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Abstracts Brochure - 2nd International Particle Accelerator Conference

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First, we develop a model describing this interaction<br />

and then we supplement it with numerical results<br />

using PIC code WARP***. We show that the ions<br />

move towards the area occupied by the dark current,<br />

but this does not increase the bombardment of<br />

micro-protrusions.<br />

* R.B. Palmer,et al, Phys. Rev ST Accel. Beams 12,<br />

031002 (2009).<br />

** P. Wilson, AIP Conf. Proc., 877, Melville, New<br />

York, 2006, p. 27.<br />

*** J.-L. Vay, et al, Physics of Plasmas, 11, 2928<br />

(2004).<br />

Funding Agency: This work is supported by Office<br />

of High Energy Physics of the U.S. Department of<br />

Energy.<br />

Sub Classification: T06 Room Temperature RF<br />

Poster Panel 100<br />

ID: 4471 - MOPC066<br />

Role of Nottingham and Thomson Effects in<br />

Heating of Micro-protrusion in High-gradient<br />

Accelerating Structures, Aydin Cem Keser, Tom<br />

Antonsen, Dmytro Kashyn, Gregory Nusinovich<br />

(UMD, College Park, Maryland) - It is widely<br />

accepted that one of the reasons for appearance of<br />

the RF breakdown which limits operation of highgradient<br />

accelerating structures is the electron dark<br />

current*. This field emitted current, usually<br />

considered as a precursor of the breakdown, can be<br />

emitted from apexes of microprotrusions on a<br />

structure surface. Therefore field and thermal<br />

processes in such protrusions deserve careful<br />

studies**. The goal of our first study*** was to<br />

analyze 2D process of RF field penetration inside<br />

protrusion of a metal with finite conductivity and to<br />

study corresponding Joule heating. In the present<br />

study, we include into consideration, first, the<br />

Nottingham effect which may significantly change<br />

the protrusion heating. Then, since protrusion<br />

heating in high-power, short-pulse operation can be<br />

strongly non-uniform, we include into consideration<br />

also Thomson effect which predicts additional<br />

heating/cooling in non-uniformly heated conductors.<br />

* Wang and Loew, SLAC-pub-7684,1997<br />

** K.L.Jensen,Y.Y. Lau, D.W. Feldman, P.G.<br />

O'Shea, Phys. Rev. ST Accel.Beams 11,<br />

081001(2008)<br />

*** Kashyn et al, AAC-2010.<br />

Sub Classification: T06 Room Temperature RF<br />

�<br />

30<br />

Poster Panel 101<br />

ID: 3159 - MOPC022<br />

Development of a Compact C-band Photocathode<br />

RF Gun, Xiaohan Liu, Chuanxiang Tang (TUB,<br />

Beijing) - A C-band photocathode RF gun for a<br />

compact electron diffraction facility is developed in<br />

Tsinghua University, which is designed to work at<br />

the frequency of 5.712GHz. This paper presents the<br />

physics and structure design of this C-band RF gun,<br />

and the comparison on beam dynamics of S-band<br />

and C-band photoinjector has been done. Some new<br />

structure design will be adopted in this gun,<br />

including the optimized cavity length and elliptical<br />

iris, which is helpful to achieve lower emittance and<br />

larger mode separation. This paper likewise presents<br />

experiment parameters and the preliminary cold test<br />

results of this C-band RF gun.<br />

Funding Agency This work is supported by<br />

National Natural Science Foundation of China and<br />

National Basic Research Program of China (973<br />

Program).<br />

Sub Classification: T06 Room Temperature RF<br />

Poster Panel 102<br />

ID: 1866 - MOPC026<br />

A-core Loaded Untuned RF Compression Cavity<br />

for HIRFL-CSR, Lirong Mei, Zhe Xu, Youjin<br />

Yuan, Hongwei Zhao (IMP, Lanzhou) - To meet the<br />

requirement of conducting high energy density and<br />

plasma physics research at HIRFL-CSR. The higher<br />

accelerating gap voltage was required. A magnetic<br />

alloy (MA)-core loaded radio frequency (RF) cavity<br />

which can provide higher accelerating gap voltage<br />

has been studied in Institute of Modern Physics,<br />

Chinese Academy of Sciences (IMP, CAS),<br />

Lanzhou. To select proper MA material to load the<br />

RF compression cavity, measurement for MA cores<br />

has been conducted. The MA core with higher<br />

permeability and shunt impedance, and lower<br />

quality factor (Q value) should be selected. The<br />

theoretical calculation and simulation for the MAcore<br />

loaded RF cavity can be consistent with each<br />

other well. Finally 230kW power was needed to<br />

meet 50-kV accelerating gap voltage by calculation.<br />

Sub Classification: T06 Room Temperature RF<br />

Poster Panel 103<br />

ID: 3198 - MOPC040<br />

The Measurement of Transversal Shunt<br />

Impedance of RF Deflector, Aleksandr Smirnov,<br />

Michael Vladimirovich Lalayan, Nicolay Sobenin<br />

(MEPhI, Moscow), Aleksandr Alekseevich<br />

Zavadtsev (Nano, Moscow) - This paper presents the

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