TY - JOUR
T1 - Shot-by-shot characterization of focused X-ray free electron laser pulses
AU - Kobayashi, Amane
AU - Sekiguchi, Yuki
AU - Oroguchi, Tomotaka
AU - Yamamoto, Masaki
AU - Nakasako, Masayoshi
N1 - Funding Information:
The authors are grateful to Dr. Kensuke Tono, Dr. Yuichi Inubushi, Dr. Takashi Kameshima, and Dr. Yasumasa Joti of JASRI, and Mr. Tetsukon Kim, Mr. Takahiro Date, Mr. Toshiyuki Murakami and the other members of the Engineering Team of the SACLA for their help in the alignment of the optics, and our apparatus. This study was supported by the grant for XFEL key technology to M.N. and M.Y., and by the X-ray Free Electron Laser Priority Strategy Program from the Ministry of Education, Culture, Sports, Science and Technology (MEXT) to M.N. and M.Y. In addition, specimen preparation and software development are supported by the grants from the Japan Society for the Promotion of Science to M.N. (jp17654084, jp23120525, jp24654140, jp25120725, jp16H02218), to Y. S. (No. 15J01707) and to A.K. (No. 15J01831), and the grants from the MEXT to M.N. (Nos jp15076210, jp20050030) and to T.O. (No. 24113723). The XFEL-CXDI diffraction data for structure analyses were collected at SACLA (proposal Nos 2014A8033, 2014B8052 and 2015A8051, 2015B8049, 2016A8048, 2016B8064, and 2017A8015). Some calculations were performed using the mini-K supercomputer system at the SACLA facility.
Publisher Copyright:
© 2018 The Author(s).
PY - 2018/12/1
Y1 - 2018/12/1
N2 - X-ray free electron lasers (XFEL) provide intense and almost coherent X-ray pulses. They are used for various experiments investigating physical and chemical properties in materials and biological science because of their complete coherence, high intensity, and very short pulse width. In XFEL experiments, specimens are irradiated by XFEL pulses focused by mirror optics. The focused pulse is too intense to measure its coherence by placing an X-ray detector on the focal spot. Previously, a method was proposed for evaluating the coherence of focused pulses from the visibility of the diffraction intensity of colloidal particles by the speckle visibility spectroscopy (SVS). However, the visibility cannot be determined exactly because the diffraction intensity is integrated into each finite size detector pixel. Here, we propose a method to evaluate the coherence of each XFEL pulse by using SVS in combination with a theory for exact sampling of the diffraction pattern and a technique of multiplying the diffraction data by a Gaussian masks, which reduces the influence of data missing in small-angle regions due to the presence of a direct beamstop. We also introduce a method for characterizing the shot-by-shot size of each XFEL pulse by analysing the X-ray irradiated area.
AB - X-ray free electron lasers (XFEL) provide intense and almost coherent X-ray pulses. They are used for various experiments investigating physical and chemical properties in materials and biological science because of their complete coherence, high intensity, and very short pulse width. In XFEL experiments, specimens are irradiated by XFEL pulses focused by mirror optics. The focused pulse is too intense to measure its coherence by placing an X-ray detector on the focal spot. Previously, a method was proposed for evaluating the coherence of focused pulses from the visibility of the diffraction intensity of colloidal particles by the speckle visibility spectroscopy (SVS). However, the visibility cannot be determined exactly because the diffraction intensity is integrated into each finite size detector pixel. Here, we propose a method to evaluate the coherence of each XFEL pulse by using SVS in combination with a theory for exact sampling of the diffraction pattern and a technique of multiplying the diffraction data by a Gaussian masks, which reduces the influence of data missing in small-angle regions due to the presence of a direct beamstop. We also introduce a method for characterizing the shot-by-shot size of each XFEL pulse by analysing the X-ray irradiated area.
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U2 - 10.1038/s41598-018-19179-3
DO - 10.1038/s41598-018-19179-3
M3 - Article
C2 - 29339756
AN - SCOPUS:85040797576
SN - 2045-2322
VL - 8
JO - Scientific Reports
JF - Scientific Reports
IS - 1
M1 - 831
ER -