Setiniyaz Sadiq, Park Seong Hee, Kim Hyun Woo, Vinokurov Nikolay A, Jang Kyu-Ha, Lee Kitae, Baek In Hyung, Jeong Young Uk
Korea Atomic Energy Research Institute, 1045 Daedeok-Daero, Yuseong-gu, Daejeon 34057, South Korea.
Korea University, 2511 Sejong-ro, Sejong 30019, South Korea.
Rev Sci Instrum. 2017 Nov;88(11):113306. doi: 10.1063/1.5006550.
We describe a compact THz-pump and X-ray-probe beamline, based on an electron linac, for ultrafast time-resolved diffraction applications. Two high-energy electron (γ > 50) bunches, 5 ns apart, impinge upon a single-foil or multifoil radiator and generate THz radiation and X-rays simultaneously. The THz pulse from the first bunch is synchronized to the X-ray beam of the second bunch by using an adjustable optical delay of a THz pulse. The peak power of THz radiation from the multifoil radiator is estimated to be 0.14 GW for a 200 pC well-optimized electron bunch. GEANT4 simulations show that a carbon foil with a thickness of 0.5-1.0 mm has the highest yield of 10-20 keV hard X-rays for a 25 MeV beam, which is approximately 10 photons/(keV pC-electrons) within a few degrees of the polar angle. A carbon multifoil radiator with 35 foils (25 μm thick each) can generate close to 10 hard X-rays/(keV pC-electrons) within a 2° acceptance angle. With 200 pC charge and a 100 Hz repetition rate, we can generate 10 X-rays per 1 keV energy bin per second or 10 X-rays per 1 keV energy bin per pulse. The longitudinal time profile of an X-ray pulse ranges from 400 to 600 fs depending on the acceptance angle. The broadening of the time duration of an X-ray pulse is observed owing to its diverging effect. A double-crystal monochromator will be used to select and transport the desired X-rays to the sample. The heating of the radiators by an electron beam is negligible because of the low beam current.
我们描述了一种基于电子直线加速器的紧凑型太赫兹泵浦和X射线探测光束线,用于超快时间分辨衍射应用。两个高能电子(γ>50)束团,相隔5 ns,撞击单箔或多箔辐射器,同时产生太赫兹辐射和X射线。通过使用太赫兹脉冲的可调光学延迟,将第一束团产生的太赫兹脉冲与第二束团的X射线束同步。对于200 pC优化良好的电子束团,多箔辐射器产生的太赫兹辐射峰值功率估计为0.14 GW。GEANT4模拟表明,对于25 MeV的束流,厚度为0.5-1.0 mm的碳箔产生10-20 keV硬X射线的产额最高,在极角几度范围内约为10个光子/(keV pC电子)。具有35个箔片(每个箔片厚25μm)的碳多箔辐射器在2°接受角内可产生接近10个硬X射线/(keV pC电子)。在200 pC电荷和100 Hz重复频率下,我们每秒可在每个1 keV能量区间产生10个X射线,或每个脉冲在每个1 keV能量区间产生10个X射线。X射线脉冲的纵向时间分布范围为400至600 fs,具体取决于接受角。由于其发散效应,观察到X射线脉冲持续时间变宽。将使用双晶单色仪选择并将所需的X射线传输到样品。由于束流电流较低,电子束对辐射器的加热可忽略不计。