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6 <strong>Atomic</strong> <strong>Physics</strong> <strong>and</strong> <strong>Quantum</strong> <strong>Optics</strong><br />

Wednesday, 15.06.2011, CE 101<br />

Time ID I: Fundamental PhysIcs / matter Waves<br />

Chair: Antoine Weis, Uni Fribourg<br />

14:00 601 Listening to the <strong>Quantum</strong> Drum: Mechanics in its Ground State<br />

Tobias Donner 1, 2, 3 , John Teufel 3 , Konrad Lehnert 2, 3 , Ray Simmonds 3<br />

1 ETH Zürich, CH-8093 Zürich<br />

2 JILA, University of Colorado 80309 Boulder, CO, USAs<br />

3 National Institute of St<strong>and</strong>ards <strong>and</strong> Technology, Boulder, 80305 CO, USA<br />

A mechanical resonator is a physicist’s most tangible example of a harmonic oscillator. If cooled to<br />

sufficiently low temperatures a mechanical oscillator is expected to behave differently to our classical<br />

perception of reality. Observing the quantum behavior of a mechanical oscillator is challenging<br />

because it is difficult both to prepare the oscillator in a pure quantum state of motion <strong>and</strong> to detect<br />

those states. I will present experiments in which we couple the motion of a micro-fabricated oscillator<br />

to the microwave field in a superconducting high-Q resonant circuit. The displacement of the oscillator<br />

imprints a phase modulation on the microwave field which we detect with a nearly shot-noise<br />

limited interferometer. We employ the radiation pressure force of the microwave photons to cool the<br />

mechanical oscillator to its motional ground state. Finally, we increase the parametric coupling <strong>and</strong><br />

the system enters the strong coupling regime.<br />

14:30 602 Entanglement in Neutron Polarimetric Experiments<br />

Stephan Sponar 1 , Jürgen Klepp 2 , Claus Schmitzer 3 , Hannes Bartosik 3 ,<br />

Katharina Durstberger-Rennhofer 1 , Gerald Badurek 1 , Yuji Hasegawa 1<br />

1 Atominstitut, Vienna University of Technology, Stadionallee 2, AT-1020 Vienna<br />

2 Faculty of <strong>Physics</strong>, University of Vienna, Boltzmanngasse 5, AT-1090 Vienna<br />

3 CERN, CH-1211 Genève 23<br />

Entanglement is a remarkable peculiarity in quantum mechanics. Not only space-like separated particles,<br />

but also systems whose observables belong to disjoint Hilbert spaces, are known for occurrence<br />

of entanglement. This is likewise the case in single-neutron systems, where entanglement is<br />

achieved between different degrees of freedom. Due to its high contrast <strong>and</strong> insensitivity to ambient<br />

disturbances, the neutron polarimeter is suitable for studying non-contextual hidden-variable<br />

theories. Two experiments, violation of a Bell-like inequality <strong>and</strong> of an inequality for a triply entangled<br />

Greenberger-Horne-Zeilinger-like state derived by Mermin, are presented. The former yields a<br />

spin-energy correlation function S=2.333(2)>2, which violates the Clauser–Horne–Shimony–Holt Bell<br />

inequality by more than 166 st<strong>and</strong>ard deviations. The latter results in a final value M = 3.936(2)>2, for<br />

an entanglement of spin, total energy <strong>and</strong> momentum degree of freedom, exhibiting a clear violation<br />

of the classical limit. Both experiments verify the predictions of quantum mechanics which are at<br />

variance with non-contextual hidden variable theories.<br />

15:00 603 Leggett's noncontextual model studied with neutrons<br />

Katharina Durstberger-Rennhofer 1 , Claus Schmitzer 2 , Hannes Bartosik 2 , Jürgen Klepp 3 ,<br />

Stephan Sponar 1 , Gerald Badurek 1 , Yuji Hasegawa 1<br />

1 Atominstitut, TU Wien, Stadionallee 2, AT-1020 Wien ; 2 CERN, CH-1211 Genève 23<br />

3 Fakultät für Physik, Universität Wien, Boltzmanngasse 5, AT-1090 Wien<br />

It is a long-lasting debate whether nature can be described by deterministic hidden variable theories<br />

(HVT) underlying quantum mechanics (QM). Bell inequalities for local HVT as well as the Kochen-<br />

Specker theorem for non-contextual models stress the conflict between these alternative theories<br />

<strong>and</strong> QM. Leggett showed that even nonlocal hidden variable models are incompatible with quantum<br />

predictions.<br />

Neutron interferometry <strong>and</strong> polarimetry are very proper tools to analyse the behaviour of singleneutron<br />

systems, where entanglement is created between different degrees of freedom (e.g., spin/<br />

path, spin/energy) <strong>and</strong> thus quantum contextuality can be studied.<br />

We report the first experimental test of a contextual model of quantum mechanics a la Leggett,<br />

which deals with definiteness of measurement results before the measurements. The results show<br />

a discrepancy between our model <strong>and</strong> quantum mechanics of more than 7 st<strong>and</strong>ard deviations <strong>and</strong><br />

confirm quantum indefiniteness under the contextual condition.<br />

119


15:15 604 Matter wave interferometry with cool metal clusters<br />

Philipp Geyer 1 , Philipp Haslinger 1 , Jonas Rodewald 1 , Stefan Nimmrichter 1 , Bernd v. Issendorff 2 ,<br />

Markus Arndt 1<br />

1 Faculty of <strong>Physics</strong>, University of Vienna, Boltzmanngasse 5, AT-1090 Vienna<br />

2 Faculty of <strong>Physics</strong>, University of Freiburg, Stefan-Meier-Str. 21, DE-79104 Freiburg<br />

Matter wave interferometry with clusters <strong>and</strong> molecules is a versatile tool for testing the foundations<br />

of quantum physics <strong>and</strong> for establishing new precision measurements on clusters.<br />

We describe a new instrument to explore de Broglie physics of large clusters. Our all-optical ionizing<br />

Talbot-Lau interferometer in the time domain [1,2] consists of three pulsed UV/VUV lasers which are<br />

all retro-reflected by one <strong>and</strong> the same single mirror to generate three st<strong>and</strong>ing light waves. The<br />

expected advantages of interferometry with optical gratings in the time-domain are the complete<br />

elimination of dispersive effects, the compactness <strong>and</strong> ruggedness as well the absence of clusterwall<br />

interaction that one would find in the presence of material gratings.<br />

[1] Reiger, E., et al., Exploration of gold nanoparticle beams for matter wave interferometry. <strong>Optics</strong>Communications,<br />

2006. 264(2): p. 326-332.<br />

[2] Nimmrichter, S., et al., Concept of a time-domain ionizing matter wave interferometer. arXiv:1102.3644v1 2011.<br />

15:30<br />

16:00 Coffee Break<br />

II: cold atoms / molecules<br />

Chair: Jean-Luc Robyr, Uni Fribourg<br />

16:30 611 Optomechanical Coupling of Ultracold Atoms <strong>and</strong> a Membrane Oscillator<br />

Andreas Jöckel 1 , Maria Korppi 1 , Stephan Camerer 2 , David Hunger 2 , Theodor W. Hänsch 2 ,<br />

Philipp Treutlein 1<br />

1 Departement Physik, Universität Basel, Klingelbergstrasse 82, CH-4056 Basel<br />

2 LMU München, Schellingstrasse 4, DE-80799 München<br />

We report the recent results of our experiment, where we couple a single mode of a high-Q membrane-oscillator<br />

to the motion of laser-cooled atoms in an optical lattice. The optical lattice is formed<br />

by retroreflection of a laserbeam from the membrane surface. The coupling is mediated by power<br />

modulation of the lattice beam due to the vibrations of the atoms in the lattice. If the trap frequency<br />

of the atoms in the lattice is matched to the eigenfrequency of the membrane, we observe resonant<br />

energy transfer between the two systems.<br />

In the long term, such coupling mechanism could be exploited to develop hybrid quantum systems<br />

between atoms <strong>and</strong> solid-state devices. As another intriguing perspective, a new generation of optical<br />

lattice experiment is in sight, where the mirrors creating the laser st<strong>and</strong>ing waves are micromechanical<br />

oscillators interacting with the atoms on a quantum level.<br />

17:00 612 Spin-Squeezing a Bose-Einstein Condensate on an Atom Chip<br />

Roman Schmied, Max Riedel, Pascal Böhi, Caspar Ockeloen, Philipp Treutlein<br />

Departement Physik, Universität Basel, Klingelbergstrasse 82, CH-4056 Basel<br />

<strong>Quantum</strong> information technology will one day tear down the speed barriers that limit our underst<strong>and</strong>ing<br />

of complex quantum systems. At its core lies the deterministic <strong>and</strong> robust generation of entanglement.<br />

Our group has succeeded in generating multiparticle entangled states of trapped atoms for<br />

the first time, by spin-squeezing a two-component Bose-Einstein condensate of 87 Rb atoms [1]. We<br />

have developed a novel tomographic method for analyzing <strong>and</strong> visualizing these experimental states<br />

through the spherical Wigner function [2].<br />

[1] M. Riedel, P. Böhi, Y. Li, T. W. Hänsch, A. Sinatra, <strong>and</strong> P. Treutlein, Atom-chip-based generation of entanglement for<br />

quantum metrology, Nature 464, 1170 (2010)<br />

[2] R. Schmied <strong>and</strong> P. Treutlein, Tomographic reconstruction of the Wigner function on the Bloch sphere, arXiv:1101.4131<br />

(2011)<br />

120


17:30 613 BCS-BEC crossover in a two-dimensional Fermi gas<br />

Gianluca Bertaina 1 , Stefano Giorgini 2<br />

1 Institut de Théorie des Phénomènes Physiques, EPFL, Station 3, CH-1015 Lausanne<br />

2 INO-CNR BEC Center <strong>and</strong> <strong>Physics</strong> Dep., Univ. of Trento, Via Sommarive 14, IT-38123 Povo, Trento<br />

We investigate the crossover from Bardeen-Cooper-Schrieffer (BCS) superfluidity to Bose-Einstein<br />

condensation (BEC) in a two-dimensional Fermi gas at T=0 using the fixed-node diffusion Monte<br />

Carlo method. We calculate the equation of state <strong>and</strong> the gap parameter as a function of the interaction<br />

strength, observing large deviations compared to mean-field predictions. In the BEC regime our<br />

results show the important role of dimer-dimer <strong>and</strong> atom-dimer interaction effects that are completely<br />

neglected in the mean-field picture. Results on Tan’s contact parameter associated with short-range<br />

physics are also reported along the BCS-BEC crossover.<br />

17:45 614 Towards an ion-photon quantum interface<br />

Andreas Stute, Bernardo Casabone, Birgit Br<strong>and</strong>stätter, Diana Habicher, Andrew McClung,<br />

Johannes Ghetta, Tracy Northup, Rainer Blatt<br />

Inst. für Experimentalphysik, Uni Innsbruck, Technikerstr. 25, AT-6020 Innsbruck<br />

In one promising scheme for an ion-based quantum network, photons transfer quantum information<br />

as flying qubits between stationary ions. For this transfer to be reversible, the quantum interface is<br />

realized via the coherent coupling of the ion to the field of an optical resonator. Here, we discuss our<br />

experimental progress towards the realization of such an ion-photon quantum interface.<br />

In our system, a single trapped 40 Ca + ion is coupled to the mode of a high-finesse optical resonator.<br />

Single photons are generated in a vacuum-stimulated Raman process between two atomic states<br />

driven by a laser <strong>and</strong> the vacuum field of the resonator. In this Raman process, all Zeeman substates<br />

of the atom are resolved. Both the polarization state of the photon as well as the state of the atom<br />

are detected. These prerequisites enable schemes including ion-photon entanglement as well as ionphoton<br />

state mapping, both of which will be discussed.<br />

18:00 615 Towards the creation of a quantum gas of polar ground state molecules<br />

Markus Debatin, Lukas Reichsöllner, Tetsu Takekoshi, Raffael Rameshan, Almar Lercher,<br />

Fransesca Ferlaino, Rudolf Grimm, Hanns-Christoph Nägerl<br />

Inst. für Experimentalphysik, Universität Innsbruck, Technikerstr 25, AT-6020 Innsbruck<br />

Dipolar quantum gases promise the realization of novel many-body quantum phases as a result of<br />

the long-range <strong>and</strong> anisotropic interaction, c.f. Ref[1]. For our Rb-Cs mixture experiment the focus<br />

is on the creation of a bosonic quantum gas of polar ground-state RbCs molecules using Feshbach<br />

association <strong>and</strong> subsequent stimulated adiabatic Raman transfer (STIRAP). Our approach is similar<br />

to the one used in Ref’s. [2,3]. We create a high phase-space density sample of ultracold Feshbach<br />

molecules. Prior to that, we produce a double Bose-Einstein condensate (BEC) of Rb <strong>and</strong> Cs atoms<br />

[4]. We perform high-resolution molecular spectroscopy on the Feshbach molecules <strong>and</strong> find intermediate<br />

electronically excited levels suitable for RbCs ground-state transfer. We have measured the<br />

binding energy of the RbCs rovibrational ground state in two-photon spectroscopy. We are currently<br />

implementing an optical lattice to create a Mott-insulator state having precisely one atom of each<br />

species at each lattice site with the aim to improve the creation efficiency for the Feshbach molecules<br />

<strong>and</strong> to shield the particles from collisional loss during state transfer.<br />

[1] M.A. Baranov, <strong>Physics</strong> Reports 464 (2008)<br />

[2] J.G. Danzl et al., Science 321 (2008), J.G. Danzl et al, Nature <strong>Physics</strong> 6 (2010)<br />

[3] K.-K. Ni et al., Science 322, 231 (2008)<br />

[4] A. Lercher et al. arXiv:1101.1409v1 (2011)<br />

18:15 616 Probing Spin-fluctuations in an ultracold Fermi gas<br />

David Stadler, Institute for <strong>Quantum</strong> Electronics, ETH Zürich, Schafmattstrasse 16, 8093 Zürich<br />

Current theoretical <strong>and</strong> experimental efforts in the field of ultra cold atoms are directed towards the<br />

preparation <strong>and</strong> detection of magnetically ordered systems, in the context of which the observation<br />

of spin-fluctuations has been proposed as a promising tool.<br />

We present in-situ observations of spin fluctuations in a two-component Fermi gas of Lithium atoms.<br />

Therefore we use a quantum-limited interferometer with a spatial resolution of 1.8 µm to directly<br />

probe the correlations in our atomic gas by measuring the probability distribution of the local spinpolarization.<br />

We observe a temperature-dependent reduction of spin-fluctuations up to 4.5 dB below<br />

121


shot-noise in weakly interacting Fermi gases <strong>and</strong> a even stronger reduction by 9.2 dB in a strongly<br />

interacting gas of molecules. From these measurements we determine the macroscopic magnetic<br />

susceptibility of our Fermi gas.<br />

18:30 Postersession <strong>and</strong> Apéro<br />

Thursday, 16.06.2011, CE 101<br />

Time ID III: <strong>Quantum</strong> oPtIcs<br />

Chair: Victor Lebedev, Uni Fribourg<br />

14:00 621 Hybrid <strong>Quantum</strong> System:Coupling Color Centers to Superconducting Cavities<br />

Johannes Majer 1 , Robert Amsüss 1 , Christian Koller 1 , Tobias Nöbauer 1 , Stefan Putz 1 ,<br />

Matthias Schramböck 1 , Stefan Rotter 2 , Jörg Schmiedmayer 1<br />

1 Atominstitut, TU Wien, Stadionallee 2, AT-1020 Wien<br />

2 Institute for Theoretical <strong>Physics</strong>, TU Wien, Stadionallee 2, AT-1020 Wien<br />

Reversible transfer of quantum information between long-lived memories <strong>and</strong> quantum processors<br />

is a favorable building block of scalable quantum information devices. We present recent experimental<br />

results of strong coupling between an ensemble of nitrogen-vacancy center electron spins in<br />

diamond <strong>and</strong> a superconducting microwave coplanar waveguide resonator. Although the coupling<br />

between a single spin <strong>and</strong> the electromagnetic field is typically rather weak, collective enhancement<br />

allows entering the strong coupling regime. With our experimental set-up we are able to directly observe<br />

this characteristic scaling of the collective coupling strength with the square root of the number<br />

of emitters. Additionally, we measure hyperfine coupling to 13 C nuclear spins, which is a first step<br />

towards a nuclear ensemble quantum memory. Using the dispersive shift of the cavity resonance<br />

frequency, we measure the relaxation time T 1 of the NV center at millikelvin temperatures in a nondestructive<br />

way.<br />

14:30 622 Generation of Orbital Angular Momentum Carrying Beams<br />

in Semiconductor Microcavities<br />

Francesco Manni 1 , Konstantinos G. Lagoudakis 1 , Taofiq Paraiso 1 , Rol<strong>and</strong> Cerna 1 ,<br />

Yoan Leger 1 , Tim C. H. Liew 2 , I. A. Shelykh 3 , A. V. Kavokin 4 , François Morier-Genoud 1 ,<br />

Benoit Deveaud-Plédran 1<br />

1 EPFL-ICMP-LOEQ, Station 3, Boite C, CH-1015 Lausanne<br />

2 EPFL-ITP, Station 3, Boite C, CH-1015 Lausanne<br />

3 Science Institute, University of Icel<strong>and</strong>, Dunhagi-3, IS-107 Reykjavik<br />

4 <strong>Physics</strong> & Astronomy School, University of Southampton, Highfield, Southampton, SO171BJ, UK<br />

It is notable that all techniques for the creation of beams with orbital angular momentum, to the best<br />

of our knowledge, require an optically inhomogeneous <strong>and</strong>/or anisotropic material or strong focusing.<br />

In this work, we demonstrate that the spin-to-orbital angular momentum (SOAM) conversion<br />

can also be achieved in a planar semiconductor microcavity. Despite being an isotropic system, microcavities<br />

exhibit a polarization splitting between transverse electric - transverse magnetic (TE-TM)<br />

modes, which induces the appearance of an L = +2 orbital angular momentum in one of the circular<br />

polarizations, under excitation in the cross-circular polarization [1]. The vortical entities resulting from<br />

this conversion process can be regarded as the optical equivalent of a pair of half-quantum vortices.<br />

We provide a theoretical model which rigorously derives the principle of the SOAM conversion <strong>and</strong><br />

quantitatively reproduces the experimental observations.<br />

[1] T. C. H. Liew, et al., PRB, 75, 241301 (2007)<br />

122


14:45 623 Phonon-tunneling dissipation in mechanical resonators<br />

Garrett Cole 1 , Ignacio Wilson-Rae 2 , Katharina Werbach 1 , Michael Vanner 1 , Markus Aspelmeyer 1<br />

1 Vienna Center for <strong>Quantum</strong> Science <strong>and</strong> Technology, Faculty of <strong>Physics</strong>, University of Vienna,<br />

Boltzmanngasse 5, AT-1090 Vienna<br />

2 Physik Department, James-Franck-Straße, DE-85748 Garching<br />

Micro- <strong>and</strong> nanoscale mechanical resonators have emerged as ubiquitous devices for application in<br />

a wide range of technical disciplines including communications, sensing, metrology, <strong>and</strong> fundamental<br />

scientific endeavors. In many instances, the performance of these devices is limited by the deleterious<br />

effects of mechanical damping. To further compound this limitation, the quantitative underst<strong>and</strong>ing<br />

of many damping mechanisms remains elusive. Here, we report a significant advancement<br />

towards predicting <strong>and</strong> controlling support-induced losses, a key dissipation mechanism in highquality-factor<br />

mechanical resonators. We have developed an efficient finite-element-enabled numerical<br />

solver, employing the recently introduced “phonon tunneling” approach. Exploiting this solver<br />

we demonstrate the ability to predict the design-limited damping of generic mechanical resonators,<br />

yielding excellent agreement with experimental measurements on custom-fabricated monocrystalline<br />

resonators [1]. Thus, our phonon-tunneling solver represents a major step towards accurate prediction<br />

of the mechanical quality factor in micro- <strong>and</strong> nanomechanical resonators.<br />

[1] G. D. Cole, I. Wilson-Rae, K. Werbach, M. R. Vanner, <strong>and</strong> M. Aspelmeyer, “Phonon-tunnelling dissipation in mechanical<br />

resonators,” Nature Communications 2, 231, 8 March (2011)<br />

15:00 624 Towards Time-Bin Entangled Photons from <strong>Quantum</strong> Dots<br />

Harishankar Jayakumar 1 , Gregor Weihs 1 , Ana Predojevic 1 , Glenn Solomon 2<br />

1 Institute for Experimental <strong>Physics</strong>, Universität Innsbruck, Technikerstrasse 25d, AT-6020 Innsbruck<br />

2 JQI, NIST, University of Maryl<strong>and</strong>, Maryl<strong>and</strong>, 20899 Gaithersburg, USA<br />

Entangled photon pairs are essential for the implementation of quantum communication protocols.<br />

The most common is the polarization entangled photons produced from a parametric down conversion<br />

(PDC) source. J.D Franson proposed an experiment for the test of Bell´s inequality with energytime<br />

entangled photons, experimentally realized by P. G. Kwiat et al using photon pairs from a PDC<br />

source. J. Brendel et al , realized a discrete version of energy-time entanglement, the time-bin entanglement<br />

by pumping PDC crystal at two well defined times set by a pump interferometer. Based on<br />

this discrete version C. Simon <strong>and</strong> J-P Poizat PRL 94, 110501 (2005) proposed a scheme for generating<br />

time-bin entangled photon pairs from quantum dots. Here we will be presenting our experimental<br />

setup <strong>and</strong> the progress towards the generation of time-bin entangled photons from quantum dots.<br />

This research was supported in part by the European Research Council (ERC) <strong>and</strong> by the Canadian Institute for Advanced<br />

Research (CIFAR).<br />

15:15 625 Optically driven electron pump using In(Ga)As quantum dots<br />

Laurent Nevou 1 , Valeria Liverini 1 , Arun Mohan 2 , Giancarlo Cerulo 1 , Fabrizio Castellano 1 ,<br />

Alfredo Bismuto 1 , Peter Friedli 3 , Hans Sigg 3 , Eli Kapon 2 , Jerome Faist 1<br />

1 Institute for <strong>Quantum</strong> Electronics, ETH Zürich, Wolfgang-Pauli-Strasse 16, CH-8093 Zürich<br />

2 EPFL, CH-1015 Lausanne<br />

3 Laboratory for Micro- <strong>and</strong> Nanotechnology, PSI, CH-5232 Villigen PSI<br />

The discoveries of the Josephson <strong>and</strong> the quantum Hall effects have revolutionized the metrology of<br />

electrical quantities. As a result, there is an increased interest in closing the metrological triangle [1]<br />

by the construction of an electron pump in which N electrons of charge q are pumped individually at<br />

a frequency f.<br />

Here, we propose an electron pump based on In(Ga)As/GaAs quantum dots (QDs) optically pumped<br />

by a pulsed laser. It consists of one plane of QDs coupled to an InGaAs quantum well (QW) reservoir<br />

via an AlGaAs barrier. A pulsed laser periodically ionizes the QDs. As a result, if the laser pulse<br />

duration is shorter than the time required for the electrons in the QW to refill the QDs, the number of<br />

electrons generated can be counted [2].<br />

[1] J. Flowers, Science,306, 1324(2004).<br />

[2] L. Nevou, et al., Nature <strong>Physics</strong> (in print),Published online: 20 February 2011<br />

123


15:30 626 Strong coupling between the cyclotron resonance<br />

of a high mobility 2D electron gas <strong>and</strong> a LC metamaterial<br />

Giacomo Scalari 1 , Dana Turcinkova 1 , Christian Reichl 2 , Dieter Schuh 3 , Werner Wegscheider 2 ,<br />

Mattias Beck 1 , Jérôme Faist 1<br />

1 Institute of <strong>Quantum</strong> Electronics, ETH Zürich, Wolfgang Pauli Strasse 16, CH-8093 Zürich<br />

2 Laboratory for Solid State physics, ETH Zürich, Schafmattstr. 16, CH-8093 Zürich<br />

3 Universität Regensburg, Universitätsstraße 31, DE-8093 Regensburg<br />

We report about observation of strong light-matter coupling between the cyclotron resonance of an<br />

high-mobility two dimensional electron gas (2DEG) <strong>and</strong> the resonances of a planar THz metamaterial<br />

composed by LC split-ring resonators. A THz-TDS system coupled to superconducting magnet<br />

probes the THz transmission of the sample in the banwidth 0-3.5THz. The LC resonances observed<br />

with no applied magnetic field are at 1 THz <strong>and</strong> 2.3 THz. Once the magnetic field value is increased,<br />

we observe a strong modification of the transmission spectra with some clear anticrossings between<br />

the different branches. Uncoupled cyclotron signal is also observed because the 2DEG in between<br />

the resonators is still present. We observe the disappearing of both cavity modes as the system enters<br />

the strong coupling regime <strong>and</strong> the evolution of the magnetopolaritonic branches as the value of<br />

the field is swept through the resonances.<br />

15:45 627 Highly efficient lasers <strong>and</strong> amplifiers in double tungstates<br />

Markus Pollnau, Dimitri Geskus, Koop van Dalfsen, Sonia M. García-Blanco, Shanmugam Aravazhi,<br />

MESA+ Institute for Nanotechnology, University of Twente, P.O. Box 217, NL-7500 AE Enschede<br />

The double tungstates KY(WO ) , KGd(WO ) , <strong>and</strong> KLu(WO ) are excellent c<strong>and</strong>idates for solid-state<br />

4 2 4 2 4 2<br />

lasers because of the large transition cross-sections of optically active rare-earth ions doped into<br />

these hosts. We grow actively doped KY Gd Lu (WO ) layers onto KY(WO ) substrates by liquid-<br />

1-x-y x y 4 2 4 2<br />

phase epitaxy. Co-doping the layers with optically inert Gd3+ <strong>and</strong> Lu3+ ions simultaneously allows for<br />

lattice matching <strong>and</strong> enhanced refractive index contrast with respect to the substrate. Low-loss channel<br />

waveguides are microstructured into the layers by Ar + 16:00<br />

-beam etching, resulting in strong pump<strong>and</strong><br />

signal-mode confinement. Yb-doped channel waveguide lasers deliver 650 mW output power at<br />

1 µm. Record-high slope efficiency (85%) <strong>and</strong> record-low quantum defect (0.7%) for dielectric lasers<br />

are achieved. In pump-signal experiments, exploiting highly doped KGd Lu Yb (WO ) chan-<br />

0.447 0.078 0.475 4 2<br />

nel waveguides, we demonstrate a giant optical gain of 950 dB/cm, exceeding the gain previously<br />

reported in rare-earth-ion-doped materials by two orders of magnitude <strong>and</strong> comparable to the gain<br />

obtained in semiconductor optical amplifiers.<br />

Coffee Break<br />

Time ID Iv: codensed helIum / atomIc clocks<br />

Chair: Antoine Weis, Uni Fribourg<br />

16:30 631 Electron Spin Resonance of 87Rb Monomers on Superfluid Helium Nanodroplets<br />

<strong>and</strong> Introduction of a Simple Model for Optical Pumping<br />

Alex<strong>and</strong>er Volk, Johannes Poms, Markus Koch, Wolfgang E. Ernst<br />

Institute of Experimental <strong>Physics</strong>, Graz University of Technology, Petersgasse 16, AT-8010 Graz<br />

Electron spin resonance (ESR) spectroscopy on superfluid helium nanodroplets (HeN) has recently<br />

been performed for 85 Rb [1]. Electronic perturbation of the alkali-metal atom induced by the HeN<br />

leads to a droplet size dependent change of the hyperfine constant aHFS. The investigation of ESR<br />

silent species inside HeN, by measuring their interaction with an alkali-metal atom situated on the<br />

droplet surface, is expected to be more sensitive for 87 Rb because of its larger hyperfine coupling<br />

(aHFS = 3417 MHz). We present new ESR spectra of single 87 Rb atoms on HeN [2]. The amplitude of<br />

ESR transitions measured by means of optically detected magnetic resonance, turned out to strongly<br />

depend on the laser polarization <strong>and</strong> power. A simple model for optical pumping on HeN has been<br />

established. Modelling of changes in the observed line shapes is expected to reveal new information<br />

concerning the droplet size dependence of aHFS <strong>and</strong> is object of current work.<br />

[1] M. Koch, G. Auböck, C. Callegari, <strong>and</strong> W. E. Ernst, Phys. Rev. Lett. 103, 035302 (2009)<br />

[2] A. Volk, J. Poms, M. Koch, <strong>and</strong> W. E. Ernst, J. Phys. Chem. A, in press 2011<br />

124


17:00 632 High-Spin States of Heavy Alkali Trimers<br />

Gerald Auböck 1 , Andreas W. Hauser 2 , Wolfgang E. Ernst 2<br />

1 Laboratory of Ultrafast Spectroscopy, EPFL, Station 6 , CH-1015 Lausanne<br />

2 Institute of Experimental <strong>Physics</strong>, Graz University of Technology, Petersgasse 16, AT-8010 Graz<br />

Triatomic alkali-metal molecules in their high-spin manifolds of electronic states are of fundamental<br />

interest for different reasons: On one h<strong>and</strong>, they represent a class of highly magnetic metal clusters<br />

whose electronic level structure obeys a simple shell model [1]. On the other h<strong>and</strong>, three parallel spin<br />

alkali atoms may form a weakly bound molecule in low-temperature collisions in a magneto-optic<br />

trap. From a theoretical point of view, they provide the chance to investigate the spectroscopic consequences<br />

of the combination of Jahn-Teller effect <strong>and</strong> spin-orbit coupling with powerful methods<br />

of quantum chemistry such as open-shell coupled cluster approaches <strong>and</strong> multireference Rayleigh-<br />

Schroedinger perturbation theory. With respect to available experimental data the 2 4 E1 4 A2 transitions<br />

are selected to document the quenching of the paradigmatic Exe Jahn-Teller distortion with<br />

increasing spin-orbit coupling. Simulated spectra for potassium, rubidium <strong>and</strong> cesium trimers are<br />

provided together with all relevant parameters such as harmonic frequencies, Jahn-Teller parameters<br />

<strong>and</strong> spin-orbit splittings obtained from the ab initio approach [2].<br />

[1] A. W. Hauser, C. Callegari <strong>and</strong> W. E. Ernst, in: Advances in the Theory of <strong>Atomic</strong> <strong>and</strong> Molecular Systems (eds. P.<br />

Piecuch et al.), (Springer Series Progress in Theoretical Chemistry <strong>and</strong> <strong>Physics</strong> 20) DOI 10.1007/978-90-481-2985-<br />

0_10, Springer Science+Business Media B.V. 2009, p. 199-214.<br />

[2] A. W. Hauser, G. Auböck <strong>and</strong> W. E. Ernst, in: Vibronic Interactions <strong>and</strong> the Jahn-Teller Effect II: Applications (ed.<br />

Claude Daul), (Springer Series Progress in Theoretical Chemistry <strong>and</strong> <strong>Physics</strong>) Springer Science+Business Media<br />

2011, in press.<br />

17:15 633 Spectroscopy of Cs <strong>and</strong> Rb perturbed by He in gas <strong>and</strong> condensed phase<br />

Victor Lebedev, Peter Moroshkin, Antoine Weis<br />

Department of <strong>Physics</strong>, University of Fribourg, Chemin du Musee 3, CH-1700 Fribourg<br />

Electronic transitions of alkali-metal atoms interacting with rare-gas atoms are well-known model<br />

systems for the study of line broadening due to atomic collisions in the gas phase, <strong>and</strong> of atomic<br />

bubbles formed by foreign atoms embedded in condensed helium cryomatrices. In the gas phase<br />

the motion of rare gas atoms is totally uncorrelated, even at high densities, <strong>and</strong> their interactions with<br />

the alkali atom can be treated independently. In contrast, in the atomic bubble model the motion of<br />

the He atoms surrounding the impurity is strongly correlated <strong>and</strong> is described in terms of collective<br />

modes, such as phonons or bubble interface oscillations. Here we present an experimental <strong>and</strong><br />

theoretical study of the crossover between these two regimes, which occurs in supercritical fluid<br />

helium doped with Cs or Rb atoms <strong>and</strong> locally heated by strong laser pulses, conditions which have<br />

not been addressed to date.<br />

Work funded by SNF, #200020-129831<br />

17:30 634 Measurement of the DC Stark shift of the Cs clock transition frequency<br />

Jean-Luc Robyr, Paul Knowles, Antoine Weis<br />

Department of physics, University of Fribourg, 3 rue du Musée, CH-1700 Fribourg<br />

The Stark effect describes the shift of atomic energy levels induced by an external electric field. In<br />

Cs atomic clocks, the AC Stark shift arising from the blackbody radiation is an important source of<br />

systematic frequency shifts. We are performing an optical Raman-Ramsey pump-probe experiment<br />

on a thermal Cs atomic beam to make a precise measurement of the Cs ground states third-order<br />

electric polarizabilities parameterizing the Stark shift. The experimental scheme is similar to that of Cs<br />

atomic beam clocks except that the microwave cavities are replaced by coherent population trapping<br />

(CPT) interactions <strong>and</strong> that a static electric field is applied to the atoms during their free evolution.<br />

The electric field calibration by numerical simulation as well as direct field measurements using the<br />

(3) Aharonov-Casher phase shift will be discussed <strong>and</strong> an absolute value for a will be presented.<br />

0<br />

Work funded by SNF #200020-126499<br />

125


18:00 635 Laser-microwave double-resonance spectroscopy<br />

in mm-scale Rb vapour cells for atomic clocks<br />

Christoph Affolderbach 1 , Matthieu Pellaton 1 , Gaetano Mileti 1 , Yves Pétrem<strong>and</strong> 2 , Nico de Rooij 2<br />

1 Laboratoire Temps-Fréquence, Université de Neuchâtel, Bellevaux 51, CH-2000 Neuchâtel<br />

2 SAMLAB, EPFL, Jaquet-Droz 1, CP 526, CH-2002 Neuchâtel<br />

We report on double-resonance spectroscopy of the 87Rb ground-state hyperfine “clock” transition in<br />

mm-scale micro-fabricated vapour cells, in view of novel miniature atomic clocks for low-power <strong>and</strong><br />

mobile applications. Compared to clocks based on coherent population trapping developed during<br />

the past decade, the double-resonance scheme has the advantage of reduced signal background<br />

<strong>and</strong> avoids the issue of high-frequency modulation of the laser source.<br />

The micro-fabricated cells are produced from Si pre-form wafers <strong>and</strong> glass plates sealed by anodic<br />

bonding, <strong>and</strong> filled with Rb <strong>and</strong> a buffer gas. Double-resonance clock signals are obtained by optical<br />

pumping with a 795 nm DFB laser <strong>and</strong> applying microwave radiation at 6.8 GHz via a compact<br />

microwave resonator. Analysis of the clock signals in view of the main parameters relevant for an<br />

atomic clock is presented. Preliminary clock stabilities are < 3·10-11 at 1 second <strong>and</strong> < 4·10-12 at 100<br />

seconds of integration time.<br />

18:15 END<br />

19:30 Conference Dinner<br />

ID atomIc PhysIcs <strong>and</strong> <strong>Quantum</strong> oPtIcs Poster<br />

641 Energy harvesting in doped helium nano-droplets<br />

Matthias Daxner 1 , Harald Schoebel 1 , Peter Bartl 1 , Christian Leidlmair 1 , Samuel Zoettl 1 , Stephan Denifl 1 ,<br />

Tilmann D. Märk 1 , Paul Scheier 1 , Daniel Spånberg 2 , Andreas Mauracher 2 , Diethard K. Bohme 3<br />

1 Institute for Ion <strong>Physics</strong> <strong>and</strong> Applied <strong>Physics</strong>, University of Innsbruck, Technikerstraße 25, AT-6020 Innsbruck<br />

2 Department of Materials Chemistry, Uppsala University, Box 538, SE-75121 Uppsala<br />

3 Department of Chemistry, York University, 4700 Keele Street, CA-Toronto, M3J 1P3<br />

We report the observation of a novel ionization mechanism in which doubly charged ions are produced inside a<br />

helium droplet by sequential Penning Ionization. Doping superfluid 4He-clusters with methyl iodide or mercury<br />

<strong>and</strong> exposing them to electrons enhances the formation of doubly charged atomic ions (I ++ or Hg ++ ) at the energy<br />

threshold for the production of two metastable He-atoms.<br />

These observation points toward a novel ionization process in which doubly-charged ions are produced by sequential<br />

PI. We observed also changes in the distribution of argon clusters within He-clusters, due to Coulomb<br />

explosion, at the energy threshold for the production of two or three metastable He-atoms, again indicating the<br />

occurrence of this novel ionization process. Our experimental results clearly demonstrate the possibility of sequential<br />

PI <strong>and</strong> energy harvesting in He nano-droplets. This universal process may well contribute substantially<br />

to radiation damage in biological systems exposed to ionizing radiation.<br />

642 Time <strong>and</strong> frequency metrology with laser cooled atoms:<br />

Evaluation of the Swiss continuous atomic fountain clock<br />

Laurent Devenoges 1 , Gianni Di Domenico 1 , André Stefanov 2 , Alain Joyet 1 , Pierre Thomann 1<br />

1 Laboratoire Temps-Fréquence, Université de Neuchâtel, Av. de Bellevaux 51, CH-2000 Neuchâtel<br />

2 Office fédéral de métrologie (METAS), Lindenweg 50, CH-3003 Bern-Wabern<br />

<strong>Atomic</strong> fountain clocks presently contributing to the international atomic time (TAI) are operating in a pulsedmode.<br />

They provide the best realization of the SI second with relative uncertainties of a few parts in 10 16 . Our<br />

alternative approach consists in using a continuous beam of laser-cooled cesium atoms. Besides circumventing<br />

the Dick effect, a continuous fountain is interesting from the metrological point of view because the relative<br />

importance of the error budget contributors is quite different compared to a pulsed one. Evaluation of the frequency<br />

shifts specific to the continuous approach is currently underway in our laboratory. In particular, we can<br />

mention the light shift, which has been measured below 1.5·10 -16 , the second order Zeeman shift, with its error<br />

budget contribution below 5·10 -16 , the collisional shift <strong>and</strong> the end-to-end cavity phase shift. The latest results<br />

will be presented at the conference.<br />

126


643 Controlling the coherent atom-light interaction in free space<br />

Lukas Slodicka, Gabriel Hetet, Nadia Röck, Markus Hennrich, Rainer Blatt<br />

Institut für Experimentalphysik, Universität Innsbruck, Technikerstrasse 25/4, AT-6020 Innsbruck<br />

Underst<strong>and</strong>ing single atom-light interaction is essential for fundamental studies of quantum mechanics <strong>and</strong> for<br />

efficient realization of many quantum information protocols. We report on extinction experiments with a single<br />

atom in free space. By focusing a weak <strong>and</strong> narrowb<strong>and</strong> Gaussian laser beam onto trapped single Barium ion<br />

using a high numerical aperture lens, we observe light extinction of up to 1.35%. We also demonstrate electromagnetically<br />

induced transparency of the ion by tuning a strong control beam over a two-photon resonance in<br />

a three-level lambda-type system. Furthermore, we investigate the properties of a single atom as a coherent<br />

reflector. We use a novel cavity setup where one of the mirrors is replaced by a single trapped ion. We observe<br />

quantum-electro-dynamics effects in a regime, where the laser intensity is already changed by the atom alone.<br />

644 On Relativistic Photoexcitation <strong>and</strong> Decay Rates in Hydrogenic Atoms<br />

Gerhard Adam 1 , A. V. Soldatov 2 , Josip Seke 1 , Martin Polak 1<br />

1 Institut für Theoretische Physik, Technische Universität Wien, Wiedner Hauptstrasse 8-10/136, AT-1040 Wien<br />

2 V. A. Steklov Mathematical Institute, Dept. of Mechanics, 8, Gubkina str., RU-119991 Moscow<br />

By using the plane-wave expansion for the electromagnetic-field vector potential, relativistic bound-bound <strong>and</strong><br />

bound-unbound transition matrix elements for hydrogenic atoms are expressed universally in terms of hypergeometric<br />

functions of the type F in such a way that these functions only depend on the absolute value of<br />

2 1<br />

the wave vector |k| <strong>and</strong> the dependence on angular variables of the wave vector is totally factored out <strong>and</strong> only<br />

comes through functional multipliers built of spherical harmonics. The newfound representation for the matrix<br />

elements in question is very convenient for exact analytical <strong>and</strong> precise numerical evaluation of the relativistic<br />

photoexcitation <strong>and</strong> decay rates in hydrogenic atoms, thus providing precise analytical expressions in terms of<br />

hypergeometric functions for the relativistic rates of bound-bound absorption-emission <strong>and</strong> bound-unbound<br />

absorption processes.<br />

645 Spatially resolved magneto-relaxation of magnetic nanoparticles detected by cesium<br />

atomic magnetometers<br />

Natascia Castagna 1 , Paul Knowles 1 , Antoine Weis 1 , Alke Fink 2 , Isabelle Geissbühler 2 , Georg Bison 3<br />

1 Department of <strong>Physics</strong>, University of Fribourg, Chenin du Musée 3, CH-1700 Fribourg<br />

2 Department of Chemistry, University of Fribourg, Chenin du Musée 9, CH-1700 Fribourg<br />

3 Department of Neurology, Friedrich-Schiller University, Erlanger Alee 101, DE-07747 Jena<br />

Biocompatible superparamagnetic iron oxide nanoparticles (SPIONs) are finding many diagnostic <strong>and</strong> therapeutic<br />

applications in medical healthcare. In an external magnetic field, SPION samples align their magnetic<br />

moments by physical rotation, <strong>and</strong> a bulk magnetization is created. Once the magnetic field is switched off, the<br />

magnetization relaxes on characteristic time scales that range from nanoseconds to seconds. The relaxation parameters<br />

can be inferred from the time evolution of the magnetization measured via the decay of the associated<br />

field (magneto-relaxometry). When functionalized, the SPIONs can be made to bind to specific morphological<br />

structures. The relaxation signals will thus carry information on the specific particles’ position <strong>and</strong> environment.<br />

We will report on first magneto-relaxometry measurements made by a Cs atomic magnetometer array operated<br />

in a second order gradiometer configuration used to construct two-dimensional relaxation maps.<br />

We acknowledge financial support by the SNF (Sinergia grant No. CRSII2-130414-1).<br />

646 Hybrid <strong>Quantum</strong> Systems: Integrating <strong>Atomic</strong> <strong>and</strong> Solid-State Qubits<br />

Stefan Minniberger, Robert Amsüss, Stephan Schneider, Fritz Diorico, Christian Koller, Stefan Haslinger,<br />

Christoph Hufnagel, Christian Novotny, Matthias Schramböck, Johannes Majer, Jörg Schmiedmayer,<br />

Atominstitut, TU Wien, Stadionallee 2, AT-1020 Wien<br />

The goal of our project is to couple superconducting qubits to an ultracold cloud of Rubidium atoms. This combination<br />

of two physical systems will allow us to make use of the long coherence times in atomic ensembles <strong>and</strong><br />

of the fast processing of solid-state qubits.<br />

A prerequisite is to transport the atom cloud into a cryostat, which we implemented by using a mangetic conveyor<br />

belt. In the cryostat, the atoms are cooled down further <strong>and</strong> the resulting BEC is transferred to a magnetic wire<br />

trap, which allows precise contol of the location of the atomic cloud with respect to the microwave resonator.<br />

127


647 Diploar quantum gases of heteronuclear molecules in optical lattices<br />

Lukas Reichsöllner, Markus Debatin, Tetsu Takekoshi, Raffael Rameshan, Almar Lercher, Francesca Ferlaino,<br />

Rudolf Grimm, Hanns-Christoph Nägerl<br />

Inst. f. Experimentalphysik, Universität Innsbruck, Technikerstraße 25/4, AT-6020 Innsbruck<br />

Dipolar quantum gases promise the realization of novel many-body quantum phases as a result of the longrange<br />

<strong>and</strong> anisotropic interaction, c.f. Ref [1]. For our Rb-Cs mixture experiment the focus is on the creation<br />

of a bosonic quantum gas of polar ground-state RbCs molecules using Feshbach association <strong>and</strong> subsequent<br />

stimulated adiabatic Raman transfer (STIRAP). Our approach is similar to the one used in Ref’s. [2,3]. Prior to<br />

that, we produce a double Bose-Einstein condensate (BEC) of Rb <strong>and</strong> Cs atoms [4].<br />

Our goal is to improve the production of RbCs molecules by performing the Feshbach association <strong>and</strong> STI-<br />

RAP transfer in the presence of an optical lattice. We create a Mott-insulator state for the cesium atoms <strong>and</strong> a<br />

separated superfluid rubidium sample. We attach the rubidium atoms to the cesium atoms to achieve precisely<br />

one atom of each species per lattice site <strong>and</strong> perform the Feshbach association <strong>and</strong> the STIRAP transfer. This<br />

scheme prevents three-body loss <strong>and</strong> thus allows us to maximize the number of RbCs ground-state molecules.<br />

[1] M.A. Baranov, <strong>Physics</strong> Reports 464 (2008)<br />

[2] J.G. Danzl et al., Science 321 (2008), J.G. Danzl et al, Nature <strong>Physics</strong> 6 (2010)<br />

[3] K.-K. Ni et al., Science 322, 231 (2008)<br />

[4] A. Lercher et al. arXiv:1101.1409v1 (2011)<br />

648 Loss of hydrogen from amino acids by low energy electron attachment<br />

Benjamin Puschnigg 1 , Violaine Vizcaino 1 , Eugen Illenberger 2 , Paul Scheier 1 , Stephan Denifl 1<br />

1 Institut für Ionenphysik und Angew<strong>and</strong>te Physik, Universität Innsbruck, Technikerstr.25/3, AT-6020 Innsbruck<br />

2 Freie Universität Berlin, Takustrasse 3, DE-14195 Berlin<br />

Theoretical calculations <strong>and</strong> experiments showed that formic acid loses the hydrogen at the O-H site upon attachment<br />

of electrons with the energy of approximately 1.5 eV. In early studies, it was proposed that electrons<br />

attach initially at the p* (C=O) orbital (at 1.8 eV) <strong>and</strong> then the hydrogen splits off. Although the s* (O-H) orbital<br />

lies at higher energy (5 eV), we show here that an electron can attach directly at this orbital because of the broad<br />

width of the s* resonance.<br />

In our experiment, we studied a- <strong>and</strong> b-alanine <strong>and</strong> found out that the shape of the ion yield was changing<br />

significantly, the same effect was observed with aminobutanoic acid isomers.<br />

We observed sharp structures in the ion yield for the different molecules which can be associated to vibrations<br />

of the molecules (OH stretch overtones). This is confirmed by the measure of deuterated molecules.<br />

649 Towards the generation of entangled microcavity polaritons<br />

Mathias Sassermann 1 , Patrick Mai 1 , Zoltan Vörös 1 , Gregor Weihs 1 , Sven Höfling 2 , Alfred Forchel 2 ,<br />

Andreas Löffler 2<br />

1 University of Innsbruck, Technikerstrasse 25/d, At-6020 Innsbruck<br />

2 University of Würzburg, Am Hubl<strong>and</strong>, DE-97074 Würzburg<br />

Several theoretical studies have recently pointed out that microcavity polaritons can be a viable source of entangled<br />

photon pairs, either in the polarisation, or the frequency degree of freedom.<br />

As a first step towards a successful implementation, one has to have access to the full polariton dispersion. In<br />

order to achieve this, we utilise two spatial light modulators in a non-st<strong>and</strong>ard configuration; one for controlling<br />

the polariton momentum, the other for arbitrarily filtering the spectrum of a fs laser pulse, thus controlling the<br />

energy.<br />

In the paper, we will discuss our first results on polariton-polariton scattering in planar GaAs microcavities. We<br />

show that with our experimental configuration, the ingredients of the above-mentioned entanglement schemes<br />

are realised. Evidence for parametric polariton scattering will be presented.<br />

This research was supported in part by the Austrian Science Fund (FWF), the European Research Council (ERC) <strong>and</strong> the Canadian<br />

Institute for Advanced Research.<br />

128


650 Non-equilibrium dynamics in mixtures of Rydberg atoms <strong>and</strong> polar molecules<br />

Alex<strong>and</strong>er Glätzle, Guido Pupillo, Bo Zhao, Mikhail Baranov, Peter Zoller<br />

Institute for theoretical <strong>Physics</strong>, University of Innsbruck, Technikerstr. 25, AT-6020 Innsbruck<br />

We study the nonequilibrium dynamics of a many-body classical system of polar molecules <strong>and</strong> Rydberg atoms,<br />

subject to driving <strong>and</strong> dissipation. We show that long-range dipole-dipole interactions between hot molecules<br />

<strong>and</strong> cold atoms separately trapped in quasi two-dimensional geometries can lead to efficient sympathetic cooling<br />

of generic polar molecules to micro-Kelvin temperatures. We propose that direct laser cooling into a strongly<br />

correlated, e.g. crystalline, phase can be performed on a gas of groundstate atoms weakly dressed by laser<br />

light with an excited Rydberg state, in turn allowing for advanced tailoring of the spatial structure of the cold<br />

molecules.<br />

651 Photon-switches in quantum-optical networks<br />

Martin Suda, Christoph Pacher, AIT-Austrian Institute of Technology, Donau-City-Str. 1, AT-1220 Vienna<br />

We investigate quantum-optical networks for several input Fock states of photons <strong>and</strong> determine the total state<br />

appearing in the output ports. The most simple network is a single-loop Mach-Zehnder interferometer with two<br />

beam splitters <strong>and</strong> a phase shifter providing two inputs <strong>and</strong> two outputs. Moreover, we consider a double-loop<br />

interferometer with 3 inputs <strong>and</strong> 3 outputs. For product Fock states of several input modes the Hong-Ou-M<strong>and</strong>el<br />

effect plays an important role. The entangled output states <strong>and</strong> the mean photon numbers are determined as<br />

a function of various phase shifters. Using computerized simulation different network structures are analyzed.<br />

These investigations can be helpful for optical quantum computing.<br />

652 Light Effects on High Q-Resonators for Hybrid <strong>Quantum</strong> Systems<br />

Christian Koller, Robert Amsüss, Tobias Nöbauer, Matthias Schramböck, Jörg Schmiedmayer, Johannes Majer,<br />

VCQ, Atominstitut TU Wien, AT-1020 Vienna<br />

Over the last years hybrid quantum systems have drawn attention in the field of quantum information processing,<br />

because of their ability to combine the advantages of different quantum worlds (e.g. cold atoms, NV centers,<br />

superconducting Qubits...). The heart of these hybrid systems are superconducting microwave resonators with<br />

high quality factors (on the order of one million). The response of these resonators under the influence of light<br />

is very crucial, since many of the hybrid applications involve laser light with different intensity. We will present<br />

measurements of the shift of resonator frequency as a function of the applied light power. Furthermore, we show<br />

the effects on the Q value due to the generation of quasiparticles <strong>and</strong> the saturation of two-level fluctuators in<br />

the superconducting thin films.<br />

We will also put these facts in perspective with resent measurements of resonators strongly coupled to an<br />

ensemble of NV centers.<br />

129

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