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Abstracts Brochure - 2nd International Particle Accelerator Conference

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Poster Panel 35<br />

ID: 2926 - WEPS011<br />

Application of Orbit Response Matrix Method at<br />

CSNS/RCS, Yuwen An, Sheng Wang, Yuanyuan<br />

Wei (IHEP Beijing, Beijing) - China Spallation<br />

Neutron Source (CSNS) accelerator consists of an<br />

H- linac and a Rapid Cycling Synchrotron(RCS).<br />

RCS operates at 25Hz, accumulates 80MeV proton<br />

beam, and accelerates to 1.6GeV. Application of<br />

response matrix(RM) method to RCS has been<br />

studied. The closed orbit correction can be well<br />

performed by optimizing solution algorithm. To<br />

calibrate the lattice function, the fudge factors of<br />

quadrupoles, the offset of beam position monitors<br />

are obtained by using RM methods, and the study to<br />

improve the measurement accuracy has been done.<br />

The detailed simulation results in the study are<br />

shown in this paper.<br />

Sub Classification: A04 Circular <strong>Accelerator</strong>s<br />

Poster Panel 36<br />

ID: 2769 - WEPS012<br />

Commissioning of Slow Extraction in HIRFL-<br />

CSR, Jian Shi, Weiping Chai, Jie Li, Peng Li,<br />

Ruishi Mao, Jia Wen Xia, Jiancheng Yang, Da Yu<br />

Yin, Youjin Yuan (IMP, Lanzhou) - The HIRFL-<br />

CSR* contains a complex in cancer therapy**, and<br />

we realized the 1/3 order resonant slow extraction in<br />

May 2008. In order to improve the beam quality that<br />

required in the clinical treatment, we have<br />

performed 5 times machine study. The extraction<br />

efficiency has been improved to 65% by change the<br />

shape of the separatrix, and the spot size in the target<br />

is less than 3.5mm in FWHM, the spill uniformity<br />

we obtained excelled 97%.In the 5th time, we<br />

utilized the fast quadrupole to make a feedback, the<br />

spill quality been improved a lot. We report the<br />

latest commissioning result about the slow<br />

extraction and spill quality in HIRFL-CSR.<br />

* J.W. Xia, W.L. Zhan et al., Nuclear Instrum.<br />

Methods A 488, 11 (2002).<br />

** Y.J Yuan, High Power Laser and <strong>Particle</strong> Beams<br />

17(2), Feb 2005. Funding Agency<br />

Sub Classification: A04 Circular <strong>Accelerator</strong>s<br />

Poster Panel 37<br />

ID: 3087 - WEPS033<br />

Matching Laser Driven Proton Injectors to CH -<br />

Drift Tube Linacs, Ali Almomani, Martin Droba,<br />

Ulrich Ratzinger (IAP, Frankfurt am Main), Ingo<br />

�<br />

Classification 4: Hadron <strong>Accelerator</strong>s<br />

11<br />

Hofmann (GSI, Darmstadt; HIJ, Jena) -<br />

Experimental results and theoretical predictions in<br />

laser acceleration of protons achieved energies of ten<br />

to several tens of MeV. This study demonstrates the<br />

transporting and focusing of laser-accelerated 10<br />

MeV protons by a pulsed magnetic solenoid with a<br />

field gradient up to 18 T. The unique features of the<br />

protons distribution like extremely small emittances<br />

and high yield of the order of 10^13 protons per<br />

shot, make them attractive for study. The possibility<br />

of using these protons as a source of energetic ions<br />

for ion accelerators is addressed. With respect to<br />

transit energies, further acceleration by matching<br />

into rf linac seems adequate. The bunch injection<br />

into a proposed CH- structure is under investigation<br />

at IAP Frankfurt. Options and simulation tools are<br />

presented.<br />

Sub Classification: A08 Linear <strong>Accelerator</strong>s<br />

Poster Panel 38<br />

ID: 3576 - WEPS036<br />

First Coupled CH Power Cavity for the FAIR<br />

Proton Injector, Robert Brodhage, Christopher<br />

Fix, Holger Podlech, Ulrich Ratzinger (IAP,<br />

Frankfurt am Main), Gianluigi Clemente, Lars<br />

Groening (GSI, Darmstadt) - For the research<br />

program with cooled antiprotons at FAIR a<br />

dedicated 70 MeV, 70 mA proton injector is<br />

required. The main acceleration of this room<br />

temperature linac will be provided by six CH<br />

cavities operated at 325 MHz. Each cavity will be<br />

powered by a 2.5 MW Klystron. For the second<br />

acceleration unit from 11.5 MeV to 24.2 MeV a 1: 2<br />

scaled model has been built. Low level RF<br />

measurements have been performed to determine the<br />

main parameters and to prove the concept of coupled<br />

CH cavities. For this second tank technical and<br />

mechanical investigations have been performed in<br />

2010 to develop a complete technical concept for the<br />

manufacturing. In Spring 2011, the construction of<br />

the first power prototype has started. The main<br />

components of this cavity will be ready for<br />

measurements in summer 2011. At that time, the<br />

cavity will be tested with a preliminary aluminum<br />

drift tube structure, which will allow precise<br />

frequency and field tuning. This paper will report on<br />

the recent technical development and achievements.<br />

It will outline the main fabrication steps towards that<br />

novel type of proton DTL. Also first low level RF<br />

measurements are expected.

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