Centrality, Transverse<br />

Momentum, and Rapidity in Au+Au Collisions<br />

at √(sNN) = 200 GeV, A. Adare et<br />

al., Phys. Rev. Lett. 98, 232201 (2007)<br />

Quarkonium Production in PHENIX, A.<br />

Bickley for the PHENIX Collaboration,<br />

Nucl. Phys. A783, 285 (2007)<br />

Charged Antiparticle to Particle Ratios<br />

Near Midrapidity in p+p Collisions at<br />

√(sNN) = 200 GeV, B.B. Back et al., Phys.<br />

Rev. C 71 021901(R) (2005)<br />

Centrality Dependence of Charged<br />

Hadron Transverse Momentum Spectra<br />

in Au+Au Collisions from √(sNN) = 62.4 to<br />

200 GeV, B.B. Back et al., Phys. Rev. Lett.<br />

94, 082304 (2005)<br />

Abigail Bickley<br />

Assistant Professor<br />

Nuclear Chemistry<br />

Nuclear Equation of State<br />

B.A., Chemistry,<br />

Dartmouth College,<br />

2000<br />

PhD, Nuclear Chemistry,<br />

University of Maryland,<br />

2004<br />

Joined <strong>NSCL</strong><br />

in May 2007<br />

bickley@nscl.msu.edu<br />

In the laboratory setting,<br />

My research interests revolve NN) = 62.4<br />

collisions<br />

around to 200 GeV,<br />

of<br />

B.B.<br />

heavy<br />

studying Back et al.,<br />

nuclei<br />

the Phys. prop- Rev.<br />

allow<br />

Lett. try energy. In the laboratory setting, collisions of heavy<br />

the density of the system 2005, to be 94, 082304. controlled and provide a window<br />

through<br />

erties of nuclear<br />

which<br />

matter<br />

we can<br />

over<br />

observe<br />

a wide<br />

the<br />

range<br />

properties<br />

of temperaof<br />

the nucleus.<br />

and The energy particles densities. produced<br />

nuclei allow the density of the system to be controlled<br />

Centrality Dependence of Charged Antiparticle to Particle<br />

Ratios<br />

tures in The the<br />

Near relationship collision<br />

Mid-Rapidity<br />

of asymmetric<br />

in between d+Au Collisions the nuclei<br />

provide constraints our understanding of the symmetry the properties of the nucleus. The particles produced<br />

at and provide a window through which we can observe<br />

environmental conditions<br />

sqrt(s_NN)<br />

a nucleus<br />

= 200 GeV,<br />

is<br />

B.B.<br />

subjected<br />

Back et al., Phys.<br />

to<br />

Rev.<br />

and<br />

C70<br />

2004, 011901(R).<br />

the properties it exhibits is governed energy by term the of equation the nuclear of in the collision of asymmetric nuclei provide constraints<br />

state of nuclear matter. The equation of of state. This not serves only on our understanding of the symmetry energy term of<br />

characterizes the properties of to nuclear further our matter, understanding but also the nuclear equation of state. This serves to further our<br />

provides a mathematical relationship of the properties between of the neutronrich<br />

characterize nuclei, which nuclei. dominate which dominate the chart of the known nuclides.<br />

thermodynamic<br />

variables used to<br />

understanding of the properties of neutron-rich nuclei,<br />

the chart of the known nuclides.<br />

My<br />

This relationship<br />

research<br />

governs<br />

interests revolve<br />

the physical<br />

around Collisions studying<br />

characteristics<br />

of heavy the properties<br />

of nuclear matter over are performed a wide range and of observed tempera-<br />

the density of the system to be controlled and provide a win-<br />

ions<br />

Collisions<br />

In the<br />

of<br />

laboratory<br />

heavy ions<br />

setting,<br />

are<br />

collisions<br />

performed<br />

of heavy<br />

and<br />

nuclei<br />

observed<br />

allow<br />

at<br />

and behavior<br />

tures and<br />

of nuclear<br />

energy densities.<br />

matter as it existed in the early<br />

at the The relationship <strong>National</strong> <strong>Superconducting</strong><br />

terrestrial is Cyclotron subjected nuclear Laborato-<br />

and mat-<br />

the cleus. opportunity The particles for studying produced the in the symmetry collision of energy asymmetric through nu-<br />

between dow<br />

<strong>NSCL</strong>.<br />

through<br />

The facilities<br />

which we<br />

available<br />

can observe<br />

at<br />

the<br />

<strong>NSCL</strong><br />

properties<br />

provide<br />

of<br />

a<br />

the<br />

unique<br />

nu-<br />

universe, the environmental in neutron conditions stars, and a nucleus<br />

ter. properties Within it a exhibits nucleus, is governed the ry by (<strong>NSCL</strong>), the equation which is of adjacent state of clei provide constraints on our understanding the collision of the symmetry of isospin<br />

energy nuclear per matter. nucleon The equation receives<br />

of state contributions not only characterizes from ment. The facilities available<br />

equation due to of state. the wide This serves variety<br />

to the Chemistry Depart-<br />

energy asymmetric term of the heavy nuclear ions<br />

the the energy properties of of symmetric nuclear matter,<br />

but matter also provides and a a cor-<br />

math-<br />

opportunity for studying the<br />

of the targets properties available. of neutron-<br />

These<br />

at the <strong>NSCL</strong> provide a unique<br />

to further of primary our understanding beams and<br />

nuclear<br />

rection ematical term relationship related to between the symmetry energy through<br />

rich capabilities nuclei, which allow dominate constraints<br />

to be made to<br />

neutron-proton<br />

the thermodynamic<br />

asymmetry<br />

known as the symme-<br />

variables the collision of isospin asymmetric<br />

heavy ions due to the<br />

clides. Collisions of heavy ions<br />

the chart of the known nu-<br />

used to characterize nuclei. This<br />

relationship governs the physical<br />

characteristics targets available. and These behavior capabilities allow constraints to be<br />

at of the state <strong>National</strong> that are Supercon-<br />

vital to<br />

wide variety of primary beams<br />

are<br />

the<br />

performed<br />

nuclear<br />

and observed<br />

equation<br />

try energy. The asymmetry<br />

and<br />

correction<br />

made of nuclear to the matter nuclear<br />

accounts as equation it existed for<br />

of state that are vital to the advancement<br />

in the differences early of universe, understanding resulting<br />

neutron of astrophysical processes related<br />

ry (<strong>NSCL</strong>), understanding which is adjacent of astroducting<br />

the Cyclotron advancement Laborato-of<br />

isospin<br />

from to stars, neutron and inequality stars terrestrial and supernova in nuclear the explosions and to the understanding<br />

matter. of Within of nuclear protons a nucleus, structure and the away from the valley of stability.<br />

ment. ed The to neutron facilities available stars and<br />

to physical the Chemistry processes Depart-<br />

relat-<br />

numbers<br />

neutrons energy per in the nucleon nucleus. receives<br />

at the supernova <strong>NSCL</strong> provide explosions a unique<br />

contributions from the energy<br />

opportunity and to the for studying understanding<br />

of nuclear<br />

the<br />

In of order symmetric to understand<br />

nuclear matter<br />

symmetry energy through<br />

structure<br />

and a correction term related to<br />

the collision of isospin asymmetric<br />

heavy ions due to the<br />

and predict the behavior<br />

away from the valley of<br />

the neutron-proton asymmetry<br />

of<br />

known<br />

nuclear<br />

as the<br />

matter<br />

symmetry<br />

exposed<br />

energy.<br />

wide stability. variety of primary beams<br />

to The different asymmetry environmental Chart of the known nuclides plotted as a function of the number of<br />

correction accounts neutrons for isospin versus the differences number of resulting<br />

from it an is inequality important in the numbers resent the of stability protons of each and neu-<br />

nucleus made and are to the described nuclear in equation the key. of state that are vital to the ad-<br />

protons and in targets the nucleus. available. The These colors capabilities rep-<br />

allow constraints to be<br />

conditions,<br />

to trons constrain the nucleus. the symme- In order to understand and predict the vancement of understanding of astrophysical processes related<br />

behavior of nuclear matter exposed to different environmental to neutron stars and supernova explosions and to the understanding<br />

of nuclear structure away from the valley of conditions, it is important to constrain the symmetry energy.<br />

stability.<br />

12 bickley@chemistry.msu.edu<br />

www.nscl.msu.edu<br />

<strong>NSCL</strong>


Scott Bogner<br />

Assistant Professor<br />

Theoretical Nuclear Physics<br />

B.S., Nuclear Engineering,<br />

University of Cincinnati,<br />

1996<br />

PhD, Theoretical Physics,<br />

SUNY Stony Brook,<br />

2002<br />

Joined <strong>NSCL</strong><br />

in July 2007<br />

bogner@nscl.msu.edu<br />

Selected Publications<br />

Convergence in the no-core shell model<br />

with low-momentum two-nucleon interactions.<br />

S.K. Bogner, R.J. Furnstahl, P. Maris,<br />

R.J. Perry and J.P. Vary, to appear in Nucl.<br />

Phys. A<br />

Are low-energy nuclear observables sensitive<br />

to high-energy phase shifts? S.K. Bogner,<br />

R.J. Furnstahl, R.J. Perry and A. Schwenk,<br />

Phys. Lett. B 649, 488 (2007)<br />

Similarity renormalization group for nucleon-nucleon<br />

interactions. S.K. Bogner, R.J.<br />

Furnstahl and R.J. Perry, Phys. Rev. C 75,<br />

061001(R) (2007)<br />

Is nuclear matter perturbative with lowmomentum<br />

interactions? S.K. Bogner, A.<br />

Schwenk, R. J. Furnstahl and A. Nogga,<br />

Nucl. Phys. A763, 59 (2005)<br />

Model-independent low momentum nucleon<br />

interaction from phase shift equivalence,<br />

S.K. Bogner, T.T.S. Kuo and A. Schwenk,<br />

Phys. Rep. 386, 1 (2003)<br />

My research focuses on applications of the renormalization<br />

group (RG) and effective field theories (EFT) to<br />

the microscopic description of nuclei and nuclear matter.<br />

The ultimate goal is to develop theoretical methods<br />

that generate model-independent predictions with reliable<br />

theoretical error estimates. Such capabilities will<br />

be necessary to confront fundamental problems of<br />

low-energy nuclear physics, such as the physics of nuclei<br />

far from stability, where controlled extrapolations to<br />

extreme N/Z ratios are essential but have been lacking<br />

in theoretical approaches to date. The development<br />

of such methods will be essential to provide reliable nuclear<br />

physics input for astrophysical applications and<br />

to provide meaningful theoretical support to existing<br />

and next-generation rare isotope beam facilities such<br />

as those at <strong>NSCL</strong>.<br />

EFT and RG methods have long enjoyed a prominent<br />

role in condensed matter and high energy theory due<br />

to their power of simplification and universality. More<br />

recently, these complementary techniques have<br />

launched a paradigm shift in theoretical low-energy<br />

Ground-State Energy [MeV]<br />

−5<br />

−10<br />

−15<br />

−20<br />

−25<br />

−30<br />

−10<br />

−15<br />

−20<br />

−25<br />

λ = 3.0 fm −1<br />

N<br />

3 LO (500 MeV)<br />

−30<br />

20 25 30 35 40<br />

h∨ [MeV]<br />

<strong>NSCL</strong><br />

λ = 1.5 fm −1<br />

λ = 2.0 fm −1<br />

4<br />

He<br />

N max = 2<br />

N max = 4<br />

N max = 6<br />

N max = 8<br />

N max = 10<br />

N max = 12<br />

10 15 20 25 30<br />

h∨ [MeV]<br />

Figure illustrating<br />

the accelerated<br />

convergence<br />

using<br />

RG-improved<br />

interactions in<br />

no-core shell<br />

model (NCSM)<br />

calculations of<br />

4 He.<br />

nuclear physics, enabling for the first time the prospect<br />

for model-independent and microscopic calculations<br />

of nuclear structure with controllable theoretical errors,<br />

within a framework that is manifestly constrained by the<br />

symmetries of the underlying quantum chromodynamics<br />

(QCD). From a computational perspective, the use<br />

of EFT and RG techniques makes practical calculations<br />

more tractable by restricting the necessary degrees of<br />

freedom to the energy scales of interest.<br />

A consequence is that microscopic nuclear structure<br />

calculations become much more amenable to<br />

straightforward perturbative methods, simple (i.e., less<br />

correlated) variational ansätze, and rapidly convergent<br />

basis expansions. Since a mean field description<br />

(e.g., Hartree-Fock) now becomes a reasonable starting<br />

point for nuclei and nuclear matter, the large arsenal<br />

of techniques developed for non-uniform electronic<br />

systems (e.g., density functional methods) become<br />

available for nuclei. Density functional theory (DFT) is<br />

the ideal framework to describe properties of the medium-to-heavy<br />

regions of the nuclear mass table where<br />

ab-initio methods are computationally prohibitive. Developing<br />

a microscopically-based, universal nuclear<br />

energy density functional (UNEDF) derived from RGimproved<br />

EFT Hamiltonians is a major component of<br />

the 5 year, $15M SciDAC project Building a Universal<br />

Nuclear Energy Density Functional that I am a part of,<br />

along with my MSU colleague Alex Brown. My research<br />

program presents a diverse range of research opportunities<br />

for potential Ph.D. students, encompassing three<br />

very different (but interrelated) components that offer<br />

a balance of analytical and numerical work: 1) internucleon<br />

interactions, 2) ab-initio methods for finite nuclei<br />

and infinite nuclear matter, and 3) density functional<br />

theory for nuclei.<br />

www.nscl.msu.edu<br />

13


Georg Bollen<br />

Professor<br />

Experimental Nuclear Physics<br />

Selected Publications<br />

Precision mass measurements of rare isotopes<br />

near N=Z=33 produced by fast beam<br />

fragmentation, P. Schury et al., Phys. Rev. C<br />

75, 055801 (2007)<br />

Octupolar excitation of ion motion in a Penning<br />

trap - A study performed at LEBIT, R.<br />

Ringle, G. Bollen, P. Schury, S. Schwarz, and<br />

T. Sun, Int. J. Mass Spec. 262, 33 (2007)<br />

Experiments with Thermalized Rare Isotope<br />

Beams from Projectile Fragmentation - A<br />

Precision Mass Measurement of the Super-<br />

Allowed β-emitter 38 Ca, G. Bollen et al., Phys.<br />

Rev. Lett. 96, 152501 (2006)<br />

A study of gas-stopping of intense energetic<br />

rare isotope beams, G. Bollen, D.J. Morrissey,<br />

S. Schwarz, Nucl. Instr. Meth. A550, 27 (2005)<br />

Traps for Rare Isotopes. Georg Bollen, Lecture<br />

Notes in Physics 651, 169 (2004)<br />

M.S., Physics,<br />

Mainz University,<br />

1984<br />

PhD, Physics,<br />

Mainz University,<br />

1989<br />

Joined <strong>NSCL</strong><br />

in June 2000<br />

bollen@nscl.msu.edu<br />

My research interests are related to nuclear and atomic<br />

physics with focus on the study of basic properties of<br />

atomic nuclei very far away from the valley of stability.<br />

A major activity in my group is the determination of the<br />

mass of such rare isotopes, which is their most fundamental<br />

property. An accurate knowledge of atomic<br />

masses is important for revealing the inner structure of<br />

exotic nuclei and to provide crucial tests for nuclear<br />

model predictions. Atomic masses are one of the key<br />

information required for the description of the synthesis<br />

of the elements in the universe. Certain special nuclei<br />

are important for testing our understanding of symmetries<br />

and the fundamental forces in nature; their masses<br />

need to be determined with an accuracy of 10 parts<br />

per billion or better. Such high-precision mass measurements<br />

have become possible at <strong>NSCL</strong> with the Low Energy<br />

Beam and Ion Trap facility, or LEBIT. In LEBIT, the<br />

movement of the rare isotopes delivered by the Coupled<br />

Cyclotron Facility is slowed down from half the<br />

speed of light to the point at which they can be kept<br />

floating in a vacuum in a device called an ion trap.<br />

Here their mass can be determined with very high precision<br />

via the observation of their cyclotron motion in a<br />

strong 9.4 Tesla magnetic field. LEBIT, in operation since<br />

2005, has started its mass measurement program very<br />

successfully; rare isotopes with half-lives of less than 100<br />

ms have been captured and studied and mass accuracies<br />

below 10 -8 have been reached.<br />

In addition to determining their mass I am interested in<br />

atomic spectroscopy of rare isotopes using lasers. This,<br />

for example, can provide information on the size and<br />

shape of the atomic nucleus. My group is involved in<br />

the on-going realization of such a laser spectroscopy<br />

facility at <strong>NSCL</strong>.<br />

Another research area is the development of advanced<br />

manipulation techniques for rare isotope<br />

beams. Developments of that kind are critical for maximizing<br />

the performance of experiments and for creating<br />

new experimental opportunities for the study of rare<br />

isotopes. My group is working on techniques that allow<br />

fast rare isotope beams to be slowed down and converted<br />

into low-energy beams efficiently and fast, on<br />

beam-cooling and bunching techniques, and on the<br />

development of a device that increases the charge<br />

state of ions. Such a charge breeder is a key component<br />

of the re-accelerator project presently underway<br />

at <strong>NSCL</strong>, which will provide rare isotope beams that are<br />

world-unique and add a new and exciting component<br />

to the strong research program of <strong>NSCL</strong>.<br />

The LEBIT ion trap: shown are the gold-plated high-precision electrodes<br />

that provide the electric fields needed for capturing and storing<br />

rare isotope ions in the 9.4 T field of the LEBIT Penning trap mass<br />

spectrometer.<br />

14 www.nscl.msu.edu<br />

<strong>NSCL</strong>


Alex Brown<br />

Professor<br />

Theoretical Nuclear Physics<br />

B.A., Physics,<br />

Ohio State University,<br />

1970<br />

M.S., Physics,<br />

SUNY Stony Brook,<br />

1972<br />

PhD, Physics,<br />

SUNY Stony Brook,<br />

1974<br />

Joined <strong>NSCL</strong><br />

in January 1982<br />

brown@nscl.msu.edu<br />

Selected Publications<br />

New USD Hamiltonians for the sd Shell,<br />

B.A. Brown and W.A. Richter, Phys. Rev.<br />

C 74, 034315 (2006)<br />

Tensor Interaction Contributions to<br />

Single-Particle Energies, B.A. Brown, T.<br />

Duguet, T. Otsuka, D. Abe and T. Suzuki,<br />

Phys. Rev. C 74, 061303(R) (2006)<br />

Magic Numbers in Neutron-Rich Oxygen<br />

Isotopes, B.A. Brown and W.A. Richter,<br />

Phys. Rev. C 72, 057301 (2005)<br />

The Nuclear Shell Model Towards the<br />

Drip Lines, B.A. Brown, Prog. Part. Nucl.<br />

Phys. 47, 517 (2001)<br />

Neutron Radii in Nuclei and the Neutron<br />

Equation of State, B.A. Brown, Phys. Rev.<br />

Lett. 85, 5296 (2000)<br />

My research in theoretical nuclear physics is motivated<br />

by broad questions in science: What are the fundamental<br />

particles of matter? What are the fundamental<br />

forces and their symmetries that govern their interactions?<br />

How were the elements formed during the evolution<br />

of the Universe? How do the simplicities observed<br />

in many-body systems emerge from their underlying<br />

microscopic properties?<br />

The diverse activities<br />

within our nuclear theory<br />

group, coupled with<br />

the forefront experimental<br />

work in nuclear<br />

structure, nuclear reactions<br />

and nuclear astrophysics<br />

at <strong>NSCL</strong> provide<br />

the perfect environment<br />

for the development<br />

of new theoretical<br />

ideas. I also have<br />

collaborations with<br />

theoretical and experimental<br />

groups in many<br />

countries including Germany,<br />

France, England,<br />

Italy, Norway, Japan<br />

and South Africa.<br />

I pursue the development of new analytical and computational<br />

tools for the description of nuclear structure,<br />

especially for nuclei far from stability. The basic theoretical<br />

tools include the configuration-interaction and<br />

energy-density functional methods. I work with collaborators<br />

to developed software for desktop computing<br />

as well for high-performance computing.<br />

Specific topics of interest<br />

include: the structure of<br />

light nuclei, nuclei near<br />

the driplines, di-proton<br />

decay, proton and neutron<br />

densities, double β<br />

decay, tests of unitarity<br />

from Fermi β-decay,<br />

isospin non-conservation,<br />

anapole moments and<br />

parity non-conservation,<br />

neutrino-nucleus interactions,<br />

quantum chaos and<br />

the rapid-proton capture<br />

process in astrophysics.<br />

<strong>NSCL</strong><br />

www.nscl.msu.edu<br />

15


Selected Publications<br />

First Superburst from a Classical Low-mass<br />

X-ray Binary Transient. L. Keek et al., Astron.<br />

Astrophys., in press (2008)<br />

Phase Separation in the Crust of Accreting<br />

Neutron Stars, C.J. Horowitz, D.K. Berry, and<br />

E.F. Brown, Phys. Rev. E 75, 066101 (2007)<br />

Heating in the Accreted Neutron Star<br />

Ocean: Implications for Superburst Ignition,<br />

S.S. Gupta, et al., Astrophys. J. 662, 1188<br />

(2007)<br />

The Laminar Flame Speedup by Neon-22<br />

Enrichment in White Dwarf Supernovae,<br />

D.A. Chamulak, E. F. Brown, and F.X. Timmes.<br />

Astrophys. J. Lett. 655, L93 (2007)<br />

Sedimentation and Type I X-ray Bursts at Low<br />

Accretion Rates, F. Peng, E.F. Brown, and<br />

J.W. Truran, Astrophys. J. 654, 1022 (2007)<br />

Superburst Ignition and Implications for Neutron<br />

Star Interiors, E.F. Brown, Astrophys. J.<br />

Lett. 614, L57 (2004)<br />

Edward Brown<br />

Assistant Professor<br />

Theoretical Nuclear Astrophysics<br />

M.S., Physics,<br />

University of California,<br />

1996<br />

PhD, Physics,<br />

University of California,<br />

1999<br />

Joined <strong>NSCL</strong><br />

in August 2004<br />

browne@nscl.msu.edu<br />

High-energy and nuclear astrophysics are truly in a<br />

golden period. I conduct theoretical research in the<br />

exciting area of compact stars,neutron stars and white<br />

dwarfs. Neutron stars are the most dense objects in nature,<br />

and have long fascinated astronomers and physicists<br />

alike. With X-ray telescopes such as Chandra and<br />

XMM to study these objects, nuclear experiments such<br />

as heavy-ion collisions to study the nuclear force, and<br />

the promise of gravitational wave detectors such as<br />

LIGO, our knowledge of these enigmatic objects and<br />

the nature of dense matter is rapidly improving. Many<br />

neutron stars accrete gas from a binary, solar-like companion.<br />

As this gas accumulates on the surface of the<br />

neutron star, unstable nuclear reactions produce bursts<br />

of X-rays.<br />

a lattice in the neutron star crust. A surprise from these<br />

simulations is that the “ashes” of these bursts chemically<br />

separate as they are compressed to high densities.<br />

In an exciting new development, a superburst was<br />

detected from an intermittently, or transient, accreting<br />

neutron star. Because the crust cools when the neutron<br />

star star is not accreting, it was previously thought that<br />

superbursts could not occur in this system, because the<br />

temperature in the crust would be too cool for carbon-12<br />

fusion to occur.<br />

0.6 t = 0 d<br />

0.5<br />

t = 80 d<br />

New observations of these nuclear processes provide<br />

clues about the properties of superdense matter, but<br />

these observations also challenge our understanding<br />

of how the fuel is accreted and burned. Particularly<br />

exciting are the recently discovered “superbursts,” energetic<br />

explosions that are believed to be powered by<br />

unstable fusion of carbon-12. The “crust” of the neutron<br />

star, where the density is less than nuclear, must be sufficiently<br />

hot in order for the superburst to ignite. By studying<br />

these superbursts we can learn about the physics of<br />

the core, which cools by emitting neutrinos.<br />

Recently, I have collaborated on the first calculation<br />

of electron captures in the crust of an accreting neutron<br />

star using realistic nuclear physics input, and have<br />

investigated the “sinking” of heavy nuclei in the outer<br />

layers. These calculations quantified the heating of the<br />

neutron star from these reactions, and the results have<br />

been used in simulations of the “freezing” of ions into<br />

8 10 12 14 16 18<br />

lg y (g cm − 2 )<br />

16 www.nscl.msu.edu<br />

<strong>NSCL</strong><br />

T (GK)<br />

0.4<br />

0.3<br />

0.2<br />

surface<br />

Cutaway of an accreting neutron<br />

star, with a recent calculation of<br />

the temperature across the crust<br />

shown in the inset plot. The calculation<br />

was for a neutron star that<br />

accretes intermittently. Some 80 days after it started accreting, an<br />

energetic explosion was observed. The plot shows the temperature,<br />

as a function of depth in the crust, when accretion began (solid<br />

line) and at the time of the superburst (dotted line.) In order for the<br />

superburst to have ignited, the temperature in the crust as a function<br />

of depth should pass through the red rectangle. The fact that it<br />

doesn’t suggests that another source of heating must be present in<br />

the crust.<br />

core


Pawel Danielewicz<br />

Professor<br />

Theoretical Nuclear Physics<br />

Selected Publications<br />

M.S., Physics,<br />

Warsaw University,<br />

1977<br />

PhD, Physics,<br />

Warsaw University,<br />

1981<br />

Joined <strong>NSCL</strong><br />

in September 1988<br />

danielewicz@nscl.msu.edu<br />

Has the QCD Critical Point been Signaled<br />

by Observations at RHIC? R.A.<br />

Lacey, N.N. Ajitanand, J.M. Alexander,<br />

P. Chung, W.G. Holzmann, M. Issah, A.<br />

Taranenko, P. Danielewicz and H. Stocker,<br />

Phys. Rev. Lett. 98, 092301 (2007)<br />

Analyzing Correlation Functions with<br />

Tesseral and Cartesian Spherical Harmonics,<br />

P. Danielewicz and S. Pratt,<br />

Phys. Rev. C 75, 034907 (2007)<br />

Nuclear Isospin Diffusivity, L. Shi and P.<br />

Danielewicz, Phys. Rev. C 68, 064604<br />

(2003)<br />

Surface Symmetry Energy, P. Danielewicz,<br />

Nucl. Phys. A727, 233 (2003)<br />

Determination of the Equation of State<br />

of Dense Matter, P. Danielewicz, R. Lacey<br />

and W.G. Lynch, Science 298, 1592<br />

(2002)<br />

My research is in the area of nuclear theory with emphasis<br />

on central energetic reactions of heavy nuclei.<br />

In central reactions, unique conditions are created<br />

where nuclear matter may be compressed to densities<br />

much larger than those typical for nuclei and may be<br />

heated gaining thermal energy far in excess of the nuclear<br />

binding energy. The pressures achieved in those<br />

reactions are the highest produced by man. The compression<br />

of matter during a reaction is followed by a<br />

decompression that throws reaction products into different<br />

directions.<br />

From the features of products emitted from a central<br />

reaction, the conditions reached during the reaction<br />

may be deduced as well as properties of matter that<br />

gets compressed. However, conclusions require a careful<br />

modeling of the reaction dynamics from the side of<br />

theory. The modeling is typically done within transport<br />

Overview of the dynamics for a Au+Au collision in the system center<br />

of mass. Time increases from left to right.<br />

<strong>NSCL</strong><br />

theory, and sample calculations are illustrated in the<br />

figure. In the course of reaction modeling, the theory,<br />

on one hand, seeks explanations for the results of measurements.<br />

On the other hand, it produces suggestions<br />

for what to measure next in order to verify the conclusions<br />

or in order to gain novel information on the nuclear<br />

medium.<br />

Multiparticle final states of the reactions in measurements<br />

potentially contain enormous amount of information.<br />

E.g. for a state with 20 particles, each collision<br />

event yields 3x20=60 independent numbers just in terms<br />

of particle momentum components. Development of<br />

strategies for reducing the abundance of information<br />

to an information that can be absorbed by a human<br />

and is simultaneously useful, has called for the involvement<br />

of theory. With my personal participation, it became<br />

apparent how to relate the geometry of emission<br />

of products to the spatial geometry of a reaction<br />

characterized by the scale of 2•10 -15 m. Techniques<br />

have been developed to create, on a statistical basis,<br />

detailed images of final stages of the reactions with<br />

multiparticle final states.<br />

Properties of matter of nuclear reactions naturally link<br />

with the properties of matter in finite nuclei. Following<br />

that link, I have ventured into aspects of nuclear<br />

structure, particularly with regard to the imbalance between<br />

the neutron and proton numbers in nuclei. Transport<br />

that is close to or fully within the quantum domain<br />

has elements that are common for different areas. The<br />

theory of nonequilibrium Green’s functions, which I<br />

pursue, links the developments made in the context of<br />

nuclear reactions with those in electrical engineering<br />

and in early cosmology.<br />

www.nscl.msu.edu<br />

17


My research interest focuses on new developments for<br />

particle accelerators at <strong>NSCL</strong>, particularly design of<br />

accelerating lattices, study of systems with linear and<br />

non-linear beam dynamics properties, development<br />

of emittance cooling techniques, and beam measurements<br />

and lattice tuning methods.<br />

The Coupled Cyclotron Facility (CCF) is one of the most<br />

powerful rare isotope production facilities in the world.<br />

At the CCF, stable isotopes beams are accelerated up<br />

to 200 MeV/nucleon of kinetic energies and sent on a<br />

production target to produce rare isotope beams that<br />

are studied in nuclear physics experiments. Over the<br />

last years, the intensity of primary beams on the production<br />

target has been steadily increased and the<br />

facility operated at a high degree of reliability to meet<br />

the constant needs of the nuclear physics research program.<br />

To continue increasing the facility performance,<br />

improving the beam quality and reducing the time for<br />

primary beam tuning are crucial and a core part of the<br />

research program in the accelerator group pertaining<br />

to the CCF. Being successful in cooling the beam (i.e.<br />

improving its quality) prior to its injection into the cyclotrons<br />

would be a significant step forward to further<br />

increase the beam power on the production target. At<br />

the same time, reducing the beam tuning time by developing<br />

automatic tuning capabilities would increase<br />

the beam time for the nuclear physics experiments and<br />

thus increase the scientific output of the laboratory.<br />

These topics, among others, are necessary to keep the<br />

CCF among the leading rare isotope research facilities<br />

in the world.<br />

Selected Publications<br />

Experimental evidences for emittance degradation<br />

by space charge effect when using<br />

a focusing solenoid below an electron<br />

cyclotron resonance ion source, G. Machicoane<br />

et al., Rev. Sci. Instrum. 79, in press<br />

(2008)<br />

Design, Construction and First Commissioning<br />

Results of SuSI <strong>Superconducting</strong> Source<br />

for Ions at <strong>NSCL</strong>/MSU, P.A. Závodszky et al.,<br />

Rev. Sci. Instrum. 79, in press (2008)<br />

Optics improvements of the K500 axial injection<br />

line, M. Doleans et al. Proc. 18 th Int.<br />

Conf. Cyclotrons and their Applications<br />

2007, in press (2008)<br />

Status Report on the <strong>NSCL</strong> RF Fragment Separator,<br />

M. Doleans et al., Proc. Part. Accel.<br />

Conf. PAC07, 3585 (2007)<br />

Beam Dynamics Studies for the Reacceleration<br />

of Low Energy RIBS at the <strong>NSCL</strong>, X. Wu<br />

et al., Proc. Part. Accel. Conf. PAC07, 1769<br />

(2007)<br />

Marc Doleans<br />

Assistant Professor<br />

Accelerator Physics & Engineering<br />

B.S., Physics,<br />

Paris 7 University,<br />

1997<br />

M.S., Physics,<br />

Paris 7 University,<br />

1999<br />

PhD, Physics,<br />

Paris 7 University,<br />

2003<br />

Joined <strong>NSCL</strong><br />

in October 2003<br />

doleans@nscl.msu.edu<br />

<strong>NSCL</strong> is currently building a new accelerator (linac).<br />

This machine will be the first of its kind to reaccelerate<br />

rare isotope beams up to a three MeV/nucleon<br />

of kinetic energies after they have been cooled and<br />

brought near to rest in a gas stopping system upstream.<br />

The linac will mainly use a room temperature radio-frequency<br />

(rf) quadrupole and superconducting resonators<br />

to re-accelerate the beams. Such a machine is a<br />

new challenge for <strong>NSCL</strong> which has a strong expertise<br />

in superconducting cyclotron accelerators but much<br />

less in superconducting linear accelerators. A strong<br />

research program in superconducting rf technology in<br />

the last few years has helped to acquire the capability<br />

to build such a linac at <strong>NSCL</strong> but many challenges lay<br />

ahead for building, commissioning and operating the<br />

newest of <strong>NSCL</strong> accelerators. For example, new tuning<br />

techniques and associated beam diagnostics are<br />

needed and currently being developed at the laboratory<br />

for the reaccelerator.<br />

Stability analysis for<br />

the motion of particles<br />

with various<br />

kinetic energies in<br />

the lattice of a linear<br />

accelerator. The trajectories<br />

in the longitudinal<br />

phase space<br />

(projections in the zz’<br />

plane) showing a region<br />

where the motion<br />

of the particles<br />

is stable (dark blue)<br />

and a region where it<br />

is unstable (light blue<br />

and beyond).<br />

18 www.nscl.msu.edu<br />

<strong>NSCL</strong>


Alexandra Gade<br />

Assistant Professor<br />

Experimental Nuclear Physics<br />

M.S., Nuclear Physics,<br />

University of Cologne,<br />

1998<br />

PhD, Physics,<br />

University of Cologne,<br />

2002<br />

Joined <strong>NSCL</strong><br />

in April 2002<br />

gade@nscl.msu.edu<br />

Selected Publications<br />

Spectroscopy of 36 Mg: Interplay of normal<br />

and intruder configurations at the<br />

neutron-rich boundary of the “Island of<br />

Inversion.”, A. Gade et al., Phys. Rev.<br />

Lett. 99, 072502 (2007)<br />

In-beam nuclear spectroscopy of<br />

bound states with fast exotic ion beams.<br />

A. Gade and T. Glasmacher, Prog. Part.<br />

Nucl. Phys. 60, 161 (2007)<br />

Measurement of excited states in 40 Si<br />

and evidence for weakening of the<br />

N=28 shell gap, C.M. Campbell et al.,<br />

Phys. Rev. Lett. 97, 112501 (2006)<br />

Direct Evidence for the Onset of Intruder<br />

Configurations in Neutron-Rich<br />

Ne Isotopes, J.R. Terry et al., Phys. Lett.<br />

B 640, 86 (2006)<br />

Quadrupole Deformation of the Self-<br />

Conjugate Nucleus 72 Kr, A. Gade et al.,<br />

Phys. Rev. Lett. 95, 022502 (2005)<br />

The structure of the atomic nucleus at the extremes of<br />

neutron-proton asymmetry is presently the focus of my<br />

research interest. Short-lived, radioactive nuclei that<br />

are composed of many more neutrons than protons,<br />

for example, often reveal surprising properties. The<br />

shape, the excitation pattern as well as the energy<br />

and occupation of the nucleus’ quantum mechanical<br />

orbits by protons and neutrons may be significantly<br />

altered compared to expectations that are based on<br />

the well-known properties of stable nuclei.<br />

My group performs scattering experiments to characterize<br />

the bulk effects of these changes by assessing<br />

the deformation of a nucleus and its excitation pattern.<br />

Nucleon knockout or pickup experiments track<br />

these exciting modifications of the nuclear structure<br />

on the level of the neutron and proton orbits that<br />

make up the nucleus on a microscopic level.<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

Reaction residues generated in<br />

the collision of a 38 Si beam with<br />

a 9 Be target. Energy loss versus<br />

flight time allows for unambiguous<br />

identification of all produced<br />

nuclei. The exotic nucleus<br />

of interest in this experiment was<br />

36 Mg which has twice as many<br />

neutrons as protons.<br />

γ-ray energy spectrum detected<br />

in coincidence with 36 Mg. The<br />

peak at 660 keV energy constitutes<br />

the first measurement of<br />

the energy of the first excited<br />

state in 36 Mg, the heaviest Mg<br />

isotope studied with γ-ray spectroscopy<br />

to date.<br />

In the grazing collision of an exotic projectile beam<br />

with a light target one or two protons or neutrons can<br />

be removed in direct, so-called knockout reaction.<br />

The heavy residue of this reaction is identified and its<br />

kinematics measured with <strong>NSCL</strong>’s large-acceptance<br />

S800 spectrograph. Spectroscopy of de-excitation<br />

γ-rays performed with <strong>NSCL</strong>’s segmented germanium<br />

array SeGA around the target then tells us if the reaction<br />

led to an excited state. The energy of the detected<br />

γ-rays measures the energy difference between<br />

two nuclear states and its intensity tells us how likely<br />

the state was actually populated in such a knockout<br />

reaction.<br />

In intermediate-energy Coulomb excitation, the exotic<br />

nuclei are scattered off a stable gold target and<br />

excited in the electromagnetic Coulomb field of the<br />

target nuclei. Excited energy levels decay back by<br />

the emission of γ radiation, which photon detectors<br />

surrounding the target register. The energy of the γ-ray<br />

reveals the energy of the excited state and its intensity<br />

relates to the probability of the excitation process. This<br />

probability increases with increased deformation of<br />

the nucleus and thus provides a method to characterize<br />

the nuclear shape.<br />

The results from those experiments are often surprising<br />

and reveal that exciting changes take place in the<br />

structure of exotic nuclei compared to stable species.<br />

We work in close collaboration with nuclear structure<br />

theorists and reaction theorists. Our experimental input<br />

helps to unravel the driving forces behind the often<br />

spectacular modifications in nuclear structure and<br />

adds to the improvement of modern theories that are<br />

aimed to provide a model of the atomic nucleus with<br />

predictive power also in the exotic regime.<br />

<strong>NSCL</strong><br />

www.nscl.msu.edu<br />

19


The research in my group focuses on the experimental<br />

exploration of the structure of very exotic atomic nuclei<br />

and the development of experimental techniques and<br />

detectors needed for such studies. Many aspects of<br />

atomic nuclei close to stability are well described with<br />

modern theories that have been extensively tested<br />

against a large set of experimental data. The situation<br />

is different for exotic nuclei far from stability. Here, experimental<br />

data is sparse and theoretical descriptions<br />

have less predictive power. Our goal is to aide in developing<br />

a predictive theory of exotic nuclei by providing<br />

measurements of key observables for exotic nuclei. At<br />

<strong>NSCL</strong>, we prepare beams of exotic nuclei and probe<br />

their internal structure through scattering experiments.<br />

In these experiments, we measure calculable quantum-mechanical<br />

observables with defined precision.<br />

The measured observables can then confront theoretical<br />

predictions.<br />

Most of the experiments we perform employ in-beam<br />

γ-ray spectroscopy of exotic beams at velocities close<br />

to 40% of the speed of light. Photons emitted from<br />

sources moving with such large velocities are strongly<br />

Doppler shifted and the emission angle of the γ-ray<br />

with respect to the scattered beam particle must be<br />

measured in position-sensitive γ-ray detectors. We employ<br />

position-sensitive NaI(Tl) detectors and segmented<br />

Germanium detectors (the SeGA array). We collaborate<br />

with Prof. Gade’s group on the development of<br />

a new CsI detector array (which provides large γ-ray<br />

detection efficiency) and with scientists at Lawrence<br />

Berkeley <strong>National</strong> Laboratory on GRETINA, a next-generation<br />

germanium-based γ-ray spectrometer (which<br />

provides superb energy resolution). A digital data acquisition<br />

system for SeGA is being developed in collaboration<br />

with Prof. Starosta’s group.<br />

Selected Publications<br />

Quadrupole collectivity in silicon isotopes<br />

approaching neutron number N=<br />

28, C.M. Campbell et al., Phys. Lett. B<br />

652, 169 (2007)<br />

Measurement of excited states in 40 Si<br />

and evidence for weakening of the<br />

N=28 shell gap, C.M. Campbell et al.,<br />

Phys. Rev. Lett. 97, 112501 (2006)<br />

Direct evidence for the onset of intruder<br />

configurations in neutron-rich Ne isotopes,<br />

J.R. Terry et al., Phys. Lett. B 640,<br />

86 (2006)<br />

Accuracy of B(E2;0 + →.2 + ) transition rates<br />

from intermediate-energy Coulomb excitation<br />

experiments, J.M. Cook, T. Glasmacher,<br />

and A. Gade. Phys. Rev. C 73,<br />

024315 (2006)<br />

‘Magic’ nucleus 42 Si, J. Fridmann et al., Nature<br />

435, 922 (2005)<br />

M.S., Physics,<br />

Florida State University,<br />

1990<br />

PhD, Physics,<br />

Florida State University,<br />

1992<br />

Joined <strong>NSCL</strong><br />

in November 1992<br />

glasmacher@nscl.msu.edu<br />

Gamma-rays traverse target material with known attenuation<br />

and are thus ideally suited to indicate inelastic<br />

excitations in fast exotic beams. In-beam γ-ray experiments<br />

allow for experiments with very low beam rates<br />

(order of ions/s), where the low beam rate is offset by<br />

the thick secondary targets. Depending on the choice<br />

of target, we can probe the electromagnetic response<br />

of the exotic nuclei in intermediate-energy Coulomb<br />

excitation (with a high-Z target) or the hadronic response<br />

of the exotic nucleus (with a hydrogen target).<br />

Comparison of the two experimental probes allows us<br />

to assess the contributions of protons and neutrons to<br />

excitation strengths separately.<br />

As experimental nuclear physicists we perform experiments<br />

to make inquiries about nature. Understanding<br />

the experimental equipment and the measurement<br />

process is crucial to measuring observables with welldefined<br />

precision.<br />

Spectra of γ-rays<br />

emitted from 40 Si<br />

following the excitation<br />

of a 40 Si<br />

beam in a liquid<br />

hydrogen target<br />

(panel (a)) and<br />

the removal of<br />

a proton and<br />

neutron from a<br />

42<br />

P beam (panel<br />

(b)).<br />

20 www.nscl.msu.edu<br />

<strong>NSCL</strong><br />

Counts / (10 keV)<br />

14<br />

12<br />

10<br />

8<br />

6<br />

4<br />

2<br />

0<br />

8<br />

6<br />

4<br />

2<br />

↓<br />

Thomas Glasmacher<br />

Professor and Associate Director<br />

for Operations<br />

↓<br />

↓<br />

↓<br />

γ-ray Energy (keV)<br />

(a) p( 40 Si, 40 Si + γ)p´<br />

v = 0.411 c<br />

(b) p( 42 P, 40 Si + γ)X<br />

v = 0.405 c<br />

0<br />

400 600 800 1000 1200 1400 1600 1800 2000<br />

Experimental Nuclear Physics


Bill Lynch<br />

Professor<br />

Experimental Nuclear Physics<br />

Selected Publications<br />

Isospin Diffusion Observables in Heavy Ion<br />

Reactions, T. X. Liu et al., Phys. Rev. C 76,<br />

034603 (2007)<br />

B.S., Physics,<br />

University of Colorado,<br />

1973<br />

PhD, Nuclear Physics,<br />

University of Washington,<br />

1980<br />

Joined <strong>NSCL</strong><br />

in December 1980<br />

lynch@nscl.msu.edu<br />

Spin Determination of Particle Unstable Levels<br />

with Particle Correlations, W.P. Tan et al.,<br />

Phys. Rev. C 69, 061304(R) (2004)<br />

Isospin effects in nuclear multifragmentation,<br />

W.P. Tan, S.R. Souza, R.J. Charity, R. Donangelo,<br />

W.G. Lynch, and M.B. Tsang, Phys.<br />

Rev. C 68, 034609 (2003)<br />

Determination of the Equation of State of<br />

Dense Matter, P. Danielewicz, R. Lacey,<br />

W.G. Lynch, Science 298, 1592 (2002)<br />

Imaging Sources with Fast and Slow Emission<br />

Components, G. Verde, D.A. Brown, P.<br />

Danielewicz, C.K. Gelbke, W.G. Lynch, M.B.<br />

Tsang, Phys. Rev. C 65, 054609 (2002)<br />

Our research is focused upon understanding nuclear<br />

collisions and how the information derived from such<br />

collisions can improve the understanding of nuclei,<br />

nuclear matter and neutron stars. Surprising as it may<br />

seem at first, constraints on the pressures that support a<br />

neutron star can be obtained by probing the pressures<br />

that are achieved in nuclear collisions or by examining<br />

the nuclear forces that bind very neutron-rich nuclei.<br />

Such nuclear properties can be related to neutron<br />

star properties through their common dependence on<br />

the equation of state of nuclear matter, which plays<br />

the same role for nuclear systems as the ideal gas law<br />

plays for gases. Finding appropriate constraints on the<br />

nuclear equation of state requires the development<br />

of new experimental devices, new experimental measurements<br />

and theoretical developments.<br />

<strong>NSCL</strong><br />

One of the largest uncertainties in the nuclear equation<br />

of state concerns the symmetry energy, which describes<br />

how the energy of nuclei and nuclear matter<br />

changes as one replaces protons in a system with neutrons,<br />

making the system more and more neutron rich.<br />

In some regions in the interiors of neutron stars, matter<br />

can be of the order of 95% neutrons. Whether this matter<br />

collapses under the gravitational attraction of the<br />

neutron star depends on the repulsive pressure from<br />

the symmetry energy. Experimental measurements<br />

presently do not satisfactorily constrain the pressure<br />

from the symmetry energy. Some of our recent experiments<br />

have provided constraints on the symmetry pressure;<br />

one of our goals is to make such constraints more<br />

stringent.<br />

Recently, our group commissioned the new High Resolution<br />

Array (HiRA), shown in figure, and applied this new<br />

device to investigations of the symmetry energy. This<br />

device was constructed by a collaboration of scientists<br />

at <strong>NSCL</strong>, at the University of Washington in St. Louis and<br />

at Indiana University. It was recently used to measure<br />

the correlations between protons emitted in the collision;<br />

such correlations can be inverted to obtain an image<br />

of the expansion of a compressed nuclear system<br />

and thereby determine the expansion rate. Members<br />

of our research group, some of whom are shown in the<br />

picture, played important roles in the development of<br />

HiRA, as they do with our other research instruments.<br />

<strong>Student</strong>s also play important roles in the interpretation<br />

and theoretical modeling of the data that they measure,<br />

providing them with opportunities to also probe<br />

theoretical aspects of the phenomena that they are<br />

investigating.<br />

www.nscl.msu.edu<br />

21


Nuclear Decay Spectroscopy<br />

Paul F. Mantica<br />

Paul Mantica<br />

PROFESSOR<br />

SELECTED PUBLICATIONS<br />

Nuclear Magnetic Moment of the 57 Cu Ground State,<br />

K. Minamisono, P.F. Mantica, T.J. Mertzimekis, A.D.<br />

(b. 1964)<br />

Davies, M. Hass, J. Pereira, J.S. Pinter, W.F. Rogers, J.B.<br />

Professor<br />

B.S., 1985,<br />

Nuclear Decay Spectroscopy<br />

Stoker, B.E. Tomlin, and R.R. Weerasiri, Phys. Rev. Lett. Rensselaer<br />

Paul F.<br />

Polytechnic<br />

Mantica<br />

2006, 96, 102501.<br />

Nuclear Chemistry<br />

SELECTED PUBLICATIONS<br />

PROFESSOR Institute;<br />

Half-life and Spin of 60 Mn g Nuclear Magnetic Moment of the<br />

, S.N. Liddick, P.F. Mantica,<br />

57 Cu Ground State,<br />

K. Minamisono, P.F. Mantica, T.J. Mertzimekis, A.D.<br />

Ph.D., (b. 1990, 1964)<br />

B.A. Brown, M.P. Selected Carpenter, Publications<br />

Davies, A.D. M. Davies, Hass, J. Pereira, M.Horoi, J.S. Pinter, W.F. Rogers, J.B. University of Maryland, B.S., 1985,<br />

Stoker, B.E. Tomlin, and R.R. Weerasiri, Phys. Rev. Lett. Rensselaer Polytechnic<br />

R.V.F. Janssens, A.C. Morton, 2006, W.F. 96, Mueller, 102501. J. Pavan,<br />

College Institute; Park;<br />

H. Nuclear Schatz, A. Magnetic Stolz, S.L. Tabor, Moment Half-life B.E. and Tomlin, of Spin of the and 57 Cu M.<br />

Weideking, Ground Phys. State, Rev. K. C Minamisono 2006, 73, 044322.<br />

60 Mn g , S.N. Liddick, P.F. Mantica, DOE Postgraduate<br />

Ph.D., 1990,<br />

B.A. Brown, et M.P. al., Carpenter, Phys. A.D. Davies, M.Horoi, University of Maryland,<br />

R.V.F. Janssens, A.C. Morton,<br />

Ground Rev. Lett. State 96, Magnetic 102501 Dipole (2006) Moment of 35 W.F. Mueller, J. Pavan, Research College Training Park;<br />

H. Schatz, A. Stolz, S.L. Tabor, K, T.J. B.E. Tomlin, and M.<br />

Weideking, Phys. Rev. C 2006, 73, 044322.<br />

Program, DOE Postgraduate 1990-93,<br />

Mertzimekis, P.F. Mantica, A.D. Davies, S.N. Liddick,<br />

Research Training<br />

Half-life and Spin of 60 MnGround g , S.N. State Liddick Magnetic et Dipole al., Moment of Oak Ridge<br />

and B.E. Tomlin, Phys. Rev. C 2006, 73, 024318.<br />

35 K, T.J.<br />

Program, 1990-93,<br />

Mertzimekis, P.F. Mantica, A.D. Davies, S.N. Liddick,<br />

Phys. Rev. C 73, 044322 (2006)<br />

Associated B.S., Universities; Oak Ridge<br />

and B.E. Tomlin, Phys. Rev. C 2006, 73, 024318.<br />

Associated<br />

Chemistry,<br />

Universities;<br />

Probing Shell Structure and Shape Probing Shell Changes Structure and in Neutron-rich<br />

Ground Sulfur State Isotopes Magnetic through tron-rich Dipole Transient-field Sulfur Moment Isotopes through of g-Transient-field g-<br />

Shape Changes in<br />

Rensselaer<br />

Neu-<br />

Staff Polytechnic<br />

Staff Scientist,<br />

1993-95, 1993-95, UNISOR,<br />

35 factor Measurements on Fast Radioactive Beams of<br />

factor K, Measurements T.J. Mertzimekis, on Fast 38<br />

P.F. Mantica, Radioactive A.D. Beams Da-ovies,<br />

and S.N. 40 S and<br />

Institute,<br />

38<br />

S S, A.D. Liddick, Davies, and A.E. B.E. Stuchbery, 40 S, A.D. Davies, A.E. Stuchbery, P.F. Mantica,<br />

Oak Ridge<br />

Tomlin, P.F. Phys. Mantica,<br />

Oak P.M. Davidson, A.N. Wilson, Rev. A. Beccerril, B.A. Brown, Associated Universities.;<br />

C.M. Campbell, J.M. Cook, D.C. Dinca, A. Gade, S.N.<br />

1985<br />

P.M. C Davidson, 73, 024318 A.N. (2006) Wilson, A. Beccerril, B.A. Brown, Associated Universities.;<br />

<strong>National</strong> Director,<br />

Liddick, T.J. Mertzimekis, W.F. Mueller, J.R. Terry, B.E.<br />

2006-present,<br />

C.M. Campbell, J.M. Cook, D.C. Tomlin, Dinca, K. Yoneda, A. Gade, and H. Zwahlen, S.N. Phys. Rev.<br />

PhD,<br />

Lett.<br />

Nuclear <strong>National</strong> ACS Chemistry,<br />

Director,<br />

Nuclear and<br />

2006, 96, 112503.<br />

Radiochemistry<br />

Liddick, Probing T.J. Shell Mertzimekis, Structure W.F. and Mueller, Shape J.R. Changes Terry, B.E.<br />

Tomlin,<br />

University<br />

2006-present,<br />

Beta-Decay Half-Lives and Beta-Delayed Neutron of Summer Maryland,<br />

Schools.<br />

Neutron-rich K. Yoneda, Sulfur and H. Isotopes Zwahlen, Emission Probabilities through Phys. Rev. for Transient-field<br />

96, 112503. g-factor Measurements to the N=82 r-Process on Path, Fast F. Montes, A. Estrade, P.T.<br />

Neutron-Rich Lett. Nuclei Close ACS Nuclear and<br />

2006, Radiochemistry College Park,<br />

Beta-Decay Radioactive Half-Lives Beams and of 38 Hosmer, S.N.<br />

Beta-Delayed S and 40 Liddick, P.F. Mantica, A.C. Morton, W.F.<br />

517-355-9672,<br />

Mueller, M. Oullette, S, A.D. E.<br />

Neutron<br />

Pellegrini, Davies<br />

et Probabilities al., Phys. Rev. for Lett. A. Stolz,<br />

P. Santi, H. Schatz,<br />

Ext. 456<br />

Summer Schools. 1990<br />

Emission Neutron-Rich 96, B.E. 112503 Tomlin, O.<br />

Nuclei (2006) Arndt, K.-L. Kratz, B. Pfeiffer, P.<br />

Reeder, W.B. Walters, A. Aprahamian, Close and A. Woehr,<br />

to the N=82 r-Process Path, F.<br />

Phys.<br />

Montes,<br />

Rev. C 2006,<br />

A.<br />

73,<br />

Estrade,<br />

035801.<br />

P.T.<br />

Hosmer,<br />

Beta-Decay<br />

S.N. Liddick,<br />

Half-Lives<br />

P.F. Mantica,<br />

and<br />

A.C.<br />

Beta-Delayed<br />

Morton, W.F.<br />

517-355-9672, Joined <strong>NSCL</strong><br />

y research has focused on<br />

Mueller,<br />

Neutron the study<br />

M. Oullette,<br />

Emission of low-energy<br />

E.<br />

Probabilities with a single<br />

Pellegrini, P. Santi,<br />

for proton Neutron- outside the purported “doubly-magic”<br />

H. Schatz,<br />

in August Ext. 4561995<br />

Rich Nuclei Close to the N=82 r-Process<br />

M<br />

Ni<br />

properties of nuclei far from the valley of ! stability<br />

to provide experimental support for the dramatic neighboring nuclei and shell model predictions (see figure).<br />

nucleus, and its mirror partner,<br />

A.<br />

Path,<br />

Stolz, B.E.<br />

F.<br />

Tomlin,<br />

Montes<br />

O.<br />

et<br />

Arndt,<br />

al.,<br />

K.-L.<br />

Phys.<br />

Kratz,<br />

Rev.<br />

B. Pfeiffer,<br />

C 73,<br />

P.<br />

57 Ni, differ significantly from<br />

structure changes predicted for nuclei Reeder,<br />

035801 with W.B. extreme (2006)<br />

Walters, neutronto-proton<br />

ratios. Two experimental approaches are used in Efforts in the !-decay spectroscopy program has focused<br />

A. Aprahamian, and A. Woehr,<br />

Phys. Rev. C 2006, 73, 035801.<br />

mantica@nscl.msu.edu<br />

these studies: !-NMR spectroscopy to measure ground state on finding evidence for dramatic changes in the neutron<br />

moments of nuclei near the proton with drip line a single and !-decay proton spectroscopy<br />

to probe the low-energy<br />

outside single-particle the spectrum purported of nuclides “doubly-magic” above 48 Ca attributed 56 Ni to<br />

nucleus, and its mirror partner, 57 the tensor<br />

Ni, differ Single-nucleon<br />

monopole interaction.<br />

significantly from g factors<br />

number (g p (see 32 = for proton figure). calcium, g<br />

quantum structure of neutron-rich<br />

Evidence for a new subshell gap at<br />

nuclei. Both approaches make use neighboring nuclei and shell model predictions neutron<br />

of short-lived, !-unstable nuclei<br />

titanium, factor, and chromium g n = neutron is based<br />

produced via projectile fragmentation<br />

at the <strong>National</strong> Superconduct-<br />

Efforts in the !-decay spectroscopy Shell program model calculations has focused predict a<br />

partly on results of our research.<br />

g factor) of mirror nuclei.<br />

shell gap The at results neutron number for the<br />

ing Cyclotron Laboratory (<strong>NSCL</strong>)<br />

new<br />

at Michigan State University. on finding evidence for dramatic changes 34 for 35 calcium K/ 35 in S and the mirror titanium neutron partners nuclei.<br />

single-particle spectrum of nuclides above Our study<br />

agree 48 Ca of the attributed low-energy quantum<br />

states of<br />

with the linear to<br />

The determination of dipole<br />

the tensor monopole 56 Ti, which has 34<br />

and quadrupole moments of exotic<br />

neutrons, trend did known not interaction.<br />

find evidence for stable for<br />

nuclei can provide insight into new<br />

Evidence for a a significant new nuclei, subshell shell although gap at gap neutron at<br />

35 K<br />

features of nuclear structure. The<br />

number 34 as expected from theory.<br />

nuclear magnetic dipole moment<br />

neutron is weakly 32 for bound. calcium, The<br />

is sensitive to the orbital contribution<br />

to the nuclear state wave func-<br />

new instrumentation to advance<br />

titanium, and We mirror chromium continue pair to is 57 implement based Cu/ 57 Ni<br />

partly on results deviates of our from research. the<br />

tion, while the electric quadrupole<br />

our studies of nuclei at the limits<br />

moment is a direct measure of the<br />

Shell model of calculations existence. trend The line, new predict<br />

suggesting<br />

Digital Data a<br />

nuclear charge distribution. Nuclear<br />

Acquisition a collapse system of will the improve 56 Ni<br />

moments at the <strong>NSCL</strong> are measured<br />

new shell gap detection at neutron efficiencies number<br />

by a factor<br />

with the technique of nuclear magnetic<br />

resonance on !-emitting nu-<br />

The Radio Frequency Fragment<br />

core.<br />

34 for calcium of two and for titanium !-decay experiments. nuclei.<br />

clei (!-NMR). We have measured Single-nucleon g factors (g p<br />

= proton g factor, Our g n<br />

= study neutron of Separator the low-energy has recently been quantum<br />

35 K/ 35 S mirror<br />

commissioned<br />

of at 56 neutron Ti, at which the <strong>NSCL</strong>. number has This new 34 32<br />

the ground state magnetic moment g factor) of mirror nuclei. The results for the<br />

Evidence for a new subshell states gap<br />

of 35 K, which has small proton separation<br />

energy and resides close to for clei, calcium, although titanium, and neutrons, chromium did not is find based evidence partly for<br />

35 K is weakly bound. The mirror pair 57 Cu/ 57 Ni nuclei nearest the proton drip line on<br />

partners agree with the linear trend known for stable nu-<br />

device will permit access to heavy<br />

the proton drip line. The magnetic deviates from the trend line, suggesting a collapse of the<br />

results of our research. Shell significant<br />

for<br />

model shell<br />

both !-decay<br />

calculations gap<br />

and<br />

at<br />

!-NMR<br />

neutron<br />

spectroscopic<br />

studies. Finally, a recent<br />

moments of predict<br />

35 56<br />

K and its mirror partner<br />

a new shell gap at neutron number number 34 as expected 34 for from calcium theory.<br />

35 S agree surprisingly well with<br />

upgrade of the NMR systems has and<br />

Ni core.<br />

the systematic trends observed for other, more stable nuclides. allowed us to obtain a precise measurement of the ground<br />

In contrast, we have found that the magnetic moments of 57 Cu, state quadrupole moment of the short-lived nucleus 37 K.<br />

My research research has has focused on on the the study of low-energy<br />

properties properties of nuclei of nuclei far from far from the valley the valley of β of stability ! stability<br />

experimental to provide experimental support for support the dramatic for the dramatic struc-<br />

to<br />

provide<br />

ture structure changes changes predicted for for nuclei nuclei with with extreme extreme neutronto-proton<br />

ratios.<br />

neutron-to-proton<br />

ratios.<br />

Two experimental<br />

Two experimental<br />

approaches<br />

approaches<br />

are used in<br />

these studies: !-NMR spectroscopy to measure ground state<br />

are used in these studies: β-NMR spectroscopy to measurtroscopy<br />

ground to probe state the moments low-energy of nuclei near the proton<br />

moments of nuclei near the proton drip line and !-decay spec-<br />

drip quantum line and structure β-decay of neutron-rich spectroscopy to probe the lowenergy<br />

nuclei. Both quantum approaches structure make of use neutron-rich nuclei. Both<br />

approaches of short-lived, make !-unstable use of nuclei short-lived, β-unstable nuclei<br />

produced via via projectile fragmentation<br />

at the <strong>National</strong> Superconduct-<br />

fragmentation at <strong>NSCL</strong>.<br />

The ing determination Cyclotron Laboratory of dipole (<strong>NSCL</strong>) and quadrupole moments<br />

of at exotic Michigan nuclei State can provide University. insight into new features<br />

of nuclear structure. The nuclear magnetic dipole moment<br />

The is sensitive determination to the of orbital dipole contribution to the nuclear<br />

and state quadrupole wave moments function, of while exotic the electric quadrupole<br />

moment nuclei can is provide a direct insight measure into new of the nuclear charge<br />

distribution. features of nuclear Nuclear structure. moments The at <strong>NSCL</strong> are measured<br />

with<br />

nuclear<br />

the<br />

magnetic<br />

technique<br />

dipole<br />

of nuclear<br />

moment<br />

mag- netic resonance titanium nuclei. Our study of the low-energy quantum<br />

is sensitive to the orbital contribution<br />

to the nuclear state wave func-<br />

new instrumentation to advance<br />

We continue to implement<br />

on β-emitting nuclei (β-NMR). We have measured the states of 56 Ti, which has 34 neutrons, did not find evidence<br />

for a significant shell gap at neutron number 34<br />

ground tion, while state the magnetic electric quadrupole moment of 35 K, which has small<br />

mantica@msu.edu<br />

33 our studies www.chemistry.msu.edu/mantica<br />

of nuclei at the limits<br />

proton moment separation is a direct measure energy of and the resides close to the proton<br />

nuclear drip charge line. The distribution. magnetic Nuclear moments of 35 K and its mirror<br />

as expected from theory. of existence. The new Digital Data<br />

We continue to implement Acquisition new instrumentation system will improve to advance<br />

our studies of nuclei at the limits of existence.<br />

partner moments 35 at S the agree <strong>NSCL</strong> surprisingly are measured well with the systematic<br />

detection efficiencies by a factor<br />

trends with the observed technique for of nuclear other, more magnetic<br />

resonance we have on found !-emitting that the nu-<br />

magnetic moments of<br />

The Radio Frequency Fragment<br />

stable nuclides. In contrast,<br />

of two for !-decay experiments.<br />

The new Digital Data Acquisition system will improve<br />

57 clei detection efficiencies by a factor of two for β-decay<br />

Cu, (!-NMR). with a single We have proton measured outside Single-nucleon the purported g factors “doubly-magic”<br />

the ground state Ni nucleus, magnetic and moment g factor) of mirror<br />

(g p<br />

= proton g factor, g n<br />

= neutron Separator has recently been commissioned<br />

at the <strong>NSCL</strong>. This new<br />

experiments. The Radio Frequency Fragment Separator<br />

has recently been commissioned at <strong>NSCL</strong>. This new<br />

its mirror partner, 57 nuclei. The results for the<br />

Ni, differ<br />

35 K/ 35 S mirror<br />

significantly<br />

of 35 K, which has<br />

from<br />

small<br />

neighboring<br />

proton separation<br />

energy and resides close to clei, although 35 K is weakly bound. device The mirror will pair permit 57 Cu/ 57 Ni access nuclei to nearest heavy the nuclei proton nearest drip line the<br />

partners agree with the linear trend known for stable nu-<br />

nuclei and shell model<br />

device will permit access to heavy<br />

predictions.<br />

the proton drip line. The magnetic deviates from the trend line, suggesting proton a drip collapse line of for the both for both β-decay !-decay and and β-NMR !-NMR spectroscopic<br />

studies. Finally, troscopic a recent studies. upgrade Finally, of a the recent NMR<br />

spec-<br />

Efforts moments in of the 35 56<br />

K β-decay and its mirror spectroscopy partner<br />

35 S agree on finding surprisingly evidence well with for dramatic changes in systems has allowed us upgrade to obtain of the a NMR precise systems measure-<br />

has<br />

Ni core.<br />

program has focused<br />

the<br />

the systematic<br />

neutron single-particle<br />

trends observed<br />

spectrum<br />

for other, more<br />

of nuclides<br />

stable nuclides.<br />

above<br />

allowed<br />

ment of<br />

us<br />

the<br />

to obtain<br />

ground<br />

a precise<br />

state<br />

measurement<br />

quadrupole<br />

of<br />

moment<br />

the ground<br />

of the<br />

48<br />

In contrast, we have found that the magnetic moments of<br />

Ca attributed to the tensor monopole interaction.<br />

57 Cu, state quadrupole moment of the short-lived nucleus<br />

short-lived nucleus 37 K.<br />

37 K.<br />

33<br />

www.chemistry.msu.edu/mantica<br />

22 www.nscl.msu.edu<br />

<strong>NSCL</strong><br />

mantica@msu.edu<br />

CHEMISTRY RESEARCH FACULTY<br />

CHEMISTRY RESEARCH FACULTY


Felix Marti<br />

Professor and Senior Physicist<br />

Accelerator Physics & Engineering<br />

B.S., Physics,<br />

University of the Republic<br />

Montevideo,<br />

1973<br />

M.S., Physics,<br />

Michigan State University,<br />

1975<br />

PhD, Physics,<br />

Michigan State University,<br />

1977<br />

Joined <strong>NSCL</strong><br />

in July 1979<br />

marti@nscl.msu.edu<br />

Selected Publications<br />

The Cyclotron Gas Stopper project at the<br />

<strong>NSCL</strong>, G.K. Pang et al., Proc. Part. Accel.<br />

Conf. PAC07, 3588 (2007)<br />

Design, Construction and Commissioning of<br />

the SUSI ECR, P.A. Zavodszky et al., Proc. Part.<br />

Accel. Conf. PAC07, 3766 (2007)<br />

End-to-end beam dynamics simulation of the<br />

ISF driver LINAC, Q. Zhao et al., Proc. Part. Accel.<br />

Conf. PAC07, 1775 (2007)<br />

An upgrade to the <strong>NSCL</strong> to produce intense<br />

beams of exotic nuclei, R. C. York et al., Proc.<br />

Lin. Acc. Conf. LINAC06, 103 (2006)<br />

Study of space charge effects using a small<br />

storage ring that works in the isochronous regime,<br />

F. Marti, E. Pozdeyev and J. Rodriguez,<br />

Proc. 17 th Intl. Conf. Cyclotrons and their Applications<br />

2004, p. 430 (2005)<br />

My research interests are in the area of accelerator<br />

physics. I have been involved in the design and construction<br />

of the two superconducting cyclotrons (K500<br />

and K1200) used for nuclear physics research at <strong>NSCL</strong>,<br />

as well as a neutron cancer therapy cyclotron used in<br />

a Detroit hospital.<br />

<strong>NSCL</strong> has a long trajectory of innovation in the design<br />

of cyclotrons starting in the early 1960s. In the last few<br />

decades the introduction of high field superconducting<br />

magnets and more recently superconducting radio<br />

frequency acceleration systems has allowed the<br />

construction of more compact and consequently less<br />

expensive accelerators.<br />

accelerators with beam power of the order of a megawatt<br />

in a small-scale accelerator with beam power of<br />

just a few watts. With that in mind a small storage ring<br />

was built that is dedicated full time to student work. A<br />

very successful experimental program confirmed the<br />

theoretical predictions of beam instabilities.<br />

The accelerator group has worked with several industrial<br />

companies that fabricate accelerators for cancer<br />

therapy serving as advisors and transferring new technologies.<br />

The design of compact accelerators requires the solution<br />

of complicated electromagnetic problems with<br />

high accuracy. As an example, the magnets have to<br />

be machined and aligned to accuracies of tenths of<br />

micrometers. The development of sophisticated software<br />

for the solution of electromagnetic problems has<br />

allowed the construction of new accelerators with very<br />

little prototyping. The accelerator group at <strong>NSCL</strong> has<br />

developed a comprehensive library of beam dynamics<br />

codes used to simulate the physics of beams in cyclotrons<br />

and linacs.<br />

<strong>Student</strong>s in the accelerator physics area are involved<br />

in the design from basic principles of the different components<br />

of the accelerators as well as in experimental<br />

work during commissioning of new devices. The study<br />

of the internal forces within the beam (space charge<br />

effects) has been the topic of several students in recent<br />

years. The goal is to simulate the effects of high-energy<br />

View of a beam bunch in the storage ring after breaking up due to<br />

space charge forces. The beam is moving from left to right. The red<br />

line shows the intensity projected along the bunch length. The study<br />

of the formation and evolution of the clusters has been the topic of<br />

student research projects.<br />

<strong>NSCL</strong><br />

www.nscl.msu.edu<br />

23


Wolfgang Mittig<br />

Hannah Professor<br />

Experimental Nuclear Physics<br />

Selected Publications<br />

Maya: An Active-Target Detector for Binary Reactions<br />

with Exotic Beams, C.E. Demonchy et al.,<br />

Nucl. Instrum. Meth. A583, 341 (2007)<br />

Resonance State in 7 H, M.Caamano et al., Phys. Rev.<br />

Lett. 99, 062502 (2007)<br />

Exotic Nuclei, why and how to make them? W. Mittig,<br />

P. Roussel-Chomaz and A.C.C. Villari, Europhysics<br />

News 35, 113 (2004)<br />

High Intensity Beams at Ganil and Future Opportunities,<br />

and Simplified Project Report: LINAG-Phase<br />

I, G. Auger, W. Mittig, M.H. Moscatello and A.C.C.<br />

Villari, Report Ganil R 01 02 (2001)<br />

Mass Measurements Far from Stability, W. Mittig, A.<br />

Lepine-Szily and N.A. Orr, Ann. Rev. Nucl. Part. Sci.<br />

47, 27 (1997)<br />

Docteur ès Sciences,<br />

Université de Paris,<br />

1971<br />

Livre Docente,<br />

University of Sao Paulo,<br />

1977<br />

Joined <strong>NSCL</strong><br />

in January 2008<br />

mittig@nscl.msu.edu<br />

Since my university studies, first in Germany and later<br />

in France, I involved myself often in very general problematics,<br />

such as the foundation of quantum mechanics<br />

(Bell inequality), precision measurements to search<br />

for nuclear color-VanderWaals forces, nuclear energy<br />

and environment, formation of superheavy systems,<br />

and very recently the possibility of resonant neutrino<br />

scattering.<br />

Z<br />

Recently, I was mainly working on experimental nuclear<br />

physics, and more specifically on the spectroscopy<br />

of exotic nuclei. This domain is at the frontline of present<br />

nuclear physics and is extremely challenging for an<br />

experimental physicist. Many new techniques have to<br />

be developed in order to study very rare nuclei far from<br />

stability. We developed an “active target,” a detector<br />

in which the detection gas is at the same time the<br />

target. This technique combines a large solid angle, in<br />

principle 4π, with a thick target and good resolution.<br />

The particles, beam and reaction products, are visualized<br />

by their ionization path in the gas. A detailed<br />

event-by-event analysis provides the reaction angles,<br />

Q-values, angular distributions, and excitation functions<br />

of the reactions.<br />

Y<br />

beam<br />

X<br />

K<br />

At <strong>NSCL</strong> we formed a collaboration for the<br />

development of such a device with even<br />

increased performance, to become operational<br />

in about 2-3 years, together with the<br />

future linear post-accelerator for rare unstable<br />

beams. The detailed specifications will<br />

be defined during this year. The combination<br />

of this detector with the new post-accelerator<br />

will provide new and competitive<br />

possibilities to study properties of very exotic<br />

nuclei.<br />

gassiplex<br />

A schematic view of the active target Maya.<br />

24 www.nscl.msu.edu<br />

<strong>NSCL</strong>


David Morrissey<br />

University Distinguished Professor<br />

Nuclear Chemistry<br />

Nuclear Chemistry<br />

B.S., Chemistry,<br />

Pennsylvania<br />

State University,<br />

1975<br />

<strong>NSCL</strong><br />

Selected Publications<br />

Beta-delayed Neutron Decay of 19 N and<br />

20 N, C.S. Sumithrarachchi, D.W. Anthony,<br />

P.A. Lofy, and D.J. Morrissey, Phys. Rev. C 74,<br />

024322 (2006)<br />

A Laser Ablation Ion Source for Gas Cell<br />

Studies, D.A. Davies, D.J. Morrissey, G. Bollen,<br />

P.A. Lofy, S. Schwarz, and J. Ottarson,<br />

Nucl. Instrum. Meth. A569, 883 (2006)<br />

SELECTED PUBLICATIONS<br />

Beta-delayed Neutron Decay of 19 N and 20 N, C.S.<br />

Experiments with Thermalized Rare Isotope Sumithrarachchi, D.W. Anthony, P.A. Lofy, and D.J.<br />

Beams from Projectile Fragmentation - A Morrissey, Phys. Rev. 2006, C74, 024322<br />

Precision Mass Measurement of the Superallowed<br />

β-Emitter, 38 Ca, G. Bollen et al., Davies, D.J. Morrissey, G. Bollen, P.A. Lofy, S. Schwarz,<br />

A Laser Ablation Ion Source for Gas Cell Studies, D.A.<br />

Phys. Rev. Lett. 96, 1525101 (2006)<br />

and J. Ottarson, Nucl. Instrum. Meth. 2006, A569, 883.<br />

Conversion of 92 MeV/u 38 Ca / 37 K Projectile Fragments<br />

Modern Nuclear Chemistry, W. Loveland, into Thermalized Ion Beams, L. Weissman, D.J.<br />

D.J. Morrissey and G.T. Seaborg, Wiley Interscience<br />

(2006)<br />

Schury, S. Schwarz, C. Sumithrarachchi, T. Sun, and R.<br />

Morrissey, G. Bollen, D.A. Davies, E. Kwan, P.A. Lofy, P.<br />

Ringle, Nucl. Instrum. Meth. Part. Sci. 2005, A540, 245.<br />

Conversion of 92 MeV/u 38 Ca / 37 K Projectile Experiments with Thermalized Rare Isotope Beams<br />

Fragments into Thermalized Ion Beams, L. from Projectile Fragmentation - A Precision Mass Measurement<br />

of the Super-allowed !-Emitter, 38 Ca, G. Bol-<br />

Weissman et al., Nucl. Instrum. Meth. A540,<br />

245 (2005)<br />

len, et al., Phys. Rev. Lett. 2006, 96 1525101.<br />

Modern Nuclear Chemistry, W. Loveland, D.J. Morrissey<br />

and G.T. Seaborg (Wiley Interscience, 2006).<br />

Radioactive Nuclear Beam Facilities Based on Projectile<br />

Fragmentation, D. J. Morrissey, and B. M. Sherrill, Proc.<br />

Royal Soc. A, 356. 1985 (1998), and Lecture Notes on<br />

Physics 2004, 651, 113.<br />

UNIVERSITY<br />

DISTINGUISHED<br />

PROFESSOR<br />

(b. 1953)<br />

B.S., 1975,<br />

PhD, Chemistry,<br />

Pennsylvania State<br />

University;<br />

University of California,<br />

Ph.D., 1978,<br />

1978<br />

University of California,<br />

Berkeley;<br />

Joined <strong>NSCL</strong><br />

Postdoctoral Fellow,<br />

1978-1981,<br />

in September 1981<br />

Lawrence Berkeley<br />

Laboratory;<br />

morrissey@nscl.msu.edu<br />

Visiting Scientist,<br />

1987-1988,<br />

GSI, Darmstadt, BRD;<br />

My research lies in the realm of nuclear chemistry and<br />

Associate Director,<br />

an auxiliary device to deliver the exotic<br />

<strong>National</strong><br />

reaction products<br />

at thermal energies. In this project, <strong>Superconducting</strong> we have ex-<br />

centers on studies of the production and use of the<br />

Cyclotron Laboratory,<br />

most exotic, short-lived nuclei created in nuclear reactions.<br />

We have applied this knowledge to produce developed primarily in Europe and Japan and recently<br />

tended the ion-guide ion-source (IGISOL) 1995-1999. technique<br />

517-355-9672,<br />

beams of very exotic radioactive ions. These nuclei are by another group at Argonne <strong>National</strong> Ext. Lab 321 to collect<br />

interesting in their own right, some of which have not individual ions. The new device is tailored to stop and<br />

been observed before. My graduate students have collect the exotic isotopes produced by the A1900 fragment<br />

produced separator by the at A1900 <strong>NSCL</strong> fragment using separator a differentially at the pumped<br />

worked My on unraveling research lies the in the mechanisms realm of nuclear of chemistry nuclear and reactions<br />

and on centers studying on studies the of decay the production properties and use of of exotic the <strong>NSCL</strong> gas using cell a differentially in a process pumped related gas cell to in a atmospheric process relat-<br />

sampling<br />

isotopes<br />

most exotic, short-lived nuclei created in nuclear reactions.<br />

We have applied this knowledge to produce beams gas-catcher system has begun operation and a number of suced<br />

to atmospheric sampling mass spectrometry. The so-called<br />

nuclei. <strong>NSCL</strong> is a unique facility that brings together a mass spectrometry. The so-called gas-catcher system<br />

strong of group very exotic of nuclear radioactive scientists ions. These and nuclei provides are interesting an in ex-cessfuceptional their own setting right, for some studying of which have the not properties been observed of before. nuclei. out by tremely the group precise headed by mass Prof. measurements Bollen (MSU Physics has Dept.). been carried<br />

has extremely begun precise operation mass measurements and a number has been carried of successful ex-<br />

The cyclotrons The experiments accelerate are carried out ions at the that <strong>National</strong> span <strong>Superconducting</strong><br />

Cyclotron<br />

the periodic out by the group headed by Prof. Bollen.<br />

table and have<br />

Laboratory<br />

very high<br />

(<strong>NSCL</strong>),<br />

kinetic<br />

next<br />

energies.<br />

door to the Chemistry<br />

When the<br />

Building. My graduate students have worked on unraveling<br />

fast ions the react mechanisms with of a nuclear target reactions nucleus, and on the studying incident the de-iocay<br />

broken properties into of exotic pieces nuclei. with The a <strong>NSCL</strong> distribution a unique of facility sizes,<br />

is often<br />

many that of which brings together are unstable a strong group and of quite nuclear scientists unusual. and The<br />

probability<br />

provides<br />

distributions<br />

an exceptional<br />

of<br />

setting<br />

the products<br />

for studying<br />

were<br />

the properties<br />

early subjects<br />

of table study and have by my very group high kinetic and energies. can be When predicted the fast ions with<br />

of<br />

nuclei. The cyclotrons accelerate ions that span the periodic<br />

reasonable react with accuracy. a target nucleus, The the momenta, incident ion or is velocities, often broken of<br />

A plot of the energyloss<br />

in a detector as a<br />

the fragments into pieces with were a distribution shown to of sizes, be many distributed of which are around unstable<br />

that of the<br />

and<br />

beam<br />

quite unusual.<br />

and to<br />

The<br />

be<br />

probability<br />

predicted<br />

distributions<br />

by models<br />

of the<br />

function of time-of-flight<br />

of<br />

products were early subjects of study by my group and can be<br />

through a fragment separator<br />

for products from<br />

the nuclear predicted reaction. with reasonable These accuracy. fast moving The momenta, fragments or velocities,<br />

of the through fragments an were isotope shown to separator be distributed to around produce that<br />

the reaction of 78 Kr with a<br />

can<br />

be passed<br />

beams of of the individual beam and to radioactive be predicted by models ions. The of the A1200 nuclear fragment<br />

separator<br />

reaction.<br />

These<br />

58 Ni target. The arrow indicates<br />

the ‘gap’ where<br />

was<br />

fast<br />

the<br />

moving<br />

central<br />

fragments<br />

instrument<br />

can be passed<br />

for research<br />

through<br />

an isotope separator to produce beams of individual radioactive<br />

and ions. provided The A1200 intense fragment beams separator of at unstable the <strong>NSCL</strong> was ions<br />

observed.<br />

69 Br should have been<br />

at <strong>NSCL</strong><br />

to study the nuclear central instrument reactions for research and decay at the <strong>NSCL</strong> properties. and provided This<br />

separator intense has beams been of unstable replaced ions to in study 2001 nuclear by a reactions larger and and<br />

more efficient<br />

decay properties.<br />

device<br />

This<br />

called<br />

separator<br />

the<br />

has been<br />

A1900<br />

replaced<br />

as part<br />

in 2001<br />

of<br />

by<br />

the<br />

a larger and more efficient device called the A1900 as part of<br />

upgrade the upgrade of the <strong>NSCL</strong> of the <strong>NSCL</strong> facility facility that that brings brings new possibilities<br />

for studying for studying the the most exotic, short-lived nuclei. nuclei. Along with using<br />

the new fragment separator, our group has completed the<br />

Along construction with using and the development new fragment of an auxiliary separator, device our to deliver group<br />

has completed<br />

the exotic reaction<br />

the construction<br />

products at thermal<br />

and<br />

energies.<br />

development<br />

In this proj-<br />

of<br />

ect, we have extended the ion-guide ion-source (IGISOL) technique<br />

developed primarily in Europe and Japan and recently by<br />

another group at Argonne <strong>National</strong> Lab to collect individual<br />

ions. The new device is tailored to stop and collect the exotic<br />

morrissey@nscl.msu.edu<br />

37<br />

David J. Morrissey<br />

A plot of the energy-loss in a detector as a function of<br />

time-of-flight through a fragment separator for products<br />

from the reaction of 78 Kr with a 58 Ni target. The arrow indicates<br />

the ‘gap’ where 69 Br should have been observed.<br />

www.nscl.msu.edu<br />

www.chemistry.msu.edu/morrissey<br />

CHEMISTRY RESEARCH FACULTY<br />

25


Filomena Nunes<br />

Assistant Professor<br />

Theoretical Nuclear Physics<br />

Selected Publications<br />

B(E1) strengths from the Coulomb excitation<br />

of 11 Be N. Summers et al., Phys. Lett. B 650,<br />

124 (2007)<br />

Scaling and interference in the dissociation<br />

of halo nuclei, M.S. Hussein, R. Lichtenthäler,<br />

F.M. Nunes and I.J. Thompson, Phys. Lett. B<br />

640, 91 (2006)<br />

Extended continuum discretized coupled<br />

channels method: Core excitation in the<br />

breakup of exotic nuclei, N. C. Summers, F.<br />

M. Nunes, and I. J. Thompson, Phys. Rev. C<br />

74, 014606 (2006)<br />

Effects of deformation in the three-body<br />

structure of 11 Li, I. Brida, F.M. Nunes and B.A.<br />

Brown, Nucl. Phys. A775, 23 (2006)<br />

Combined method to extract spectroscopic<br />

information, A. M. Mukhamedzhanov and<br />

F. M. Nunes, Phys. Rev. C 72, 017602 (2005)<br />

Engenharia Fisica<br />

Technologica,<br />

Instituto Superior<br />

Tecnico Lisboa,<br />

1992<br />

PhD, Theoretical<br />

Physics,<br />

University of Surrey,<br />

England,<br />

1995<br />

Joined <strong>NSCL</strong><br />

in February 2003<br />

nunes@nscl.msu.edu<br />

I study direct nuclear reactions and structure models<br />

that are useful in the description of reactions. Unstable<br />

nuclei are mostly studied through reactions, because<br />

they decay back to stability (often lasting less than a<br />

few seconds). My work focuses on developing models<br />

for reactions with exotic unstable nuclei. Reaction theory<br />

is very important because it makes the connection<br />

between experiments such as the ones performed at<br />

<strong>NSCL</strong>, and the nuclear structure information we want<br />

to extract. Within the realm of direct reactions, my contributions<br />

have been toward understanding inelastic<br />

excitation, breakup and transfer reactions.<br />

Given that many unstable nuclei break up so easily,<br />

the nucleus can go through the continuum (scattering<br />

states) in the reaction. Introducing breakup accurately<br />

involves computer intensive calculations, so we use the<br />

High Performance Computers at MSU.<br />

The motivation to study these reactions are three-fold.<br />

Breakup and transfer reactions can be used as indirect<br />

methods to obtain capture rates of astrophysical relevance.<br />

These capture rates enter in the simulations of<br />

stars, and explosive sites such as novae and supernovae.<br />

In addition, reliable models for some specific direct<br />

reactions are crucial for nuclear waste management.<br />

Finally, and most importantly, we also need reactions<br />

to unveil the hidden secrets of the effective nuclear<br />

force which binds some exotic systems such and not<br />

others.<br />

Nuclei are many body systems of large complexity. Describing<br />

a reaction while retaining all the complexity of<br />

the projectile and target nuclei would be a daunting<br />

task. Fortunately, to describe many direct reactions,<br />

only a few structure degrees of freedom are necessary.<br />

Thus we develop simplified few-body structure<br />

models which retain the important features of the nucleus<br />

of interest and can be used as input to the reaction<br />

calculations. When comparing with the data,<br />

we learn whether our initial assumptions were correct.<br />

When there are too many neutrons or protons in a nucleus, strange<br />

things happen. An example is shown in the figure: 11 Li is a nucleus<br />

with 8 neutrons but only 3 protons. It has a central core but has two<br />

valence neutrons which hang loosely to the 9 Li core, in an orbital<br />

of the size of Pb. If we remove any of the bodies (the core or either<br />

neutrons), the system falls apart. This is a characteristic also seen in<br />

Borromean rings. It means that the binding of the valence neutrons<br />

to the core is very, very subtle. Albeit the efforts developed over the<br />

last 20 years since the appearance of radioactive beam facilities,<br />

the effective force that keeps unstable systems together (whether it<br />

is 11 Li or 100 Sn) still has hidden secrets to unveil.<br />

26 www.nscl.msu.edu<br />

<strong>NSCL</strong>


Hendrik Schatz<br />

Professor<br />

Experimental Nuclear Astrophysics<br />

Selected Publications<br />

Heating in the Accreted Neutron Star Ocean: Implications<br />

for Superburst Ignition, S. Gupta, E.F.<br />

Brown, H. Schatz, P. Moeller, and K.-L. Kratz, Astrophys.<br />

J. 662, 1188 (2007)<br />

M.S., Physics,<br />

University of Karlsruhe,<br />

1993<br />

PhD, Physics,<br />

University of Heidelberg,<br />

1997<br />

Joined <strong>NSCL</strong><br />

in December 1999<br />

schatz@nscl.msu.edu<br />

X-ray Binaries, H. Schatz and K.E. Rehm, Nucl.<br />

Phys. A 777, 601 (2006)<br />

The importance of nuclear masses in the astrophysical<br />

rp-process, H. Schatz, Int. Jour. Mass Spect. 251,<br />

293 (2006)<br />

Half-life of the Doubly Magic r-process Nucleus 78 Ni,<br />

P. Hosmer, H. Schatz, A. Aprahamian, O. Arndt,<br />

R.R. Clement, A. Estrade, K.L. Kratz, S.N. Liddick,<br />

P.F. Mantica, W.F. Mueller, F. Montes, A.C. Morton,<br />

M. Ouellette, E. Pellegrini, B. Pfeiffer, P. Reeder, P.<br />

Santi, M. Steiner, A. Stolz, B.E. Tomlin, W.B. Walters,<br />

A. Wöhr, Phys. Rev. Lett. 94, 112501 (2005)<br />

A New Approach for Measuring Properties of rp Process<br />

Nuclei, R.R.C. Clement et al., Phys. Rev. Lett.<br />

92, 2502 (2004)<br />

Our group’s interdisciplinary research program is at the<br />

intersection of nuclear physics and astrophysics. The<br />

goal is to understand the nuclear processes that occur<br />

naturally in our universe. Nuclear reactions created, and<br />

still create, the chemical elements our world is made of.<br />

Nuclear reactions make the sun and all the stars shine,<br />

and nuclear reactions power some of the greatest fireworks<br />

in our universe - stellar explosions like supernovae,<br />

novae, and X-ray bursts. Our research is tied in closely<br />

with the Joint Institute for Nuclear Astrophysics (JINA), offering<br />

unique opportunities for interdisciplinary research,<br />

such as targeted schools and workshops, opportunities<br />

for student and postdoc exchange with other institutions<br />

in the US and world wide, interaction with visitors,<br />

and a JINA club for students and postdocs.<br />

Our main interest is the role that very unstable radioactive<br />

nuclei play in astrophysics. Despite their very short<br />

lifetimes - many decay within 10-100 milliseconds - they<br />

can shape the nature of the observed stellar explosions.<br />

They are also intermediate steps for the synthesis of the<br />

elements. Elements like silver, gold or uranium found today<br />

on Earth are the decay products of exotic isotopes<br />

probably produced in supernova explosions. Very unstable<br />

nuclei therefore determine the composition of<br />

the entire universe. Another site where unstable nuclei<br />

exist in large quantities are the crusts of neutron stars.<br />

Neutron stars are typically a bit more massive than our<br />

sun, yet their radius is only that of a small city (6 miles)<br />

and they rotate so rapidly that a neutron star day can<br />

last less than a second. Neutron stars represent the most<br />

compact state of matter - a tablespoon full of neutron<br />

star matter weighs 500 million tons. At such extreme densities,<br />

the decay of isotopes that are extremely unstable<br />

on Earth is blocked. These isotopes therefore form layers<br />

in the neutron star crust and need to be understood to<br />

explain observations.<br />

Our group is mainly concerned with recreating the unstable<br />

isotopes made in stellar explosions and neutron<br />

stars in the laboratory. Little is known so far about these<br />

nuclei because of the extreme difficulty of producing<br />

them. This has hampered the explanation of many recent<br />

observations of X-ray burst and nova explosions,<br />

and is one of the issues that prevents us from answering<br />

the question of the origin of the heavy elements in<br />

nature. At <strong>NSCL</strong> we are now able to produce many of<br />

the important unstable isotopes and study their often<br />

surprising properties for the first time. We are involved<br />

in a variety of experiments ranging from mass measurements<br />

and decay studies to the use of reactions.<br />

Consequently, we use a range of devices such as the<br />

neutron detector NERO, <strong>NSCL</strong> Beta Counting System,<br />

the SeGA γ-array, and the S800 spectrometer and work<br />

together with other groups at <strong>NSCL</strong> and elsewhere. The<br />

new <strong>NSCL</strong> low energy facility expected to be operational<br />

in 2009-2010 will also offer unique new opportunities<br />

for nuclear<br />

astrophysics<br />

experiments.<br />

At the same<br />

time, we are<br />

also involved<br />

in theoretical<br />

astrophysics<br />

calculations.<br />

Some of the<br />

calculations<br />

Artists view of a neutron star that<br />

accretes matter from a companion.<br />

are done in our group, and others with collaborations<br />

through JINA.<br />

<strong>NSCL</strong><br />

www.nscl.msu.edu<br />

27


Brad Sherrill<br />

University Distinguished Professor and<br />

Associate Director for Research<br />

Experimental Nuclear Physics<br />

Selected Publications<br />

Discovery of 40 Mg and 42 Al suggests neutron drip-line<br />

slant towards heavier isotopes, T. Baumann, et al.,<br />

Nature 449, 1022 (2007)<br />

The Physics of a Rare Isotope Accelerator, D. Geesaman,<br />

C.K. Gelbke, R. Janssens, B.M. Sherrill, Ann.<br />

Rev. Nucl. Part. Sci. 56, 53 (2006)<br />

Frontiers of Nuclear Structure: Exotic Nuclei, B.M.<br />

Sherrill and R.F. Casten, Nucl. Phys. News 15(2), 13<br />

(2005)<br />

New Approach for Measuring Properties of rp-Process<br />

Nuclei, R.R.C. Clement et al., Phys. Rev. Lett.<br />

92, 172502 (2004)<br />

Commissioning the A1900 projectile fragment separator,<br />

D.J. Morrissey et al., Nucl. Instrum. Meth.<br />

Phys. Res. B 204, 90 (2003)<br />

B.A., Physics,<br />

Coe College,<br />

1980<br />

M.S., Physics,<br />

Michigan State University,<br />

1982<br />

PhD, Physics,<br />

Michigan State University,<br />

1985<br />

Joined <strong>NSCL</strong><br />

in January 1985<br />

sherrill@nscl.msu.edu<br />

The rise of nanotechnology is garnering much attention<br />

for its ability to construct objects out of individual atoms<br />

and molecules, at a scale roughly a billion times smaller<br />

than the objects we encounter in our everyday lives.<br />

In parallel to nanotechnology’s achievements; my research<br />

is to develop the capacity to construct objects<br />

on an even more minute scale, that of the atomic nucleus<br />

another 100,000 times smaller. It is probably best<br />

to describe this as femtotechnology. One femtometer,<br />

the unit of measurement used to describe the dimensions<br />

of a nucleus, is 10 -15 meters.<br />

Approximately 270 isotopes are found naturally. However,<br />

many more isotopes, nearly 7000 in total, can be<br />

produced by particle accelerators or in nuclear reactors.<br />

These isotopes are radioactive and spontaneously<br />

decay to more stable forms.<br />

times the size of a normal lithium nucleus. The existence<br />

of such nuclei allows researchers to study the interaction<br />

of neutrons in nearly pure neutron matter, similar to<br />

what exists in neutron stars.<br />

The approach that I have helped develop for production<br />

of new isotopes is called in-flight separation; where<br />

a heavy ion, such as a uranium nucleus, is broken up<br />

at high energy. This produces a cocktail beam of fragments<br />

that are filtered by a downstream system of<br />

magnets called a fragment separator. The efficiency<br />

of this technique can be nearly 100% and we are able<br />

to identify a single ion out of 10 15 other particles.<br />

There are several reasons why a latent demand exists<br />

within the scientific community for new, rare isotopes.<br />

One is that the properties of particular isotopes often<br />

hold the key to understanding some aspect of nuclear<br />

science. Another is that the rate of certain nuclear reactions<br />

can be important for modeling astronomical<br />

objects, such as supernovae. And of course, the pursuit<br />

of ever more exotic isotopes sometimes advances<br />

basic understanding in unexpected ways. A recent, remarkable<br />

example was our discovery of 42 Al, whose existence<br />

was thought to be unlikely. The result indicates<br />

that nuclei can bind more neutrons than previously<br />

predicted.<br />

Femtotechnology gives scientists access to designer<br />

nuclei with characteristics that can be adjusted to the<br />

research need. For example, super-heavy isotopes of<br />

light elements, such as lithium, have a size nearly five<br />

The rich variety of nuclei is indicated by the depiction of three<br />

isotopes 4 He, 11 Li, and 220 Ra overlaid on the chart of nuclides<br />

where black squares indicate the combination of neutrons<br />

and protons that result in stable isotopes, yellow those produced<br />

so far, and green those that might exist. Nuclei like 11 Li<br />

have very different characteristics, such as a diffuse surface<br />

of neutron matter, than do normal nuclei.<br />

28 www.nscl.msu.edu<br />

<strong>NSCL</strong>


Krzysztof Starosta<br />

Assistant Professor<br />

Experimental Nuclear Physics<br />

Selected Publications<br />

Z=50 shell gap near 100 Sn from intermediateenergy<br />

Coulomb excitations in even-mass<br />

106-112 Sn isotopes, C. Vaman et al., Phys. Rev.<br />

Lett. 99, 162501 (2007)<br />

M.S., Physics,<br />

Warsaw University,<br />

1992<br />

PhD, Physics,<br />

Warsaw University,<br />

1996<br />

Joined <strong>NSCL</strong><br />

in August 2003<br />

starosta@nscl.msu.edu<br />

Linear polarization sensitivity of SeGA detectors,<br />

D. Miller et al., Nucl. Instr. Meth. A581,<br />

713 (2007)<br />

Clock and trigger synchronization between<br />

several chassis of digital data acquisition<br />

modules, W. Hennig et al., Nucl. Instr. Meth.<br />

B261, 1000 (2007)<br />

Shape and Structure of N=Z 64 Ge: Electromagnetic<br />

Transition Rates from the Application<br />

of the Recoil Distance Method to a<br />

Knockout Reaction, K. Starosta et al., Phys.<br />

Rev. Lett. 99, 042503 (2007)<br />

Effect of γ-Softness on the Stability of Chiral<br />

Geometry: Spectroscopy of 106 Ag, P. Joshi et<br />

al., Phys. Rev. Lett. 98, 102501 (2007)<br />

I am investigating structure of short-lived exotic states<br />

in nuclei far from stability. My experimental program at<br />

<strong>NSCL</strong> concentrates on in-beam studies which explore<br />

nuclear properties through electromagnetic excitations.<br />

The electromagnetic probe provides an excellent<br />

way to study nuclear systems bound by still poorly<br />

known effective nuclear interactions; it is well understood,<br />

and can be treated quantitatively in structure<br />

and reaction models. In particular, the electromagnetic<br />

transition matrix elements are observables that models<br />

can be examined against. These matrix elements can<br />

be obtained from transition rates or lifetimes of nuclear<br />

states.<br />

Many important excited nuclear states that decay by<br />

γ-ray emission with lifetimes in the picosecond range<br />

can be reliably measured using Doppler shift methods.<br />

A significant fraction of my research program at <strong>NSCL</strong><br />

is based on applications of the Recoil Distance Method<br />

(RDM) and Doppler Shift Attenuation Method (DSAM)<br />

which I have developed for fast beams from fragmentation<br />

reactions. In an RDM experiment the beam ions<br />

are excited on a movable target, emerge from the target<br />

and decay in flight after a distance related to the<br />

lifetime. A stationary degrader positioned downstream<br />

with respect to the target is used to further reduce the<br />

velocity of the excited nuclei. The resulting γ-ray spectra<br />

exhibit two peaks; one with a larger Doppler shift<br />

that corresponds to the gamma-rays emitted before<br />

traversing the degrader, and one with a smaller Doppler<br />

shift that corresponds to γ-rays emitted after the<br />

degrader. From the relative intensity of the peak areas<br />

as a function of target-degrader distance, the lifetime<br />

of the state can be inferred. The RDM was first applied at<br />

<strong>NSCL</strong> in experiments with the Segmented Germanium<br />

Array (SeGA), in measurements of the lifetimes of the<br />

<strong>NSCL</strong><br />

first excited state in 64 Ge (produced by a single neutron<br />

knock-out reaction from 65 Ge) and in 114 Pd (populated<br />

by intermediate-energy Coulomb excitation).<br />

The scientific reach of the RDM and DSAM methods<br />

will be greatly enhanced by applications of the digital<br />

signal processing to γ-ray spectroscopy. I am currently<br />

leading a project to develop a fully digital, state-ofthe-art,<br />

600-channel Digital Data Acquisition System<br />

(DDAS) for the SeGA array; one of the largest array of<br />

segmented detectors available for use with rare ion<br />

beams. The DDAS will have γ-ray tracking capability<br />

and will allow determination of the first interaction position<br />

of a γ-ray in a SeGA detector with a precision by<br />

a factor of two better than currently available. This will<br />

translate into significantly improved energy resolution<br />

from more precise Doppler correction, or increased<br />

efficiency available with more compact SeGA geometries.<br />

Lifetimes below 1 ps are expected to be accessible<br />

in digital SeGA experiments. Such RDM and DSAM<br />

studies of the products from fragmentation reactions<br />

have the promise of reaching far from stability and providing<br />

lifetime information for intermediate-spin excited<br />

states in a wide range of nuclei.<br />

Target Degrader<br />

Variable distance<br />

Counts Counts Counts<br />

Energy<br />

www.nscl.msu.edu<br />

Schematic arrangement<br />

of the excitation<br />

target (gray)<br />

and the degrader<br />

(red) in a RDM<br />

lifetime measurement<br />

with a short<br />

(top), intermediate<br />

(middle), and a<br />

long (bottom) flight<br />

path.<br />

29


Andreas Stolz<br />

Assistant Professor and<br />

Deputy Department Head - Operations<br />

Experimental Nuclear Physics<br />

Selected Publications<br />

New isotope 44 Si and systematics of the production<br />

cross sections of the most neutronrich<br />

nuclei, O. B. Tarasov et al., Phys. Rev. C<br />

75, 064613 (2007)<br />

Two-proton correlations in the decay of 45 Fe,<br />

K. Miernik et al., Phys. Rev. Lett. 99, 192501<br />

(2007)<br />

Discovery of 40 Mg and 42 Al suggests neutron<br />

drip-line slant towards heavier isotopes, T.<br />

Baumann et al., Nature 449, 1022 (2007)<br />

Heteroepitaxial diamond detectors for<br />

heavy ion beam tracking, A. Stolz et al., Diamond<br />

and Related Materials 15, 807 (2006)<br />

First observation of 60 Ge and 64 Se, A. Stolz et<br />

al., Phys. Lett. B 627, 32 (2005)<br />

M.S., Physics,<br />

Technological<br />

University of Munich<br />

1995<br />

PhD, Physics,<br />

Technological<br />

University of Munich,<br />

2001<br />

Joined <strong>NSCL</strong><br />

in June 2001<br />

stolz@nscl.msu.edu<br />

My primary research interest is centered on the production<br />

of rare isotope beams with fragment separators<br />

and the study of the structure of nuclei at the<br />

limits of existence. At <strong>NSCL</strong>, rare isotope beams are<br />

produced by projectile fragmentation. The coupled<br />

cyclotrons accelerate stable ions to a velocity up to<br />

half the speed of light. The fast ions then impinge on a<br />

production target where they break up into fragments<br />

of different mass and charges. Most of the fragments<br />

are unstable and many of them have an unusual ratio<br />

of protons and neutrons. To study their properties,<br />

the fragments of interest need to be separated from<br />

all other produced particles. The A1900 fragment separator<br />

at <strong>NSCL</strong> filters rare isotopes by their magnetic<br />

properties and their energy loss in thin metal foils. Detector<br />

systems installed in the path of the beam allow<br />

the unambiguous identification of every single isotope<br />

transmitted through the device. The large acceptance<br />

of the separator together with intense primary beams<br />

from the cyclotrons allow access to the most exotic nuclei<br />

that exist, some of which were observed for the first<br />

time at <strong>NSCL</strong>. The investigation of the limits of nuclear<br />

stability provides a key benchmark for nuclear models<br />

and is fundamental to the understanding of the nuclear<br />

forces and structure.<br />

Another research area is the development of particle<br />

detectors made from diamond produced by chemical<br />

vapor deposition in collaboration with the Department<br />

of Physics and Astronomy at MSU. Radioactive<br />

beam facilities of the newest generation can produce<br />

rare isotope beams with very high intensities. The special<br />

properties of diamond allow the development of<br />

radiation-hard timing and tracking detectors that can<br />

be used at incident particle rates up to 10 8 particles per<br />

second. Detectors based on poly-crystalline diamond<br />

were built and tested at <strong>NSCL</strong> and excellent timing<br />

properties were achieved. Those detectors have been<br />

successfully used as timing detectors in several <strong>NSCL</strong> experiments<br />

by now. First detectors based on MSU-grown<br />

single-crystal diamond showed superior efficiency and<br />

energy resolution. Further development will continue<br />

with the investigation of electronic properties of singlecrystal<br />

diamond and the production of detectors with<br />

larger active areas.<br />

energy loss in silicon [GeV]<br />

2.0<br />

1.8<br />

1.6<br />

1.4<br />

no 59 Ga<br />

60 Ge<br />

54 Co<br />

53 Fe<br />

52 Mn<br />

1.2<br />

200 210 220 230 240 250<br />

time of flight through separator [ns]<br />

Particle identification plot showing the energy loss in a silicon<br />

detector as a function of time-of-flight through the A1900<br />

fragment separator. The separator tune was optimized for<br />

60 Ge, a rare isotope observed for the first time at <strong>NSCL</strong>.<br />

10 4<br />

10 3<br />

10 2<br />

10<br />

1<br />

30 www.nscl.msu.edu<br />

<strong>NSCL</strong>


Michael Thoennessen<br />

Professor and Associate Director<br />

for Education<br />

Experimental Nuclear Physics<br />

Selected Publications<br />

M.S., Physics,<br />

University of Cologne,<br />

1985<br />

PhD, Physics,<br />

SUNY Stony Brook,<br />

1988<br />

Joined <strong>NSCL</strong><br />

in November 1990<br />

thoennessen@nscl.msu.edu<br />

Discovery of exotic nuclides 40 Mg and<br />

42 Al suggests neutron dripline slant towards<br />

heavier isotopes, T. Baumann et<br />

al., Nature 449, 1022 (2007)<br />

Selective Population and Neutron Decay<br />

of the First Excited State of Semimagic<br />

23 O, A. Schiller et al., Phys. Rev.<br />

Lett. 99, 112501 (2007)<br />

First Observation of 60 Ge and 64 Se, A.<br />

Stolz et al., Phys. Lett. B 627, 32 (2005)<br />

Construction of a Modular Large-Area<br />

Neutron Detector for the <strong>NSCL</strong>, T. Baumann<br />

et al., Nucl. Instr. Methods A543,<br />

517 (2005)<br />

Reaching the Limits of Nuclear Stability,<br />

M. Thoennessen, Rep. Prog. Phys. 67,<br />

1187 (2004)<br />

Vertical (cm)<br />

50<br />

0<br />

-50<br />

-100<br />

<strong>NSCL</strong><br />

-50 0 50 100<br />

Horizontal (cm)<br />

Intensity<br />

Neutron hits distributed over the front face of MoNA. The<br />

intense distribution in the center is due to neutrons emitted<br />

from the decay of the neutron unbound nucleus.<br />

70<br />

60<br />

50<br />

40<br />

30<br />

20<br />

10<br />

0<br />

My research begins where the nuclear chart ends. While<br />

normal neutron-rich nuclei decay by converting a neutron<br />

into a proton (β decay) on a time scale of milliseconds<br />

or longer, nuclei beyond the end of the nuclear<br />

chart, or neutron-unbound nuclei, contain so many<br />

neutrons that they decay by emitting one or two of the<br />

excess neutrons on a time scale of 10 -21 s. I am part of<br />

the MoNA/Sweeper collaborations which specialize in<br />

the study of these neutron-unbound nuclei. The masses<br />

and lifetimes of these extremely shortlived nuclei cannot<br />

be measured with standard techniques. The availability<br />

of fast radioactive ion beams at <strong>NSCL</strong> gives us<br />

the opportunity to create neutron-unbound nuclei and<br />

study them by detecting their decay products. For example<br />

25 O, the first neutron-unbound oxygen nucleus,<br />

was recently studied by our group. A primary beam of<br />

48 Ca was accelerated to about 50% of the speed of<br />

light with the Coupled Cyclotron Facility and a secondary<br />

beam of 26 F was selected by the A1900 fragment<br />

separator. The 26 F interacted with a target where we<br />

were specifically interested in the one-proton stripping<br />

reaction which leads to 25 O. Instantaneously, 25 O then<br />

decays in the target into 24 O and a neutron. Due to<br />

the large incoming energy from both, 24 O and the neutron<br />

will leave the target essentially at beam velocity.<br />

Following the target are two devices which were specifically<br />

designed for these studies. The 4 Tesla superconducting<br />

“Sweeper” magnet deflects the charged<br />

decay fragment into a set of particle detectors that<br />

identify the 24 O fragments and measure their energies<br />

and angles. The Sweeper magnet was built at the <strong>National</strong><br />

High Magnetic Field Laboratory at Florida State<br />

University in collaboration with <strong>NSCL</strong>.<br />

The second device is MoNA, the Modular Neutron Array.<br />

It is a highly efficient large area neutron detector<br />

which measures the energy and angle of the emitted<br />

neutrons. It was constructed by a collaboration of primarily<br />

undergraduate institutions, and undergraduates<br />

continue to participate in the experiments and data<br />

analysis. From the energies and angles of the fragments<br />

and neutrons, it is possible to reconstruct the<br />

mass of the neutron-unbound nuclei. 25 O is only one<br />

example of the many neutron-unbound nuclei at the<br />

limit of nuclear existence, and our experiment was the<br />

first to identify this exotic nucleus. With the exception<br />

of the lightest elements (up to boron – and now 25 O),<br />

none of these nuclei have been explored. The combination<br />

of MoNA and the Sweeper with the fast radioactive<br />

beams is one of the few facilities in the world<br />

where these nuclei can be explored. In addition to the<br />

measurement of neutron-unbound nuclei, the setup is<br />

also ideal to search for more exotic decay modes for<br />

example di-neutron emission.<br />

www.nscl.msu.edu<br />

31


Betty Tsang<br />

Professor<br />

Nuclear Chemistry<br />

Selected Publications<br />

Fragmentation cross sections and binding<br />

energies of neutron-rich nuclei, M.B. Tsang<br />

et al., Phys. Rev. C 76, 041302 (2007)<br />

Survey of ground State neutron Spectroscopic<br />

Factors from Li to Cr isotopes, M.B.<br />

Tsang, J. Lee, W.G. Lynch, Phys. Rev. Lett.<br />

95, 222501 (2005)<br />

The Thermodynamic Model for Nuclear<br />

Multifragmentation, C.B. Das, S. Das Gupta,<br />

W.G. Lynch, A.Z. Mekjian and M.B. Tsang,<br />

Phys. Rep. 406, 1 (2005)<br />

Isospin Diffusion in Heavy Ion Reactions,<br />

M.B. Tsang et al., Phys. Rev. Lett. 92, 062701<br />

(2004)<br />

Isotope Scaling in Nuclear Reactions, M.B.<br />

Tsang, W.A. Friedman, C.K. Gelbke, W.G.<br />

Lynch, G. Verde, H. Xu, Phys. Rev. Lett. 86,<br />

5023 (2001)<br />

B.S., Mathematics,<br />

California State College,<br />

1973<br />

M.S., Chemistry,<br />

University of Washington,<br />

1978<br />

PhD, Chemistry,<br />

University of Washington,<br />

1980<br />

Joined <strong>NSCL</strong><br />

in December 1980<br />

tsang@nscl.msu.edu<br />

As an experimentalist, I study collisions of nuclei at energies<br />

at approximately half the speed of light. From the<br />

collisions of nuclei, we can create environments, which<br />

resemble the first moments of the universe after the big<br />

bang. Properties of extra terrestrial objects such as neutron<br />

stars can be obtained from studying collisions of a<br />

variety of nuclei with different compositions of protons<br />

and neutrons. One important research area of current<br />

interest is the density dependence of the symmetry energy,<br />

which governs the stability as well as other properties<br />

of neutron stars. Symmetry energy also determines<br />

the degree of stability in nuclei. We have an active program<br />

to study the symmetry energy term in the nuclear<br />

equation of state. In one experiment, which measured<br />

the isotope yields from the collisions of different tin isotopes,<br />

112 Sn+ 112 Sn (light tin systems), 124 Sn+ 124 Sn (heavy<br />

tin systems with more neutrons), we discovered that<br />

the ratios of the yields of specific isotopes between two<br />

different tin systems follow a nice systematic. The yield<br />

ratios depend exponentially on the neutron number N<br />

and proton number Z of the specific isotopes as shown<br />

in the figure. This phenomenon is coined “isoscaling”<br />

and has been observed in various types of reactions.<br />

Through model simulations, we have related the slopes<br />

of the lines to the symmetry energy. Experiments are<br />

planned at <strong>NSCL</strong>, as well as RIKEN, Japan, to further understand<br />

the symmetry energy observables at different<br />

nuclear densities created in nuclear collisions. Transport<br />

simulations of nuclear collisions carried out at the high<br />

performance computing center at MSU also help us in<br />

our quest to understand the role of symmetry energy in<br />

nuclear collisions, nuclear structure and neutron stars.<br />

By studying particles emitted in nuclear collisions, we<br />

also gain knowledge about the structure of nuclei. Sin-<br />

32<br />

www.nscl.msu.edu<br />

gle nucleon transfer reactions, when either a proton or<br />

neutron is transferred from the projectile to the target<br />

or vice versa, have been used successfully in the study<br />

of nuclear structure. This type of reaction is especially<br />

useful in understanding the single particle states in a<br />

nucleus. Accurate descriptions of single particle states<br />

are of fundamental importance to check the validity<br />

of the nuclear shell models. Shell models that can<br />

predict properties of exotic nuclei are relevant in our<br />

understanding of nucleosynthesis of elements when<br />

the early universe was formed. Our group has an active<br />

experimental program in transfer reactions using a<br />

state of the art high resolution detector array (HiRA).<br />

Experiments are being planned for using radioactive<br />

beams at <strong>NSCL</strong> as well as with re-accelerated rare isotope<br />

beams.<br />

Yield ratios of fragments<br />

produced<br />

in the central collisions<br />

of heavy<br />

( 124 Sn+ 124 Sn) and<br />

light ( 112 Sn+ 112 Sn)<br />

tin isotopes plotted<br />

as a function<br />

of the neutron<br />

number N, (top<br />

panel) and proton<br />

number Z, (bottom<br />

panel) of the fragments.<br />

The lines<br />

are best fits with<br />

exponential functions<br />

on N and Z.<br />

Isotopes of the<br />

same elements use same symbols. Z=1 indicate hydrogen isotopes<br />

and Z=8 indicate oxygen isotopes.<br />

<strong>NSCL</strong>


John Vincent<br />

Professor, Chief Engineer and<br />

Head, Elect Dept<br />

Accelerator Physics & Engineering<br />

Selected Publications<br />

M.S., Electrical<br />

Engineering,<br />

Michigan State University,<br />

1993<br />

PhD, Electrical<br />

Engineering,<br />

Michigan State University,<br />

1996<br />

Joined <strong>NSCL</strong><br />

in July 1983<br />

vincent@nscl.msu.edu<br />

Status Report on the <strong>NSCL</strong> RF Fragment<br />

Separator, M. Doleans et al., Proc. Part. Accel.<br />

Conf. PAC07, 3585 (2007)<br />

Design, Construction and Commissioning<br />

of the SUSI ECR, P.A. Zavodszky et al., Proc.<br />

Part. Accel. Conf. PAC07, 3766 (2007)<br />

Adaptive Feedforward Cancellation of Sinusoidal<br />

Disturbances in <strong>Superconducting</strong><br />

RF Cavities, T.H. Kandil et al., Nucl. Instrum.<br />

Meth. Phys. Res. A 550, 514 (2005)<br />

Inexpensive RF Modeling and Analysis Techniques<br />

as Applied to Cyclotrons, J. Vincent,<br />

Proc. 16 th Int. Conf. Cyclotrons and their<br />

Applications 2001, p. 293 (2001)<br />

Medical Accelerator Projects at Michigan<br />

State University, H. Blosser et al., Proc. 1989<br />

IEEE Part. Accel. Conf. PAC89, 742 (1989)<br />

My research interests are in RF electronics and resonant<br />

structures, power electronics, systems engineering, and<br />

controls.<br />

Accelerators<br />

I led the effort for the design and construction of the<br />

modern RF systems for the two superconducting cyclotrons<br />

(K500 and K1200) used for nuclear physics research<br />

at <strong>NSCL</strong>, as well as a neutron cancer therapy<br />

cyclotron used in a Detroit hospital. I have also consulted<br />

on two proton cancer therapy machines in Europe,<br />

as well as a new state-of-the-art proton therapy<br />

machine currently being developed in the US. Recently<br />

I have been involved in the design & development of<br />

advanced RF controls for superconducting RF cavities.<br />

supplies are typically single polarity supplies that can<br />

only source energy (single quadrant) and regulate to<br />

about 1 part in 1000. Accelerator laboratories, on the<br />

other hand, typically require bipolar supplies that can<br />

both source and sink energy (4 quadrant) and regulate<br />

to at least 1:10,000. As another example, 12-bit<br />

resolution is considered high quality in industrial control<br />

and embedded systems, whereas accelerator systems<br />

typically require at least 16-bit resolution. My group<br />

has developed highly sophisticated instrumentation, 4<br />

quadrant power supplies, and MIMO control algorithms<br />

and continue to improve and innovate in these areas.<br />

We also develop sophisticated software interfaces to<br />

the laboratory systems and are currently engaged in<br />

developing console software that is agile and crossplatform<br />

(Windows, Linux, OS X).<br />

Rf systems<br />

My interests include the design and development of<br />

charged particle accelerator RF resonators, RF power<br />

amplifiers from 100s of Watts to 100s of KWs, as well as<br />

sophisticated RF controls, modulation electronics, and<br />

associated algorithms in the frequency range up to 1<br />

GHz. As an example, continuing collaborative efforts<br />

with the MSU College of Engineering have yielded advanced<br />

innovative control algorithms and associated<br />

electronics applied to the control of superconducting<br />

RF cavities.<br />

Power Supplies, Controls, and Instrumentation<br />

Accelerators push the limits of stability and accuracy<br />

for power supplies, instrumentation and controls. For<br />

example, high quality industrial programmable power<br />

<strong>NSCL</strong><br />

RF Separator Control Station showing custom electronic modules<br />

and software interfaces.<br />

www.nscl.msu.edu<br />

33


Thomas Wangler<br />

Professor<br />

Accelerator Physics & Engineering<br />

Selected Publications<br />

Beam Halo in Mismatched Proton Beams.<br />

T.P. Wangler et al., Nucl. Instrum. Meth. Phys.<br />

Res. A 519, 425 (2004)<br />

RF Linear Accelerators, T.P. Wangler, Wiley-<br />

VCH Verlag GmbH & Co. KG, Weinheim,<br />

Germany, (2004)<br />

Beam Halo Measurements in High Current<br />

Proton Beams. C.K. Allen et al., Phys. Rev.<br />

Lett. 89, 214802 (2002)<br />

Design of a Proton <strong>Superconducting</strong> Linac<br />

for a Neutron Spallation Source. T.P. Wangler<br />

et al., Proc. 9 th Workshop on RF Superconductivity<br />

1999 Report LA-13782-C, p. 336<br />

(2000)<br />

Particle-Core Model for Transverse Dynamics<br />

of Beam Halo, T.P. Wangler, K.R.Crandall,<br />

R.Ryne, and T.S.Wang, Phys. Rev. ST-AB 1,<br />

084201 (1998)<br />

B.S., Physics,<br />

Michigan State University,<br />

1958<br />

PhD, Physics,<br />

University of Wisconsin,<br />

1964<br />

Joined <strong>NSCL</strong><br />

in August 2007<br />

wangler@nscl.msu.edu<br />

My main focus is on the physics and design of ion linear<br />

accelerators and particularly on the physics of<br />

high-current and high-brightness ion linacs. I began my<br />

career as an experimental high-energy physicist, and<br />

switched to the accelerator field after reading about E.<br />

O. Lawrence, from which I<br />

realized that there was a lot<br />

of challenging and exciting<br />

physics to be understood in<br />

the accelerator field.<br />

The thrust of much of today’s<br />

beam-physics research<br />

is in the area of high<br />

beam brightness, including<br />

brightness limitations and<br />

methods to increase the<br />

brightness. This requires understanding<br />

and control<br />

of unwanted emittance<br />

growth, where emittance is<br />

the phase-space area occupied<br />

by the beam. Another<br />

important research<br />

area is to understand and<br />

control beam losses in intense<br />

beams.<br />

I have worked in the accelerator<br />

field for more than 30<br />

years, conducting beam-physics research associated<br />

with large and small accelerator projects. I developed<br />

design methods for high-current radio frequency quadrupole<br />

(RFQ) linacs, and proton-linac designs for normal-conducting<br />

and superconducting linacs.<br />

The measured points are taken from an experiment at Los<br />

Alamos showing the rms-emittance growth versus the<br />

strength of the beam mismatch in a high current proton<br />

beam. The curves show the prediction based on a spacecharge<br />

free-energy model. The agreement between the<br />

data points and the curves is excellent.<br />

I have carried out<br />

theoretical research<br />

on emittance growth<br />

in space-chargedominated<br />

beams,<br />

studying the relationship<br />

between spacecharge<br />

field energy<br />

and emittance<br />

growth. Working with<br />

a team of accelerator<br />

physicists and engineers,<br />

I carried out<br />

experimental and<br />

theoretical research<br />

on beam-halo formation<br />

and beam<br />

losses in high-current<br />

mismatched proton<br />

beams. An example<br />

of some of the highcurrent<br />

beam research<br />

is shown in the<br />

figure included.<br />

34 www.nscl.msu.edu<br />

<strong>NSCL</strong>


Gary Westfall<br />

University Distinguished Professor<br />

Experimental Nuclear Physics<br />

Selected Publications<br />

Incident Energy Dependence of Correlations<br />

at Relativistic Energies, STAR Collaboration,<br />

Phys. Rev. C 72, 044902 (2005)<br />

B.S., Physics,<br />

University of Texas,<br />

Arlington,<br />

1972<br />

PhD, Physics,<br />

University of Texas,<br />

Austin,<br />

1975<br />

Joined <strong>NSCL</strong><br />

in September 1981<br />

westfall@nscl.msu.edu<br />

Experimental and Theoretical Challenges in<br />

the Search for the Quark Gluon Plasma: The<br />

STAR Collaboration’s Critical Assessment of<br />

the Evidence from RHIC Collisions, STAR Collaboration,<br />

Nucl. Phys. A757, 102 (2005)<br />

Fluctuations and Correlations in STAR, G.D.<br />

Westfall, J. Phys. G: Nucl. Part. Phys. 30,<br />

S1389 (2004)<br />

Narrowing of the Balance Function with<br />

Centrality in Au+Au Collisions at = 130 GeV,<br />

STAR Collaboration, Phys. Rev. Lett. 90,<br />

172301 (2003)<br />

Isolation of the Nuclear Compressibility with<br />

the Balance Energy, D. J. Magestro, W.<br />

Bauer, and G. D. Westfall, Phys. Rev. C 62,<br />

041603R (2000)<br />

My research focuses on studying the quark-gluon liquid<br />

at the Relativistic Heavy Ion Collider (RHIC) at<br />

Brookhaven <strong>National</strong> Laboratory using the STAR detector.<br />

At RHIC, we collide gold nuclei at center-of-mass<br />

energies of up to 200 GeV per nucleon pair. At this energy,<br />

the protons and neutrons in the incident nuclei are<br />

transformed into a hot, dense, and strongly interacting<br />

liquid of quarks and gluons. This quark-gluon liquid is a<br />

nearly perfect liquid, which has nearly zero viscosity as<br />

evidenced by the comparison of flow measurements<br />

to hydrodynamic calculations. The universe is thought<br />

to have existed in this form a few microseconds after<br />

the big bang.<br />

The main detector of STAR is its time projection chamber<br />

(TPC). This TPC can produce a full three-dimensional<br />

picture of the collision of two ultrarelativistic nuclei.<br />

A collision of two gold nuclei is shown as measured in<br />

the STAR detector. Each line in the picture corresponds<br />

to a single particle leaving the collision. Several thousand<br />

tracks are observed in this one central collision.<br />

The color of the track represents the ionization density<br />

of the track. By correlating the curvature of the track<br />

and its ionization density, the particles that created the<br />

track can be identified.<br />

The three cornerstones of the observation of the quarkgluon<br />

liquid at RHIC are thermalization, collective flow<br />

and jet suppression. The spectra of particles emitted in<br />

gold-gold collisions can be well described by a blastwave<br />

model incorporating a kinetic temperature and<br />

an expansion velocity. The relative number of various<br />

types of particles can be well described by a thermal<br />

model using a chemical temperature and a chemical<br />

potential. Collective flow manifests itself in terms of azi-<br />

<strong>NSCL</strong><br />

muthal anisotropies. The original anisotropy in the overlap<br />

region of the two colliding nuclei is translated into<br />

momentum correlations in the final state. Central collisions<br />

of gold nuclei also show strong jet suppression.<br />

Jets are created when a quark or a gluon undergoes a<br />

hard scattering with another quark or gluon. These highenergy<br />

quarks or gluons cannot be observed directly,<br />

and the quark or gluon decays into a jet of observable<br />

particles in the direction of the original quark or gluon.<br />

By comparing gold-gold collisions with deuteron-gold<br />

and proton-proton collisions, RHIC experimenters were<br />

able to show that the quark-gluon liquid originates with<br />

the scattering of quark and gluons.<br />

I am also working on the design and construction of a<br />

TPC to carry out studies of the isospin dependence of<br />

the nuclear equation of state at <strong>NSCL</strong>.<br />

www.nscl.msu.edu<br />

A central collision<br />

of two<br />

gold nuclei at<br />

130 GeV per<br />

nucleon pair as<br />

observed in the<br />

STAR detector<br />

at RHIC. The<br />

figure is drawn<br />

looking down<br />

the beam line<br />

of RHIC.<br />

35


Richard York<br />

Professor and Associate Director<br />

for New Initiatives<br />

Accelerator Physics & Engineering<br />

Selected Publications<br />

Beam Dynamics Studies for the Reacceleration<br />

of Low Energy RIBS at the <strong>NSCL</strong>, X. Wu<br />

et al., Proc. Part. Accel. Conf. PAC07, 1769<br />

(2007)<br />

Design Studies of the Reaccelerator RFQ at<br />

<strong>NSCL</strong>, Q. Zhao et al., Proc. Part. Accel. Conf.<br />

PAC07, 1772 (2007)<br />

End-to-end beam dynamics simulation of<br />

the ISF driver LINAC, Q. Zhao et al., Proc.<br />

Part. Accel. Conf. PAC07, 1775 (2007)<br />

Design of Half-Reentrant SRF Cavities for<br />

Heavy Ion Linacs, J. Popielarski et al., Proc.<br />

Part. Accel. Conf. PAC07, 2328 (2007)<br />

An upgrade to the <strong>NSCL</strong> to produce intense<br />

beams of exotic nuclei, R. C. York et al.,<br />

Proc. Lin. Acc. Conf. LINAC06, 103 (2006)<br />

M.S., Physics,<br />

University of Iowa,<br />

1973<br />

PhD, Physics,<br />

University of Iowa,<br />

1976<br />

Joined <strong>NSCL</strong><br />

in March 1993<br />

york@nscl.msu.edu<br />

My primary interests are in the arena of accelerator<br />

physics. Specific areas of interest are: beam dynamics,<br />

particularly in the high intensity regime; accelerator<br />

systems design, particularly rings, both storage and<br />

synchrotron; and linacs.<br />

Particle accelerators have long been essential to scientific<br />

discovery and technological advancement.<br />

Accordingly, research in this area that, for example,<br />

provide increased reach into energy and/or intensity<br />

frontiers can produce long-term benefits for the physical<br />

and life sciences.<br />

Accelerator physics research is interdisciplinary involving<br />

a broad range of arenas including beam physics,<br />

electrodynamics, plasma physics, optics, condensed<br />

matter physics, surface physics, electrical engineering,<br />

mechanical engineering, and materials science. As a<br />

consequence, training in accelerator physics is broadly<br />

applicable to a host of careers in a multitude of academic<br />

and industrial roles.<br />

Experiments using a small (6.6 m circumference) ring<br />

where space charge effects similar to those of megawatt-class<br />

facilities can be explored.<br />

Accelerator Systems Design (examples)<br />

Design optimization of a high-duty factor heavy ion<br />

linac appropriate for energies of several hundred MeV/<br />

nucleon.<br />

Design optimization of an electron storage ring for a<br />

light source.<br />

High power FEL design based upon recovering the<br />

beam energy through utilization of superconducting<br />

radio frequency structures<br />

<strong>NSCL</strong> has for many years had a research program in<br />

accelerator physics. The general research areas are<br />

beam dynamics, especially in the high intensity regime,<br />

and accelerator systems design.<br />

Beam Dynamics (examples)<br />

Computer code development to model space charge<br />

forces in a way that captures the physics but allows<br />

rapid exploration of possible designs.<br />

<strong>Superconducting</strong> Radio Frequency (SRF) accelerating<br />

structures developed at <strong>NSCL</strong>.<br />

36 www.nscl.msu.edu<br />

<strong>NSCL</strong>


Remco Zegers<br />

Assistant Professor<br />

Experimental Nuclear Physics<br />

M.S., Technical Physics,<br />

State University of<br />

Groningen,<br />

1995<br />

PhD, Mathematics and<br />

Natural Sciences,<br />

State University of<br />

Groningen,<br />

1999<br />

Joined <strong>NSCL</strong><br />

in February 2003<br />

zegers@nscl.msu.edu<br />

Selected Publications<br />

On the extraction of weak transition<br />

strengths via the ( 3 He,t) reaction at 420<br />

MeV, R.G.T Zegers et al., Phys. Rev. Lett. 99,<br />

202501 (2007)<br />

The (t, 3 He) and ( 3 He,t) reactions as probes<br />

of Gamow-teller Strength, R.G.T. Zegers et<br />

al., Phys. Rev. C 74, 024309 (2006)<br />

Measurement of the Gamow-Teller Strength<br />

Distribution in 58 Co via the 58 Ni(t, 3 He) reaction<br />

at 115 MeV/nucleon, A.L. Cole et al.,<br />

Phys. Rev. C 74, 034333 (2006)<br />

Development of a secondary triton beam<br />

for (t, 3 He) experiments at intermediate energies<br />

from primary 16, 18 O beams, G.W. Hitt<br />

et al., Nucl. Instr. Meth. A 566, 264 (2006)<br />

Excitation and Decay of the Isovector Giant<br />

Monopole Resonances via the 208 Pb( 3 He,tp)<br />

Reaction at 410 MeV, R.G.T. Zegers et al.,<br />

Phys. Rev. Lett. 90, 202501 (2003)<br />

My research is focused on nuclear charge-exchange<br />

reactions. In such reactions, a proton in a target nucleus<br />

is exchanged for a neutron in the projectile nucleus,<br />

or vice-versa, thereby transferring charge between the<br />

target and the projectile. Although such reactions are<br />

governed by the strong nuclear force, they are closely<br />

connected to electron-capture and β-decay, which<br />

are transitions governed by the weak nuclear force.<br />

Since those weak transitions play an important role in a<br />

number of astrophysical phenomena, such as supernova<br />

explosions, the study of charge-exchange reactions<br />

is an important element in better understanding the<br />

mechanisms that drive such events. Charge-exchange<br />

reactions are also very useful for probing specific properties<br />

of nuclei, especially those related to spin and<br />

isospin and are, therefore, used to improve and test<br />

our understanding of nuclear structure. The information<br />

obtained from such experiments is, for example, important<br />

for describing the process of neutrinoless double<br />

β decay, which provides insight into fundamental descriptions<br />

of how particles interact.<br />

We use a variety of projectiles to perform chargeexchange<br />

reactions. To study stable nuclei, we use a<br />

reaction in which a hydrogen-3 particle (consisting of<br />

2 neutrons and 1 proton) exchanges a neutron for a<br />

proton in a target nucleus, thus becoming a helium-3<br />

particle (2 protons and 1 neutron). Since the hydrogen-3<br />

particles are not stable, they are produced by<br />

impinging a beam of oxygen particles, accelerated in<br />

the Coupled Cyclotron Facility at <strong>NSCL</strong>, on a thick production<br />

target. The A1900 fragment separator is then<br />

used to purify the hydrogen-3 beam before it interacts<br />

with the target. The helium-3 particles are detected in<br />

the S800 magnetic spectrometer.<br />

<strong>NSCL</strong><br />

My group is also leading efforts to study charge-exchange<br />

reactions on unstable nuclei. Although such nuclei<br />

only exist for a short amount of time, they can play<br />

an important role in stellar environments where temperatures<br />

and densities are high. To study charge-exchange<br />

reactions on unstable nuclei, new experimental<br />

techniques and detectors have to be developed.<br />

At present, we focus on the (Lithium-7, Beryllium-7) and<br />

(proton, neutron) charge-exchange reactions for such<br />

studies.<br />

The charge-exchange group also performs experiments<br />

at other facilities, in particular the Research Center for<br />

Nuclear Physics in Osaka, Japan. There, we investigate<br />

the (Helium-3, Hydrogen-3) charge-exchange reaction,<br />

which is just the inverse of the (Hydrogen-3, Helium-3)<br />

reaction that we study at <strong>NSCL</strong>. An important<br />

motivation for the experiments at RCNP is to better understand<br />

the charge-exchange reaction mechanism.<br />

Results from an experiment<br />

in which<br />

the (Hydrogen-3, Helium-3)<br />

reaction was<br />

studied on a target of<br />

Nickel-58. In the top<br />

two figures, the experimental<br />

(Gamow-<br />

Teller) transition<br />

strengths as a function<br />

of the transferred<br />

(excitation) energy to<br />

the Nickel-58 nucleus<br />

are compared with<br />

different theoretical<br />

models. The experimental<br />

and theoretical<br />

strengths are used to calculate electron-capture rates in massive<br />

stars just before they turn supernova in the bottom figure.<br />

www.nscl.msu.edu<br />

37


Vladimir Zelevinsky<br />

Professor<br />

Theoretical Nuclear Physics<br />

Selected Publications<br />

Tunneling of a composite particle: Effects<br />

of intrinsic structure, C.A. Bertulani, V.V.<br />

Flambaum and V.G. Zelevinsky, J. Phys. G<br />

34, 2289 (2007)<br />

Continuum Shell Model, A. Volya and V.<br />

Zelevinsky, Phys. Rev. C 74, 064314 (2006)<br />

Nuclear structure, random interactions<br />

and mesoscopic physics, V. Zelevinsky<br />

and A. Volya, Phys. Rep. 391, 311 (2004)<br />

The nuclear shell model as a testing<br />

ground for many-body quantum chaos,<br />

V. Zelevinsky, B.A. Brown, N. Frazier, and M.<br />

Horoi, Phys. Rep. 276, 85 (1996)<br />

Quantum chaos and complexity in nuclei,<br />

V. Zelevinsky, Ann. Rev. Nucl. Part. Sci. 46,<br />

237 (1996)<br />

M.S., Physics,<br />

Moscow University,<br />

1960<br />

PhD, Physics,<br />

(Budker) Institute of<br />

Nuclear Physics,<br />

1963<br />

Joined <strong>NSCL</strong><br />

in June 1993<br />

zelevinsky@nscl.msu.edu<br />

My current interest is concentrated on mesoscopic aspects<br />

of nuclear physics. The mesoscopic world is intermediate<br />

between elementary particles and macroscopic<br />

bodies. Mesoscopic systems consist of a relatively<br />

small number of particles which still show up noticeable<br />

properties of matter. On the other hand, such systems<br />

are small enough so that we can study, in theory and in<br />

experiments, individual quantum states. Nuclei provide<br />

one of the best examples of such arrangement and<br />

self-organization. Other mesoscopic systems are complex<br />

atoms, molecules (including biological ones), solid<br />

state nano-devices and future quantum computers. In<br />

all cases, we have certain symmetry, particles, their individual<br />

motion in a common field, their interactions,<br />

collective excitations (waves, vortices, rotation), coexistence<br />

of regularity, complexity and chaos, response<br />

to external forces and possible decay.<br />

wire, quantum computer). Our experience in nuclear<br />

physics helps in understanding a more broad class of<br />

problems.<br />

Another important theoretical topic is related to symmetries<br />

and phase transitions. We still do not have a reliable<br />

theory of nuclear shapes and their transformations<br />

along the nuclear chart or as a function of excitation<br />

energy. The problem is that in mesoscopic systems frequently<br />

the shape is not sharply fixed as, for example,<br />

in perfect crystals, but many nuclei are soft and reveal<br />

large shape fluctuations. On the other hand, there are<br />

reasons to believe that soft modes can enhance some<br />

unusual phenomena, such as violation of fundamental<br />

symmetries (invariance with respect to coordinate inversion<br />

and time reversal). This is a bridge between mesoscopic<br />

physics and physics of elementary particles.<br />

Loosely bound nuclei are of special interest just because<br />

of weak binding. In this situation quantum particles<br />

can live far away from the rest of the system in<br />

a classically forbidden region forming quantum skins,<br />

halos and clusters. Intrinsic structure of such system is<br />

strongly coupled with continuum (or an environment<br />

in the context of condensed matter). It is a challenge<br />

to learn how one can describe in the same consistentframework<br />

intrinsic properties, resonant interaction with<br />

external fields and numerous nuclear reactions which<br />

give the only available tool to study such exotic systems.<br />

Our method of choice is the Continuum Shell<br />

Model that combines on equal footing structure and<br />

reactions. There are still many unsolved problems in this<br />

promising approach. Nuclear reactions have many<br />

common features with the signal transmission through a<br />

mesoscopic solid state device (quantum dot, quantum<br />

For the chain of isotopes from 16 to 28 we have calculated, in the<br />

same approach, bound states, resonances and neutron scattering<br />

cross sections. In red we show unstable states with strong color indicating<br />

shorter lifetimes.<br />

38 www.nscl.msu.edu<br />

<strong>NSCL</strong>


<strong>NSCL</strong><br />

<strong>NSCL</strong> in the News<br />

The experimental results and theoretical interpretations<br />

of <strong>NSCL</strong> results are published in peer<br />

reviewed journals such as Physical Review and<br />

Physical Review Letters, Nuclear Physics A and<br />

Physics Letters B, and the Astrophysical Journal<br />

and Astrophysical Journal Letters.<br />

One of the most recent results was published<br />

in the journal Nature. In the October 25, 2007<br />

issue, <strong>NSCL</strong> researchers described the successful<br />

creation of three never-before-observed<br />

isotopes of magnesium and aluminum.<br />

The results not only stake out new territory on<br />

the nuclear landscape, but also suggest that<br />

variants of everyday elements might exist that<br />

are heavier than current scientific models predict.<br />

“It’s been a longstanding project since the<br />

beginning of nuclear science to establish<br />

what isotopes can exist in nature,” said Dave<br />

Morrissey, University Distinguished Professor<br />

of chemistry and one of the paper’s authors.<br />

“This result suggests that the limit of stability<br />

of matter may be further out than previously<br />

expected; really, it shows how much mystery<br />

remains about atomic nuclei.”<br />

The research was covered by media outlets<br />

around the world, including Science, the Los<br />

Angeles Times and BBC News.<br />

On the left, a picture from the <strong>NSCL</strong> experimenters’<br />

logbook used during the experiment.<br />

The partially visible scrawled note “Let<br />

the celebrations begin!” reflects the researchers’<br />

excitement at the discovery.<br />

Above, a particle identification<br />

plot reveals several of the isotopes<br />

produced in the experiment, including<br />

magnesium-40.<br />

www.nscl.msu.edu<br />

39


<strong>NSCL</strong><br />

Michigan State University<br />

A Brief History<br />

In 1855, the Michigan State Legislature passed<br />

Act 130 which provided for the establishment<br />

of the “Agricultural College of the State of<br />

Michigan,” which came to be known as the<br />

Michigan Agricultural College or “MAC.” MAC<br />

was formally opened and dedicated on May<br />

13, 1857, in what is now East Lansing. MAC was<br />

the first agricultural college in the nation, and<br />

served as the prototype for the 72 land-grant<br />

institutions which were later established under<br />

the Federal Land Grant Act of 1862, unofficially<br />

known as the “Morrill Act” after its chief<br />

sponsor, Senator Justin Morrill of Vermont.<br />

The Campus<br />

The East Lansing campus of MSU is one of the<br />

most beautiful in the nation. Early campus architects<br />

designed it as a natural arboretum<br />

with 7,000 different species of trees, shrubs<br />

and vines represented. The Red Cedar River<br />

bisects the campus; north of the river’s treelined<br />

banks and grassy slopes is the older, traditional<br />

heart of the campus. Some of the existing<br />

ivy-covered red-brick buildings found in<br />

this part of campus were built before the Civil<br />

War. On the south side of the river are the more<br />

recent additions to campus — the medical<br />

complex, the veterinary medical center, and<br />

most of the science and engineering buildings<br />

are included in this area. The<br />

surrounding communities are varied,<br />

and offer rural and “big city”<br />

alternatives.<br />

Events<br />

The arts have flourished at MSU, especially in<br />

the past two decades after our impressive<br />

performing arts facility, the Wharton Center for<br />

Performing Arts, opened in the Fall of 1982. The<br />

Wharton Center’s two large concert halls are<br />

regularly used for recitals, concerts and theater<br />

productions by faculty, student groups,<br />

and visiting and<br />

touring performing<br />

artists. Wharton<br />

Center brings to our<br />

campus dozens of<br />

professional musical<br />

and theatrical<br />

groups each year.<br />

MSU is also home<br />

to the Jack Breslin<br />

<strong>Student</strong> Events<br />

Center, a 15,000+<br />

seat arena which is home to the MSU Spartan<br />

basketball team and also plays host to worldclass<br />

concerts and attractions.<br />

Two facilities that offer both educational<br />

and recreational opportunities are the MSU<br />

Museum and the Kresge Art Center. The Museum<br />

houses documented research collections<br />

in Anthropology, Paleontology, Zoology<br />

and Folklife, as well as regularly hosting traveling<br />

exhibits. The Kresge Art Center contains<br />

studios and classrooms, and an art museum<br />

where both a permanent collection and visiting<br />

exhibitions are on display to the public.<br />

The Kresge Center’s art museum is strongest<br />

in examples of 19 th and 20 th century art, but<br />

also contains a wide variety of other artworks<br />

spanning global history.<br />

40<br />

www.nscl.msu.edu


<strong>NSCL</strong><br />

Michigan State University<br />

Recreation<br />

Many recreational activities are available on<br />

campus and in the Lansing area. Walking and<br />

running trails, available extensively throughout<br />

the campus, take you through protected<br />

natural areas along the Red Cedar River. MSU<br />

has two 18-hole golf courses available to students,<br />

faculty and staff. There are three fitness<br />

centers that provide basketball, handball and<br />

squash courts, exercise machine rooms, and<br />

aerobic workouts. Two indoor ice skating rinks,<br />

an indoor tennis facility, more than thirty outdoor<br />

tennis courts, and five swimming pools<br />

are accessible as well. In both summer and<br />

winter, local state parks such as Rose Lake offer<br />

many outdoor activities. In Michigan, snow<br />

is not a problem, but an activity, so bring your<br />

skis.<br />

MSU, which was<br />

admitted into the<br />

Big Ten in 1948, has<br />

a rich tradition in<br />

athletics. MSU first<br />

competed in conference<br />

football in<br />

1953, sharing the<br />

title that year with<br />

Illinois. Since that<br />

time, MSU has enjoyed<br />

considerable<br />

success in Division I<br />

athletics, including<br />

NCAA titles in basketball and hockey, among<br />

other sports. <strong>Graduate</strong> students, faculty, and<br />

staff at <strong>NSCL</strong> are strong supporters of the athletic<br />

programs, which offer opportunities for<br />

social interactions outside of the laboratory.<br />

Academics<br />

There are approximately 44,000 students on<br />

campus— from every state and 126 foreign<br />

nations. Of these, approximately 9,000 are<br />

in graduate and professional programs. MSU<br />

leads all public universities<br />

in attracting <strong>National</strong><br />

Merit Scholars,<br />

and is also a leader<br />

in the number of students<br />

who win <strong>National</strong><br />

Science Foundation<br />

Fellowships. Michigan<br />

State was the first university<br />

to sponsor <strong>National</strong><br />

Merit Scholarships.<br />

If students are the lifeblood of a campus, then<br />

the faculty is the heart of a great university.<br />

The more than 4,000 MSU faculty continue to<br />

distinguish themselves, and include members<br />

in the <strong>National</strong> Academy of Sciences (two<br />

newly appointed in May, 2003), and honorees<br />

of prestigious fellowships such as the Fullbright,<br />

Guggenheim and Danforth.<br />

University-wide research has led to important<br />

developments throughout MSU’s history. Early<br />

research led to important vegetable hybrids,<br />

and the process for homogenization<br />

of milk. More recently, the<br />

world’s widest-selling and most<br />

effective type of anticancer<br />

drugs (cisplatin<br />

and carboplatin) were<br />

discovered at MSU.<br />

www.nscl.msu.edu<br />

41


<strong>NSCL</strong><br />

The Lansing Area<br />

Capital City<br />

Lansing, Michigan’s capital city, is centrally<br />

located in Michigan’s lower peninsula. The<br />

greater metropolitan area has a population<br />

of approximately 446,000 and is home to several<br />

large industries. The city offers a variety of<br />

restaurants, the Lansing<br />

Symphony Orchestra,<br />

a number of theater<br />

companies, and the<br />

Lansing Lugnuts baseball<br />

team. The Impression<br />

5 Science Museum,<br />

the R.E. Olds Transportation<br />

Museum, and<br />

the Michigan Historical<br />

Museum attract visitors<br />

from throughout the region.<br />

Major local employers include MSU, the<br />

state government, and General Motors. Several<br />

high-tech companies are located in the<br />

area, including the Michigan Biotechnology<br />

Institute, BioPort Corporation and Neogen<br />

Corporation.<br />

There is a large scientific community in the<br />

Lansing area which, along with MSU, is due in<br />

part to the presence of a number of the State<br />

of Michigan research laboratories in the area<br />

including the Department of Agriculture,<br />

the Department of Natural<br />

Resources, the Department<br />

of Public Health Laboratories,<br />

and the Michigan State<br />

Police Crime Laboratories.<br />

In addition to MSU, the Lansing Community<br />

College, the Thomas M. Cooley Law School,<br />

and Davenport College are all located in the<br />

capital city area, and the MSU College of Law<br />

is housed on the MSU campus.<br />

Natural Wonders<br />

Situated in the heart of the Great Lakes region<br />

of the United States, MSU’s East Lansing Campus<br />

is centrally located to not only metropolitan<br />

areas such as Chicago and Detroit, but to<br />

outstanding natural resources and to northern<br />

Michigan’s world-class summer and winter<br />

resorts. Michigan’s Upper Peninsula is an undeveloped<br />

and unspoiled area of immense<br />

natural beauty with a population density of<br />

less than twenty persons per square mile. It offers<br />

many unique “getaway” opportunities for<br />

all seasons. The Lansing area itself provides a<br />

variety of recreational opportunities including<br />

many golf courses, boating and beach life at<br />

Lake Lansing in the summer, and cross-country<br />

skiing in the winter. Hunting and fishing opportunities<br />

are also found widely throughout<br />

the state.<br />

East Lansing<br />

Complementing campus life is the city of East<br />

Lansing, which surrounds the northern edge<br />

of the MSU campus. East Lansing is noted for<br />

its congenial atmosphere and tree-lined avenues.<br />

Shops, restaurants, bookstores, cafés,<br />

malls and places of worship serve the student’s<br />

needs. East Lansing provides students<br />

with a relaxing and stimulating environment<br />

for their graduate school experience.<br />

42<br />

www.nscl.msu.edu


<strong>NSCL</strong><br />

www.nscl.msu.edu<br />

43


44 www.nscl.msu.edu<br />

<strong>NSCL</strong>


<strong>NSCL</strong><br />

Useful Links<br />

<strong>NSCL</strong> Website<br />

<strong>NSCL</strong> Publications<br />

www.nscl.msu.edu<br />

www.nscl.msu.edu/ourlab/publications<br />

The <strong>Graduate</strong> School at Michigan State University<br />

www.grad.msu.edu<br />

<strong>National</strong> Science Foundation<br />

www.nsf.gov<br />

U.S. Department of Energy<br />

www.energy.gov<br />

Department of Chemistry at MSU<br />

www.chemistry.msu.edu<br />

Department of Physics & Astronomy at MSU<br />

www.pa.msu.edu<br />

College of Engineering at MSU<br />

www.egr.msu.edu<br />

Statistical Research Center of the American Institute of Physics<br />

www.aip.org/statistics<br />

Joint Institute for Nuclear Astrophysics (JINA)<br />

www.jinaweb.org<br />

www.nscl.msu.edu<br />

45


<strong>National</strong> <strong>Superconducting</strong> Cyclotron Laboratory<br />

at Michigan State University<br />

Spring 2008<br />

Portions of this brochure were adapted<br />

from the Department of Chemistry<br />

at Michigan State University.<br />

Designed by Jon Whiting


<strong>National</strong> <strong>Superconducting</strong> Cyclotron Laboratory<br />

Michigan State University<br />

1 Cyclotron, East Lansing, Michigan 48824-1321<br />

Phone 517-355-9671<br />

www.nscl.msu.edu<br />

Operation of <strong>NSCL</strong> as a national<br />

user facility is supported by the<br />

Experimental Nuclear Physics Program<br />

of the U.S. <strong>National</strong> Science Foundation.

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