superconducting rf
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Author(s):  
L. Lain Amador ◽  
P. Chiggiato ◽  
L. M. A. Ferreira ◽  
E. Garcia-Tabares ◽  
T. Koettig ◽  
...  

2021 ◽  
Vol 92 (6) ◽  
pp. 063303
Author(s):  
Kuldeep K. Singh ◽  
Vikas K. Jain ◽  
Dharmraj V. Ghodke ◽  
Avinash Puntambekar

2021 ◽  
Vol 32 (24) ◽  
pp. 245701
Author(s):  
Li Yang ◽  
Baiqi Liu ◽  
Zongbiao Ye ◽  
Chi Yang ◽  
Zhijun Wang ◽  
...  

Author(s):  
Yu-Lu Huang ◽  
Lu-Bei Liu ◽  
Tian-Cai Jiang ◽  
Ruo-Xu Wang ◽  
Sheng-Xue Zhang ◽  
...  

2021 ◽  
Vol 103 (2) ◽  
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Jared Carlson ◽  
Alden Pack ◽  
Mark K. Transtrum ◽  
Jaeyel Lee ◽  
David N. Seidman ◽  
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T. Junginger ◽  
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2020 ◽  
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A. Lumpkin ◽  
R. Thurman-Keup ◽  
D. Edstrom ◽  
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B. Jacobson ◽  
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2020 ◽  
Vol 77 (5) ◽  
pp. 337-343
Author(s):  
Ji-Gwang Hwang ◽  
Michael Abo-Bakr ◽  
Aleksandr Matveenko ◽  
Georgios Kourkafas ◽  
Thorsten Kamps

Abstract Over the past decades, many accelerator laboratories have put much effort into the development of compact energy-recovery linac (ERL) demonstrators to verify various physical and technical aspects of the generation, acceleration, transport and energy recovery of high brightness and high average current electron beams in a superconducting radio-frequency (SRF) linear accelerator. Beyond these goals, the ERL demonstrator also offers unique opportunities to study novel schemes for THz and X-ray radiation generation. In this paper, we discuss feasible options for schemes generating THz and X-ray radiation at low-energy continuous-wave (CW) SRF ERL demonstrators such as the bERLinPro accelerator.


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