Noh Seon Yeong, Kim Eun-San, Hwang Ji-Gwang, Heo A, Jang Si won, Vinokurov Nikolay A, Jeong Young U K, Park Seong Hee, Jang Kyu-Ha
Department of Physics, Kyungpook National University, Daegu 702-701, South Korea.
WCI Center for Quantum-Beam-based Radiation Research, Korea Atomic Energy Research Institute, 989-111 Daedeok-Daero, Yuseong-gu, Daejeon, South Korea.
Rev Sci Instrum. 2015 Jan;86(1):014703. doi: 10.1063/1.4905532.
A cavity-type beam position monitor (BPM) has been developed for a compact terahertz (THz) free-electron laser (FEL) system and ultra-short pulsed electron Linac system at the Korea Atomic Energy Research Institute (KAERI). Compared with other types of BPMs, the cavity-type BPM has higher sensitivity and faster response time even at low charge levels. When electron beam passes through the cavity-type BPM, it excites the dipole mode of the cavity of which amplitude depends linearly on the beam offset from the center of the cavity. Signals from the BPM were measured as a function of the beam offset by using an oscilloscope. The microtron accelerator for the KAERI THz FEL produces the electron beam with an energy of 6.5 MeV and pulse length of 5 μs with a micropulse of 10-20 ps at the frequency of 2.801 GHz. The macropulse beam current is 40 mA. Because the microtron provides multi-bunch system, output signal would be the superposition of each single bunch. So high output signal can be obtained from superposition of each single bunch. The designed position resolution of the cavity-type BPM in multi-bunch is submicron. Our cavity-type BPM is made of aluminum and vacuum can be maintained by indium sealing without brazing process, resulting in easy modification and cost saving. The resonance frequency of the cavity-type BPM is 2.803 GHz and the cavity-type BPM dimensions are 200 × 220 mm (length × height) with a pipe diameter of 38 mm. The measured position sensitivity was 6.19 (mV/mm)/mA and the measured isolation between the X and Y axis was -39 dB. By measuring the thermal noise of system, position resolution of the cavity-type BPM was estimated to be less than 1 μm. In this article, we present the test results of the S-band cavity-type BPM and prove the feasibility of the beam position measurement with high resolution using this device.
韩国原子能研究所(KAERI)已为紧凑型太赫兹(THz)自由电子激光(FEL)系统和超短脉冲电子直线加速器系统开发了一种腔式束流位置监测器(BPM)。与其他类型的BPM相比,腔式BPM即使在低电荷水平下也具有更高的灵敏度和更快的响应时间。当电子束穿过腔式BPM时,它会激发腔的偶极模式,其幅度与束流相对于腔中心的偏移呈线性关系。通过示波器测量BPM的信号作为束流偏移的函数。KAERI太赫兹FEL的微回旋加速器产生能量为6.5 MeV、脉冲长度为5 μs、微脉冲为10 - 20 ps、频率为2.801 GHz的电子束。宏脉冲束流为40 mA。由于微回旋加速器提供多束团系统,输出信号将是每个单束团的叠加。因此,通过每个单束团的叠加可以获得高输出信号。腔式BPM在多束团中的设计位置分辨率为亚微米级。我们的腔式BPM由铝制成,通过铟密封可维持真空,无需钎焊工艺,从而易于改装并节省成本。腔式BPM的共振频率为2.803 GHz,腔式BPM尺寸为200×220 mm(长×高),管径为38 mm。测量的位置灵敏度为6.19(mV/mm)/mA,X轴和Y轴之间的测量隔离度为 - 39 dB。通过测量系统的热噪声,估计腔式BPM的位置分辨率小于1 μm。在本文中,我们展示了S波段腔式BPM的测试结果,并证明了使用该装置进行高分辨率束流位置测量的可行性。