2015
DOI: 10.1088/1674-1137/39/2/028102
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Design and test of frequency tuner for a CAEP high power THz free-electron laser

Abstract: Zhenghui (米正辉) 1;2;1) SUN Yi(孙毅) 2 PAN Weimin(潘卫民) 2 LIN Haiying(林海英) 2 ZHAO Danyang (赵丹阳) 1;2 LU Xiangyang(鲁向阳) 3 QUAN Shengwen(全胜文) 3 LUO Xing(罗星) 3 LI Ming(黎明) 4,5 YANG Xingfan(杨兴繁) 4,5 WANG Guangwei(王光伟) 2 DAI Jianping(戴建枰) 2 LI Zhongquan(李中泉) 2 MA Qiang(马强) 2 SHA Peng(沙鹏)

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“…Constraining Galactic Dark Photons through Diurnal Modulation Analysis -We now embark on a search for the diurnal modulation of signals stemming from galactic dark photons, leveraging data from a previous DPDM search employing a single-cell elliptical niobium SRF cavity [32]. The cavity was equipped with a frequency tuning mechanism [79,80] and an amplifier circuit, and maintained in liquid helium at a temperature of approximately 2 K. The experimental platform [81][82][83][84][85][86] facilitated the calibration of relevant parameters, including the loaded quality factor Q L , coupling factor β, net amplification factor G net , and the resonant frequency of the TM 010 mode, centered around ω 0 ≈ 2π1.3 GHz, along with its stability range for each scanning process. Each scan step was approximately 5 minutes, with 100 seconds dedicated to data acquisi- In our analysis, only the received power at the resonant frequency bin with a bandwidth of 2π11.5 Hz [32], denoted by P i for the i-th step, was considered.…”
mentioning
confidence: 99%
“…Constraining Galactic Dark Photons through Diurnal Modulation Analysis -We now embark on a search for the diurnal modulation of signals stemming from galactic dark photons, leveraging data from a previous DPDM search employing a single-cell elliptical niobium SRF cavity [32]. The cavity was equipped with a frequency tuning mechanism [79,80] and an amplifier circuit, and maintained in liquid helium at a temperature of approximately 2 K. The experimental platform [81][82][83][84][85][86] facilitated the calibration of relevant parameters, including the loaded quality factor Q L , coupling factor β, net amplification factor G net , and the resonant frequency of the TM 010 mode, centered around ω 0 ≈ 2π1.3 GHz, along with its stability range for each scanning process. Each scan step was approximately 5 minutes, with 100 seconds dedicated to data acquisi- In our analysis, only the received power at the resonant frequency bin with a bandwidth of 2π11.5 Hz [32], denoted by P i for the i-th step, was considered.…”
mentioning
confidence: 99%