Experimental studies of a high-gradient X-band welded hard-copper split accelerating structure

被引:6
|
作者
Agustsson, R. [1 ]
Carriere, P. [1 ]
Chimalpopoca, O. [1 ]
Dolgashev, V. A. [2 ]
Gusarova, M. A. [3 ]
Kutsaev, S., V [1 ]
Smirnov, A. Yu [1 ]
机构
[1] RadiaBeam Technol LLC, 1717 Stewart St, Santa Monica, CA 90404 USA
[2] SLAC Natl Accelerator Lab, 2575 Sand Hill Rd, Menlo Pk, CA 94025 USA
[3] Natl Res Nucl Univ MEPhI, Kashirskoe Sh 31, Moscow 115409, Russia
关键词
split accelerating structure; high-gradients; electron beam welding; hard copper; TECHNOLOGIES; SIMULATION; LINAC;
D O I
10.1088/1361-6463/ac4632
中图分类号
O59 [应用物理学];
学科分类号
摘要
Recent research on high-gradient radio frequency (RF) accelerating structures indicates that the use of hard copper alloys provides improvement in high gradient performance over annealed copper. Such structures are made by bonding individually manufactured parts. However, there are no well-established bonding techniques that preserve the hardness, surface finish and cleanliness required for high gradient operation. To preserve the copper hardness, RadiaBeam has developed a novel high-gradient split accelerating structure, based on electron beam welding joining technique. This technique provides efficient bonding with strong, clean welds and minimal thermal loading, while maintaining a clean inner RF environment. Our RF design and fabrication methodology limits the small heat affected zone to the outer cavity envelop, with virtually no distortions or thermal loading of critical RF surfaces. It also incorporates provisions to precisely control the gap despite conventional issues with weld joint shrinkage. To date we have manufactured and validated an RF accelerating structure joined by electron-beam welding that incorporates a novel open split design to significantly reduce the assembly complexity and cost. In this paper, we will present the electromagnetic design of this structure, discuss bonding, and present the results of high-power tests, where the accelerating gradients of 140 MV m(-1) with surface peak fields of 400 MV m(-1) were achieved for flat-top pulse length of 600 ns with an RF breakdown rate of 10(-4) 1/(pulsecm).
引用
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页数:17
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