Proceedings of the 19th International Conference on RF Superconductivity 2019
DOI: 10.18429/jacow-srf2019-mop049
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Prototypes Fabrication of 1.3 GHz Superconducting Rf Components for SHINE

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“…( 1)- (3) and are related to some parameters, such as the coupling coefficient b, beam current I b , cavity intrinsic quality factor Q 0 , cavity voltage V c , R/Q of the cavity, frequency detuning df, and resonant frequency f 0 [13]. For the SHINE project, the optimal Q ext of the 1.3 GHz superconducting cavities is 4.12 9 10 7 , under the following working conditions: the average linac beam current is 0.3 mA, the nominal accelerating gradient E acc of the 1.3 GHz superconducting cavity is 16.0 MV/m, the cavity intrinsic quality factor Q 0 is 2.7 9 10 10 , and the frequency detuning df caused by the peak microphonics effect is 10 Hz [14,15]. The required input power from a solid-state amplifier (SSA) for maintaining the operating gradient is approximately 6.6 kW, considering a waveguide transmission loss of 15%.…”
Section: Introductionmentioning
confidence: 99%
“…( 1)- (3) and are related to some parameters, such as the coupling coefficient b, beam current I b , cavity intrinsic quality factor Q 0 , cavity voltage V c , R/Q of the cavity, frequency detuning df, and resonant frequency f 0 [13]. For the SHINE project, the optimal Q ext of the 1.3 GHz superconducting cavities is 4.12 9 10 7 , under the following working conditions: the average linac beam current is 0.3 mA, the nominal accelerating gradient E acc of the 1.3 GHz superconducting cavity is 16.0 MV/m, the cavity intrinsic quality factor Q 0 is 2.7 9 10 10 , and the frequency detuning df caused by the peak microphonics effect is 10 Hz [14,15]. The required input power from a solid-state amplifier (SSA) for maintaining the operating gradient is approximately 6.6 kW, considering a waveguide transmission loss of 15%.…”
Section: Introductionmentioning
confidence: 99%
“…To reduce the construction and operating costs of large superconducting radio frequency (SRF) accelerating facilities [1][2][3], several surface treatments including standard surface treatment methods [4][5][6], nitrogen doping [7][8][9] and nitrogen infusion [10,11] have been investigated with 1.3 GHz superconducting cavities to obtain a high accelerating gradient of High Energy Physics [14,15] and the Thomas Jefferson National Accelerator Facility [16]. These baking recipes were first tested on 1.3 GHz single-cell cavities, and then successfully repeated on 1.3 GHz nine-cell cavities.…”
Section: Introductionmentioning
confidence: 99%
“…Recently, superconducting radio-frequency (SRF) cavities have been adopted in many accelerators worldwide [1][2][3][4][5]. To * Authors to whom any correspondence should be addressed.…”
Section: Introductionmentioning
confidence: 99%