Overview of the 100 mA average-current RF photoinjector

被引:16
|
作者
Nguyen, DC
Colestock, PL
Kurennoy, SS
Rees, DE
Regan, AH
Russell, S
Schrage, DL
Wood, RL
Young, LM
Schultheiss, T
Christina, V
Cole, M
Rathke, J
Shaw, J
Eddy, C
Holm, R
Henry, R
Yater, J
机构
[1] Los Alamos Natl Lab, Los Alamos, NM 87545 USA
[2] Adv Energy Syst, Medford, NY 11763 USA
[3] USN, Res Lab, Washington, DC USA
来源
NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT | 2004年 / 528卷 / 1-2期
关键词
FEL; photoinjector; high current; high brightness; cw; photocathode;
D O I
10.1016/j.nima.2004.04.021
中图分类号
TH7 [仪器、仪表];
学科分类号
0804 ; 080401 ; 081102 ;
摘要
High-average-power FELs require high-current, low-emittance and low-energy-spread electron beams. These qualities have been achieved with RF photoinjectors operating at low-duty factors. To date, a high-average-current RF photoinjector operating continuously at 100% duty factor is yet to be demonstrated. The principal challenges of a high-duty-factor normal-conducting RF photoinjector are related to applying a high accelerating gradient continuously, thus generating large ohmic losses in the cavity walls, cooling the injector cavity walls and the high-power RF couplers, and finding a photocathode with reasonable Q.E. that can survive the poor vacuum of the RF photoinjector. We present the preliminary design of a normal-conducting 700 MHz photoinjector with solenoid magnetic fields for emittance compensation. The photoinjector is designed to produce 2.7 MeV electron beams at 3 nC bunch charge and 35 MHz repetition rate (100 mA average current). The photoinjector consists of a 2-1/2-cell, pi-mode, RF cavity with on-axis electric coupling, and a non-resonant vacuum plenum. Heat removal in the resonant cells is achieved via dense arrays of internal cooling passages capable of handling high-velocity water flows. Megawatt RF power is coupled into the injector through two tapered ridge-loaded waveguides. PARMELA simulations show that the 2 1/2-cell injector can produce a 7 mum emittance directly. Transverse plasma oscillations necessitate additional acceleration and a second solenoid to realign the phase space envelopes of different axial slices at higher energy, resulting in a normalized rms emittance of 6.5 mum and 34 keV rms energy spread. We are developing a novel cesiated p-type GaN photocathode with 7% quantum efficiency at 350 ran and a cesium dispenser to replenish the cathode with cesium through a porous silicon carbide substrate. These performance parameters will be necessary for the design of the 100 kW FEL. (C) 2004 Published by Elsevier B.V.
引用
收藏
页码:71 / 77
页数:7
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