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IInnddeexx
Welcome 2
Committees 4
Program 5
Sponsors and Exhibitors 9
Author Index 10
Presentations
Orals 14
Posters 43
AOFSRR Shuttle Bus 102
1
2
WWeellccoommee Welcome to the 4th AOFSRR workshop in Shanghai, China! It is our honor to host the fourth Asia Oceania Forum on Synchrotron Radiation Research. The workshop will be held along with the first Users Meeting of Shanghai Synchrotron Radiation Facility, which is to be held on November 28 and 29; therefore, you are also welcome to attend the users meeting. We would like to express our heartfelt appreciation to the council members and committees of AOFSRR, and all the sponsors for helping us to make a successful workshop. For this workshop, we will have the delegates from Japan, Korea, Australia, Singapore Taiwan Hongkong, India, Thailand, Malaysia, New Zealand, Vietnam and mainland China. We believe that it is a great opportunity for participants to exchange the latest developments, to discuss future directions for
synchrotron radiation research and to broaden the collaborations among facilities and regions. It is also a special opportunity for Shanghai Synchrotron Radiation Facility, which has just started its operation this year. The success of SSRF construction itself is a good example of international cooperation. We believe that the future of SSRF will still be benefited from the collaboration and we hope to contribute to the regional collaboration as well. We feel happy that you have chosen to join us for the workshop. We wish that your experiences at 4th AOFSRR will be beneficial to your research and wish you a very pleasant stay in Shanghai. Professor Hongjie Xu Director, Shanghai Synchrotron Radiation Facility
WWeellccoommee On behalf of the Council of AOFSRR, I would like to welcome all of you to the 2009 Workshop in Shanghai. As we all have witnessed, following the fast economic growth in the region in the last 20 years, many synchrotrons, ranging from first- to fourth-generation machines, have been built in the Asia-Oceania region. This makes synchrotron facilities among the most visible major scientific developments in the region. The AOFSRR was first established in November 2006 at KEK with eight members, each having synchrotron facilities Australia, China, India, Korea, Japan, Singapore, Taiwan, and Thailand. The charge of the organization is to
promote collaboration between the facilities and user communities in the Asia-Oceania region. At this years workshop, we are especially delighted to welcome New Zealand, Malaysia, and Vietnam to join as associate members. Through the workshop, we hope to achieve increase in inter-facility cooperation and scientific collaboration. We welcome you to Shanghai and wish for a very successful two-day meeting. Keng S. Liang Council President, AOFSRR
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Council committee President: Keng S. Liang Secretary-General:
Masaki Takata Vice president:
Moonhor Ree Past president:
Yoshiyuki Amemiya Treasurer: Robert Lamb Secretary-Treasure:
Richard Garrett Special Advisor of President:
Osamu Shimomura Member: Hongjie Xu Member: V.C.Sahni Member: Weerapong Pairswan Member: Herbert O. Moser Member: Masaharu Oshima
Organizing committee Chair: Hongjie Xu Secretaty: Renzhong Tai Member: Keng S. Liang Member: Moonhor Ree Member: Robert Lamb Member: Masaharu Oshima Member: V.C.Sahni Member: Weerapong Pairswan Member: Herber O. Moser Member: Xiaoming Jiang Member: Ziyu Wu Member: Masaki Takata Member: Richard Garrett Member: Osamu Shimomura Program committee Chair: Jianhua He Member: Keng S. Liang Member: Yaw-Wen Yang Member: Kyung Jin Kim Member: Jung Nam Hwang Member: Kilwon Cho Member: Masaki Takata Member: Ian Gentle Member: Caozheng Diao Member: Yangchao Tian Member: Nobuhiro Kosugi Member: Soichi Wakatsuki Member: Tiandou Hu
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The 4th AOFSRR Program (Nov. 30 Dec. 1, 2009)
NOV. 30, 2009
OPENING
9:00-9:40
Welcome Address
Chair: Hongjie Xu
The Vice President, Chinese Academy of Sciences, China
The Vice President, Prof. Wenqing Shen, National Natural Science Foundation of China (NSFC), China
The Vice director, Mr. Qianghua Shi, Science and Technology Commission of Shanghai Municipality, China
Mr. Hiroki Takaya Director, the office of Synchrotron Radiation Research, Ministry of Education, Culture, Sports, Science & Technology (MEXT), Japan
Prof. Zhentang Zhao Deputy Director of Shanghai Synchrotron Radiation Facility Director of Shanghai Institute of Applied Physics
9:40-12:20
I. Recent Progress and Future Plan of SR Activitiesin AO Region-I
Chair: Moonhor Ree
9:40-10:00 Overview of AOF Activities K. Liang, NSRRC
10:00-10:20 Current Status of SSRF Hongjie Xu, SINAP,CAS
10:20-10:40 Present Status of BSRF Yuhui Dong, IHEP, CAS 10:40-11:20 Group photo and coffee break
Chair: Jianhua He
11:20-11:40 NSRL and its applications facing the quantum control age Ziyu Wu, NSRL
11:40-12:00 Shanghai SXFEL Project Zhentang Zhao, SINAP, CAS
12:00-12:20 The Science Plan of TPS Di-Jing Huang, NSRRC
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12:20-14:00 Lunch & Poster Session
Scientific Poster; Facility Poster
14:00-16:50
II. Recent Progress in SR-based Science and Techniques-I
Chair: Di-Jing Huang
14:00-14:30 IR and THz Sciences at UVSOR-II Shinichi Kimura, UVSOR, Japan
14:30-15:00 Application of VUV Synchrotron Radiation in Chemical Dynamics Research Xueming Yang, Dalian Institute of Chemical Physics, CAS
15:00-15:30 Anisotropic electrical conductivity of PdCoO2 studied by angle-resolved photoemission spectroscopy Hyeong-Do Kim, PAL, Korea
15:30-15:50 Coffee Break
Chair: Renzhong Tai
15:50-16:20 Electronic structure of unusual charge and spin density waves Donglai Feng, Fudan University, China
16:20-16:50 Structure and Ferroelectric Behavior of BiFeO3 (001) Thin Film Ping Yang , Singapore Light Source, Singapore
16:50-17:50
III. Recent Progress and Future Plan of SR Facilities
in AO Region-II
Chair: Osamu Shimomura
16:50-17:10 XFEL project at SPring-8 Takashi Tanaka, RIKEN SPring-8 Center, Japan
17:10-17:30 Status of PLS-II Upgrade and Korean XFEL Kyung-Ryul Kim, PAL,Korea
17:30-17:50 Present Status of the Siam Photon Laboratory Prayoon Songsiriritthigul, SLRI ,Thailand
18:00 Banquet
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Dec. 1st
8:30-11:50
IV. Recent Progress in SR-based Science and Techniques-II
Chair: Yoshiyuki Amemiya
8:30-9:00 Synchrotron X-rays in quest of new horizons in the protein universe Soichi Wakatsuki ,PF, Japan
9:00-9:30 Structure and Mechanism of an Amino Acid Antiporter Yigong Shi, Qinghua University, China
9:30-10:00 The development of X-ray microscopy for biomedical applications Yeukuang Hwu, NSRRC
10:00-10:20 Coffee Break
Chair: Ian Gentle
10:20-10:50
The advanced SR structural materials science utilizing novel measuring and data analysis technique. - From nano science to pharmaceutical chemistry Makoto Sakata, Japan Science & Technology Agency
10:50-11:20 Megapixels per hour: fast fluorescence imaging at the Australian Synchrotron David Paterson, Australian Synchrotron
11:20-11:50 Fast switching of circular polarization using APPLE-II type undulators Kenta AmemiyaPFJapan
11:50-12:50 A Tour of SSRF
12:50-14:30 Lunch & Poster Session Scientific Poster, Facility Poster
14:30-15:30
V. Promotion of the SR Activities in AO Region-I
Chair: Richard Garrett The Activities in the Associate Members 1) New Zealand (15min.)
Richard Haverkamp, Massey University, New Zealand 2) Malaysia (15min.)
Swee Ping Chia, University of Malaya 3) Vietnam (15min.)
Tran Duc Thiep, Vietnam Academy of Science and Technology
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4) Discussion for alliance between the members (15min.) 15:30-15:50 Coffee Break
15:50-16:40
VI. Promotion of the SR Activities in AO Region-II
Chair: K. Liang
15:50-16:10 Inter-facility Cooperation. Richard Garrett, ANSTO, Australia
16:10-16:40
Cheiron School Report 1) Cheiron School 2009 (20min.)
Masaki Takata, JASRI/SPring-8, Japan 2) Students Reports (10min.)
Jingyuan Ma, SSRF, China Somchai Tancharakorn, SLRI, Thailand
16:40-17:30
Remarks & Closing
Chair: Masaki Takata
16:40-17:00 Council Report & Discussion K. Liang, NSRRC
17:00-17:15 AOFSRR2010 Moonhor Ree, POSTECH, Korea
17:15-17:30 Closing Remarks Hongjie Xu, SINAP, CAS
17:40 Back to hotel
Dec. 2rd
Excursion to Suzhou
Detailed information is available on the webpage:
http://www.sinap.ac.cn/aof2009/
8
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AAuutthhoorr IInnddeexx Ahn, Byungcheol 54, 56, 57, 58, 59, 60, 61, 62, 63, 64, 66, 67, 71 Amemiya, Kenta 20 Bao, Liangman 74 Bian, Fenggang 53 Bian, Feng-Gang 37 Bottjer, David J. 72 Byun, Gwang-su 66 Cai, Zhonghou 70 Chang, Chien-Hung 45 Chang, Shih-Lin 45 Chang, Taihyun 62 Chen, Hsin-Lung 45 Chen, J. M. 55 Chen, Jiahua 48, 38 Chen, Jun-Yuan 72 Chen, Min 38, 48 Chen, Ming 43 Chen, Ming-Chou 69 Chen, Mingzhi 52 Chen, Rongchang 49 Chen, S. A. 55 Cheng, Yung-Chiuan 69 Chia, Swee-Ping 24 Cho, En-Jin 9 Choi, Junman 54, 56, 57, 58, 59, 60, 62, 63, 64, 66, 67, 71 Chou, T. L. 55 Chuang, W. T. 55 Chun, M. H. 27 Davidson, Eric H. 72 Deng, Biao 49 Dong, Yuhui 3 Du, Guohao 49, 73 Du, Yonghua 11 Duangnil, S. 14
Fan, Liang-Jen 69 Feng, Chao 32 Feng, Dong-Lai 10 Feng, Guangyao 34 Fu, Yuan 36, 51
Gao, Mei 47 Gao, Xiang 16 Garrett, Richard F. 21 Gong, Pei-rong 41, 42 Gu, Songqi 51 Guo, Zhi 48 Hadfield, Michael G. 72 Haverkamp, Richard 23 Hayakawa, Teruaki 54 He, Jianhua 52 He, Qing 47 Heo, Kyuyoung 58, 62, 64, 71 Hirai, Tomoyasu 54 Hiraoka, N. 55 Howarda, D. L. 19 Hsw, S. A. 55 Hu, Chun 39, 41 Hua, Wei 52 Huai, Ping 68 Huang, Chi-Yi 45 Huang, Di-Jing 6 Huang, Sheng 52 Huang, Wei 75 Huang, Yu-Shan 45 Huang, Yuying 51, 75 Hwang, Ilmoon 30 Hwu, Yeukuang 17, 70 Ishii, H. 55 Jeong, Jinhwan 9 Jeong, Jinwon 9 Jiang, Zheng 51, 75 Jin, Kyeong 71 Jin, Kyeong Sik 58, 62, 67 Jin, Sangwoo 54, 56, 57, 58, 59, 60, 61, 62, 63, 64, 66, 67, 71 Jongea, M. D. de 19 Jung, Jungwoon 54, 56, 57, 58, 59, 60, 61, 62, 63, 64, 66, 67, 71 Jung, Sungmin 54, 56, 57, 58, 59, 60, 62, 63, 64, 66, 67, 71 Kakizaki, Akito 46 Kawata, Hiroshi 26
Ke, Ming 40 Kim, D.T. 29 Kim, Dong Min 54, 56, 57, 58, 59, 60, 61, 62, 63, 64, 66, 67, 71 Kim, Gahee 64, 71 Kim, Hyeong-Do 9 Kim, J. M. 28 Kim, Jae-Hong 67 Kim, Jehan 62 Kim, Jin Chul 54, 56, 57, 58, 59, 60, 61, 62, 63, 64, 66, 67, 71 Kim, K. R. 27, 28, 29, 31 Kim, Kwang-Woo 62 Kim, Kyoo 9 Kim, Kyung-Ryul 13 Kim, Kyungtae 54, 56, 57, 58, 59, 60, 61, 63, 64, 66, 67, 71 Kim, Mihee 54, 56, 57, 58, 59, 60, 61, 62, 63, 64, 66, 67, 71 Kim, SikHyun Chul 71 Kim, Sung Baek 9 Kimura, Shin-ichi 7 Kirkhamb, R. 19 Klysubun, P. 14 Ko, Yong-Gi 54, 56, 57, 58, 59, 60, 61, 62, 63, 64, 66, 67, 71 Kwon, Wonsang 54, 56, 57, 58, 59, 60, 61, 62, 63, 64, 66, 67, 71 Lai, Barry 70 Lee, Chih-Hao 45 Lee, E.H. 2829 Lee, J. F. 55 Lee, J. M. 55 Lee, J. W. 27282931 Lee, Taek Joon 54565758596061626364666771 Li, A.G. 50 Li, Gang 72 Li, J. 50 Li, Jun 65 Li, Tingju 65 Li, weimin 34 Li, Xiaochun 16 Li, Xiuhong 53
Li, Yan 7074 Li, Yulan 70 LI, Zhong 39, 4147 Liang, Feng 70 Liang, Keng S. 1 Lin, C. M. 55 Lin, Jun 74 Lin, Tsang-Lang 45 Liu, Huajun 11 Liu, Ke 52 Liu, Ping 39 Liu, Shi-Lei 37 Liu, Wei 74 Liu, Yi 53 Lu, Feiran 16 Lu, Jie 33 Lu, K. T. 55 LU, Qipeng 38 Luo, Hongxin35 Ma, Jingyuan 25A51 Maeda, Rina 54 Mao, C.W. 50 Mi, Qingru 39 Min, B. I. 9 Nam, N. S. 31 Noh, Han-Jin 9 Okajima, Toshihiro 44 Oshima, Masaharu 46 Ozaki, Yukihiro 58 Pairsuwan, W. 14 Park, B.R. 27 Park, H. G. 31 Park, Joon Kyu 67 Park, S. J. 27282931 Park, Samdae 54565758596061626364666771 Paterson, D. 19
Peng, Wen-Yan 45 Peng, Zhongqi 38 Qing, Xiang-yun 41 Ree, Moonhor 5456575859606162636465666771 Rho, Yecheol 545657585960616263646771 Ryanb, C. G. 19
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Sakata, Makoto 18 Sato, Harumi 58 Shen, Da-Wei 10 Sheu, H.-S. 55 Shi, Yigong 16 Siddonsc, D. P. 19 Songsiriritthigul, P. 14 Sun, Bo 52 Sun, Peijian 68 Tafforeau, Paul 72 Tai, Renzhong 3848 Tan, Mingguang 70 Tanaka, Takashi 12 Tancharakorn, Somchai 25B Tang, Lin 52 Tang, Mau-Tsu 45 Thiep, Tran Duc 22 Tong, Yajun 49 Tsuei, K. D. 55 Wakatsuki, Soichi 15 Wang, Chia-Hsin 69 Wang, Hongfei 33, 50 Wang, Jiawei 16 Wang, Jie 355340 Wang, John 11 Wang, Lin 34 Wang, Mouhua 73 Wang, Na-Xiu 37 Wang, Qisheng 52 Wang, Sisheng 47 Wang, Tongmin 65 Wang, Yong 3848 Wang, Yu 52 Wang, Yuzhu 53 Wei, Xiangjun 51 Wei, Zhi-hua 41 Wen, Wen 47 Wu, Guanyuan 43 Wu, Guozhong 7375 Wu, Yanqing 3848 Wu, Yingfeng 39 Wu, Ziyu 434 Xia, Shaojian 51 Xian, Ding-Chang 72
Xiao, Tiqiao 3565, 73 Xiao, Xianghui 70 Xiao, Tiqiao 49 Xie, Honglan 49, 73 Xing, Zhe 73 Xu, Chunyan 52 Xu, Gongliang 34 Xu, Hongjie 24849515375 Xu, Jian 70
Xu, Jingjing 65 Xu, Zhong-Min 37 Xue, Bing 68 Xue, Song 363840, 48 Xue, Yanling 49 Yan, Chonghuai 70 Yan, F. 50 Yan, Rui 48 Yan, S. 50 Yang, K. 50 Yang, Le-Xian 10 Yang, P. 11 Yang, Xueming 8 Yang, Yaw-Wen 69 Yoon, J. C. 31 Yoon, Jinhwan 54586271 Yu, Chenghao 40 Yu, Feng 52 Yu, Xiaohan 50, 51 Zhang, Chuanfu 70 Zhang, Guilin 70 Zhang, Min 43 Zhang, Shuo 51 Zhang, Wei 3368 Zhang, Yan 10 Zhang, Zhao-hong 39, 41 Zhang, shancai 34 Zhao, Z. T. 5 Zhao, Zhentang 232 Zhen, Xiangjun 48 Zheng, Lifang 39 Zhou, Jian-ying 41 Zhou, Lijun 16 Zhou, Qiaogen 33 Zhou, Xiang 52
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13
Zhou, Xingtai 47 Zhu, Wanqian 3649 Zhu, Z.X. 42 Zhu, Zhiyuan 68 Zou, Yang 5175
14
Orals
01 4th AOFSRR
Overview of AOF Activities
Keng S. Liang
NSRRC, Hsinchu, Taiwan
In view of the increased activities of synchrotron facility developments and synchrotron
radiation research in the Asia Oceania region, the Asia Oceania Forum of Synchrotron
Radiation Research was established in November 2006 at KEK under the initiation of
Japanese Society for Synchrotron Radiation Research (JASRR). Currently the AOFSRR
includes eight regional members with each having its own synchrotron facilities in operation
(Australia, China, India, Korea, Japan, Singapore, Taiwan, and Thailand) and three associate
members (New Zealand, Malaysia, and Vietnam). The AOFSRR has sponsored two major
annual events: the workshop and the Cheiron School. The first workshop was held in Tsukuba
in November 2006, followed by the second at Hsinchu in 2007, the third at Melbourne in
2008, and the 4th one of this meeting. The Cheiron School, starting with first one in
September 2007, has been held at SPring-8 each year for 10 days since. Each School was
attended by 60 to 70 students and young researchers from the region. Both the annual
workshop and the Cheiron School serve the purpose in promoting networking of synchrotron
researchers, the collaboration among synchrotron facilities, and the nurturing of young
generation of synchrotron users through out the region. In this talk, I will give a short history
and an overview of the AOFSRR activities of the last few years.
15
02 4th AOFSRR
Current Status of Shanghai Synchrotron Radiation Facility
Hongjie Xu and Zhentang Zhao Shanghai Synchrotron Radiation Facility, Shanghai Institute of Applied Physics, Chinese
Academy of Sciences, Shanghai 201800, China
The Shanghai Synchrotron Radiation Facility (SSRF) is a third generation light source of
3.5GeV electron energy, aimed at producing very brilliant X-ray and soft X-ray beams to
facilitate the researches in life science, material science, earth and environmental sciences,
and many other fields. The construction of SSRF started in December of 2004 and was
completed by the end of April 2009. During the commissioning stage, the technical
parameters of accelerators and beamlines were measured systematically with the conclusion
that all the design specifications have been met. The test user operation of SSRF started in
May of 2009 and more than 2000 hours user beamtime has been scheduled for this year.
At present, seven beamlines have been built on SSRF as the phase I beamlines and are all in
operation now:
Macromolecular Crystallography Beamline
X-ray Diffraction Beamline
X-ray Absorption Fine Structure Beamline
Hard X-ray Micro-focusing Beamline
X-ray Imaging and Biomedical Applications Beamline
Soft X-ray Spectromicroscopy Beamline
Small Angle X-ray Scattering Beamline
Two calls for user proposals were made in this year and about 570 proposals were received.
Hundreds of users have come to SSRF for experiments and lots of interesting results are
expected.
16
In this talk, an overview of the construction and the commissioning of SSRF will be
introduced. Some representative experimental results obtained since the operation will be
shown and the future beamline programs will be introduced as well.
17
03 4th AOFSRR
Present Status of BSRF Yuhui Dong
Beijing Synchrotron Radiation Facility, Institute of High Energy Physics, Chinese Academy of Sciences
19B Yuquan Road, Beijing 100049, China Email: [email protected]
BSRF was in commissioning from 1991. After about 20 years of development, there are
14 beamlines and end-stations. Although the accelerator of BSRF is a parasitic machine,
BSRF still provide 2000 hours of beamtime; arrange 300 proposals and 1000 user for
expeiments per year.
The beamlines of BSRF cover the fields of condensed matter physics, chemistry, biology,
environment, geology, and materials sciences. Due to the huge numbers of research teams
around Beijing, many important and interesting researches archive great success in BSRF.
Due to the unexpectedly high speed of the growth in the numbers of research teams and
the funding from government in China in the recent years, BSRF will still keep the position
for supporting the frontier research of the scientists in China, especially around Beijing. Now
BSRF plans to improve the commissioning in order to provide more support for the research
teams around Beijing. These improvements include parasitic mode commissioning for more
beamtime, in situ experimental environment for real time studies, new experimental
techniques for frontier research. We believe BSRF, and also the other two synchrotron
radiation facilities in China, SSRF and NSRL, will provide better supporting for the scientific
research of all of the groups in China in the future.
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04 4th AOFSRR
NSRL and its Application -- Facing the Quantum Age Ziyu Wu
National Synchrotron Radiation Laboratory
University of Science and Technology of China
Email: [email protected]
As the first dedicated VUV synchrotron radiation facility in China, the construction of the
National Synchrotron Radiation Laboratory (NSRL) started in 1984 and the Phase II Project
was carried out in the period 1999-2004. It recently celebrated its 20 anniversaries after the
first synchrotron radiation light observation and since then it hosted more then 2000 users.
NSRL is based on a 200 MeV Linac that is the injector, a transport line, an 800 MeV
electron storage ring hosting 14 beamlines and end-stations covering a wide energy range
from the infrared through the x-ray region. The domestic community performed hundreds of
experiments in many disciplines ranging from physics to chemistry, biology, life sciences,
material sciences, surface sciences, metrology, medicine, microscopy and imaging, detectors,
instrumentation, etc..
Nowadays, to face up new experimental demands and the coming of the quantum age,
NSRL is planning in the next three years an important upgrade project. After that, new
research opportunities for the investigations of quantum systems and in modern researches
regarding cell imaging, surface interactions and interfaces, combustion processes, energy and
environmental science, water, as well as the generation of coherent sources in the THz and IR
domain will be available thanks to the designed high brilliance and low emittance.
As a national user-oriented large-scale scientific infrastructure supported by the National
science foundations, NSRL enthusiastically welcome scientists from all disciplines interested
to carry out their state-of-the-art researches in our facility.
19
05 4th AOFSRR
Shanghai Soft X-Ray Free Electron Laser Test Facility
Z. T. Zhao for the SXFEL Project Team
Shanghai Institute of Applied Physics, Chinese Academy of Sciences
As a development step towards constructing a hard X-ray FEL in China, a soft X-ray FEL
test facility (SXFEL) was proposed and will be constructed in Shanghai by a joint team of
Institute of High Energy Physics, Tsinghua University and Shanghai Institute of Applied
Physics. This test facility, based on an 840MeV S-band electron linear accelerator, aims at
generating 9nm FEL radiation with two-stage cascaded HGHG scheme. This presentation
reports the preliminary design of this Chinese soft X-ray test facility and the R&D progress of
the key FEL technologies in the SDUV-FEL test bench.
20
06 4th AOFSRR
The Science Plan of TPS Di-Jing Huang, NSRRC
21
07 4th AOFSRR
IR and THz Sciences at UVSOR-II
Shin-ichi Kimura UVSOR Facility, Institute for Molecular Science, Okazaki 444-8585, Japan
Synchrotron radiation is a powerful light source not only in the x-ray and VUV regions but
also in the IR and THz regions because of the high brilliance. At UVSOR, the IR/THz
beamline firstly dedicated to users in the world has been constructed about 25 years ago.
Recently, the IR/THz beamline was reconstructed and the acceptance angle was expanded to
215 (H) 90 (V) mrad2 by using a three-dimensional magic mirror, which is a perfect
focusing mirror for a circular trajectory [1]. Due to the improvement, unexplored IR and THz
spectroscopies, for instance THz spectroscopy under extreme conditions, became available. In
addition, intense coherent THz radiation and VUV coherent harmonic generation produced by
the interaction between the electron beam in the storage ring and a pulse laser are studied at
UVSOR-II. Since these lights originate from the same electron bunch, these lights are
perfectly synchronized with each other. The property is useful for pump probe experiments.
Then we plan to perform a THz pump PES probe experiment using the coherent THz and
VUV lights. In this talk, we discuss sciences using the present IR/THz beamline and prospects
using the intense coherent THz radiation.
References:
[1] S. Kimura, E. Nakamura, T. Nishi, Y. Sakurai, K. Hayashi, J. Yamazaki, and M. Katoh,
Infrared Phys. Tech. 49, 147 (2006).
22
08 4th AOFSRR
Application of VUV Synchrotron Radiation in Chemical
Dynamics Research
Xueming Yang State Key Laboratory of Molecular Reaction Dynamics
Dalian Institute of Chemical Physics, Chinese Academy of Sciences
In this talk, a brief overview of the VUV synchrotron applications in the chemical
dynamics research will be provided. Strong and tunable VUV light sources are very useful
in the detection of radical and exotic species in chemical processes. In the last ten years, we
have been involved in using VUV synchrotron radiation to investigate the dynamics of
molecular photodissociation and crossed beams reactions. New experimental tools have
been developed in this area. In this work, I will give a few examples to show the advantages
of using VUV light source to investigate the fundamental mechanisms of chemical reactions.
23
09 4th AOFSRR
Anisotropic electrical conductivity of PdCoO2 studied by
angle-resolved photoemission spectroscopy
Hyeong-Do Kim,1 Han-Jin Noh,2 Jinwon Jeong,2 Jinhwan Jeong,2
En-Jin Cho,2 Sung Baek Kim,2 Kyoo Kim,4 and B. I. Min4 1Pohang Accelerator Laboratory, POSTECH, Pohang 790-784, Korea
2Department of Physics, Chonnam National University, Gwangju 500-757, Korea 3Laboratory of Pohang Emergent Materials and Department of Physics, POSTECH,
Pohang 790-784, Korea 4Department of Physics, POSTECH, Pohang 790-784, Korea
An explicit connection between the electronic structure and the anisotropic high
conductivity of delafossite-type PdCoO2 has been established by angle-resolved
photoemission spectroscopy (ARPES), core-level x-ray photoemission spectroscopy, and
x-ray absorption spectroscopy. The ARPES spectra show that a large hexagonal electronlike
Fermi surface (FS) consists of very dispersive Pd 4d states. The carrier velocity and lifetime
are determined from the ARPES data, and the conductivity is calculated by a solution of the
Boltzmann equation, which demonstrates that the high anisotropic conductivity originates
from the high carrier velocity, the large two-dimensional FS, and the long lifetime of the
carriers.
24
10 4th AOFSRR
Electronic structure of unusual charge and spin density waves
Dong-Lai Feng, Yan Zhang, Le-Xian Yang, Da-Wei Shen
Department of Physics and Laboratory of Advanced Materials, Fudan University, Shanghai, 200433, P. R. China
Charge and spin density waves (CDW and SDW) are two basic forms of order in solids.
In our study of various density wave systems, we found their microscopic mechanisms are
often unconventional. In this talk I will give several examples about the rich and anomalous
density waves in complex materials.
The transition metal dichalcogenides with 2H structure is the first system in which two
dimensional CDW was discovered. However it had puzzled people for nearly 30 years that it
cannot be explained by either the Fermi surface nesting scenario, or the saddle point scenario.
We measured the electronic structure of 2H-NaxTaS2 [1] and NbSe2 [2] and proved that the
CDW is not related to the Fermi surface but to the Fermi patch region all over the Brillion
zone. This new mechanism could explain the charge instability in many strongly coupled
systems.
Similar to the cuprate, both superconducting and magnetically ordered phases appear in the
phase diagram of the newly discovered iron pnictides. We find that the itinerant SDW order in
materials such as BaFe2As2 the SDW is caused by the band splitting [3], instead of Fermi
surface nesting; moreover the coexistence of superconductivity and SDW is discovered in
Sr0.82K0.18Fe2As2 [4].
References:
[1] D. W. Shen et al. Phys. Rev. Lett. 99, 216404 (2007),
[2] D. W. Shen et al. Phys. Rev. Lett. 101,226406 (2008),
[3] L. X. Yang et al. Phys. Rev. Lett. 102, 107002 (2009),
[4] Y. Zhang et al. Phys. Rev. Lett.102 (2009) 127003.
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11 4th AOFSRR
Structure and Ferroelectric Behavior of BiFeO3 (001) Thin Film
P. Yang Singapore Synchrotron Light Source (SSLS), National University of Singapore
5 Research Link, Singapore 117603
LIU Huajun and John Wang Department of Materials Science and Engineering, National University of Singapore
Singapore 117574
DU Yonghua Institute of Chemical and Engineering Sciences (ICES)
1 Pesek Road, Jurong Island, Singapore 627833
Bismuth ferrite (BiFeO3) is perhaps the only material that is both magnetic and strong
ferroelectric at room temperature. It has significant impact in the field of multiferroic
materials, which simultaneously shows ferroelectricity, ferromagnetism, and ferroelasticity,
with promising applications in data storage, the new generation of sensors and actuators, and
spintronic devices. Indeed, hundreds of papers have been published in this area in recent years
[1]. Especially, the mechanism of coexistence of ferroelectricity and magnetism has drawn
great attention from researchers, as it is different from traditional ferroelectric materials and it
will also show indications to design new multiferroic materials. Structure-correlated origin or
mechanism of ferro-electricity in Bismuth Ferrite (BiFeO3, BFO) films is studied using
high-resolution X-ray diffractometry (HR-XRD) and XAFS (X-ray Absorption Fine
Structure).
A twinning rotation structure is revealed by reciprocal space mappings (RSMs) obtained
from synchrotron radiation HR-XRD [2] for the epitaxial BFO thin film that was grown on
(001) SrTiO3 substrate. The lattice strain is not fully relaxed at a film thickness of 720 nm.
The structure is indexed as a monoclinic with lattice parameters a = 5.610 , b = 5.529 , c =
4.031 and = 89.34. The twinning rotation leads to an enhanced remanent polarization
(2Pr = 163.5C/cm2, 2Ec = 509.5 kV/cm) and greatly reduced leakage current density of 1.2
26
10-6 A/cm2 at 100 kV/cm [3].
XAFS offers the coordination info for local structures around the cations Bi and Fe.
Possible correlations between the microscopic distortion in crystal structure and macroscopic
remanent polarization would be established.
Besides, structure change on growth condition is outlined.
Based on the understanding of the ferroelectricity and magnetism in BFO, we would be
able to design a structure which could simultaneously enhance both of ferro-electricity and a
strong magneto-electric coupling.
References:
G. Catalan and J.F. Scott, Advanced Materials, 21, 2463, (2009)
P. Yang and H.O. Moser, Advances in Synchrotron Radiation, 1, 105, (2008).
Huajun Liu, P. Yang, Kui Yao and John Wang, Appl. Phys. Lett., submitted.
27
12 4th AOFSRR
XFEL project at SPring-8 Takashi Tanaka, RIKEN SPring-8 Center, Japan
An x-ray free electron laser (XFEL) facility is under construction at the SPring-8 site,
which aims at lasing in the angstrom region in 2011. The civil construction has been
completed in April this year and accelerator components such as C-band accelerator cavities,
electron beam monitors, power supplies, undulatos, are being installed. In this talk, an
overview of the facility and construction status are reported together with the results of the
prototype accelerator operated at the electron energy of 250 MeV and lasing wavelength from
50 nm to 60 nm.
28
13 4th AOFSRR
Status of PLS-II Upgrade and Korean XFEL Kyung-Ryul Kim, on behalf of PLS-II Project Teams of PAL
Pohang Accelerator Laboratory, POSTECH, Pohang Korea, 790-784
The 2.5 GeV Pohang Light Source (PLS) at the Pohang Accelerator Laboratory has been
successfully operated with a total of 27 beamlines installed and 3 beamlines under
construction, in which 6 insertion devices such as undulators and multipole wigglers have
been put into operation to produce special photon beams. Nowadays, Korea synchrotron
users community is demanding higher beam stability and photon energies through the
installation of more insertion devices in the PLS. The PLS-II upgrade program has been
formerly launched in January 2009, incorporating new achromatic version of Double Bend
Achromat (DBA) to allow almost twice as many straight sections of the current PLS with a
design goal of the relatively low emittance of 5.9 nmrad. In the PLS-II, the top-up injection
using full energy injector linac of 3.0 GeV beam energy is planned for much higher stable
beam as well, and thus the production of hard x-ray undulator radiation of 8 to 13 keV is
anticipated to allow for the successful research program namely Protein Crystallography. The
PLS-II machine components of storage ring, linear accelerator and photon beamlines will be
partly dismantled and reinstalled in an 6-months shutdown beginning January 2011, and then
be started the initial commissioning with a 100 mA beam current from July 2011. And PAL
has also proposed the Korean new light source of linac-based X-ray Free Electron Laser
(XFEL) to produce an intense X-ray pulse down to a 0.1 nm wavelength with a 100 fs rms
pulse length. The in-vacuum undulator with a 5.3 mm gap is employed in combination with
an S-band RF linear accelerator to produce a 10.053 GeV electron beam. In this report, the
PLS-II upgrade and XFEL status will be done with a focus on the basic design results and
project implementation plans.
29
14 4th AOFSRR
Present Status of the Siam Photon Laboratory
P. Songsiriritthigul1,2*, P. Klysubun1, S. Duangnil1 and W. Pairsuwan1
1 Synchrotron Light Research Institute, P.O. Box 93, Muang, Nakhon Ratchasima 30000, Thailand 2 School of Physics, Suranaree University of Technology, Muang, Nakhon Ratchasima 30000, Thailand
The current status and future plan of the Siam Photon Laboratory (SPL) will be reported. The
Siam Photon Source has been in routine operation since 2005. The light source has been
continuously upgraded. The energy of stored electrons upgraded from 1.0 GeV to 1.2 GeV. At
present, the beam lifetime is 23 hours at 100 mA. A plannar undulator has been installed and
being commissioned. A 6.4-T WLS will be installed in the beginning of 2009. The light
source has 8 beam channels. Two beamlines for XAS and deep X-ray lithography are in
operation. Two more beamlines for spectromicroscopy/PEEM and SAXS beamlines are in the
commissioning phase. A WLS beamline for macromolecule crystallography is being installed.
An IR microspectrocopy beamline and an additional XAS beamline are in the design phase.
Recently, an energy dispersive monochromator beamline and a normal-incidence
monochromator beamline were relocated from the University of Bonn, Germany, to be
installed at SPL soon. This report will include the development of in-house technical
capabilities and the utilities improvement at the facility.
Keywords: synchrotron light source, beamline
Corresponding author: Prayoon Songsiriritthigul
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15 4th AOFSRR
Synchrotron X-rays in quest of new horizons in the protein
universe Soichi Wakatsuki, Photon Factory, IMSS, KEK, Tsukuba, Japan
X-ray protein crystallography with high brilliance and tuneability of synchrotron
radiation X-ray beams has been a method of choice for structural biology for the last two
decades. A number of new synchrotron sources, medium to large scales with low emittance
have been constructed and are being constructed while well established SR sources have gone
through or have plans for refurbishment programs to best utilize insertion devices for the next
decades. One remarkable example is PETRA-III which uses the high energy ring with large
circumference for producing low emittance beam. Another project is being proposed as
KEK-X where the 3 km-circumference KEK-B rings with 2000 to 3700 mA of currents will
be used to produce extremely high brilliance beams.
With all these advancements, what kind of biology do we aim to explore? There are three
frontiers: (1) ultimate protein crystallography for large macromolecular complexes and
extremely small crystals (1 micron scale) of flexible molecules, (2) X-ray solution scattering
for medium resolution structures of uncrystallizable complexes and dynamics of
protein-protein interactions and (3) 3D cell imaging with nm-level spatial resolution to
investigate cellular localization and transport of protein complexes in response to various
signals. The need for such hierarchical understanding of biological systems will be discussed
using a rapidly expanding and extremely competitive biological theme of novel ubiquitin
chains. Ubiquitin, a small protein with 76 residues, is involved in almost all biological
phenomena. It is covalently attached to proteins providing a complex pattern of polyubiquitin
chains. These posttranslational modifications provide basis for a plethora of signaling
cascades including immunity, cancer, protein trafficking, DNA repair to name but a few. Due
to the flexibility of the polyubiquitin chains, it is extremely difficult to crystallize them in
complex with their cognate proteins, hence the need for the ultimate protein crystallography.
31
Very often these complexes undergo drastic structural changes during their signal cascades.
X-ray solution scattering is well suited for providing vital information on dynamics of these
protein complexes. Signal cascades involve detection and amplification of external signals,
and transport of signaling molecules from one place to another in the cell, hence the need for
higher resolution (ideally several nm) 3D imaging for understanding their dynamic behavior.
Finally, the combination of these three frontiers will lead to faster and reliable design
strategies for novel drugs with lower side effects against cancer, rheumatoid and immune
responses.
32
16 4th AOFSRR
Structure and Mechanism of An Amino Acid Antiporter
Xiang Gao1,2,4, Feiran Lu1,2,4, Lijun Zhou1,2,4, Xiaochun Li1,2,4, Jiawei Wang1,2, and Yigong Shi2,3,5
1State Key Laboratory of Bio-membrane and Membrane Biotechnology, 2Center for Structural Biology, Department of Biological Sciences & Biotechnology, 3School of Medicine, Tsinghua University, Beijing 100084, China 4These authors contributed equally to this work. 5To whom correspondence should be addressed. E-mail: [email protected]
Virulent enteric pathogens such as Escherichia coli strain O157:H7 rely on acid
resistance (AR) systems to survive the acidic environment in the stomach. A major component
of AR is an arginine-dependent arginine:agmatine antiporter that expels intracellular protons.
Here we report the crystal structure of AdiC, the arginine:agmatine antiporter from E. coli
O157:H7 and a representative member of the amino acid/polyamine/organocation (APC)
superfamily of transporters. AdiC contains 12 transmembrane segments, forms a homodimer,
and exists in an outward conformation in the crystals. A conserved, acidic pocket opens to the
periplasm and is poised to associate with extracellular arginine. Structural and biochemical
analysis reveals the essential ligand-binding residues, defines the transport route, and suggests
a conserved mechanism for the antiporter activity.
mailto:[email protected]
33
17 4th AOFSRR
The development of X-ray microscopy for biomedical applications
Yeukuang Hwu, NSRRC
34
18 4th AOFSRR
The advanced SR structural materials science utilizing novel
measuring and data analysis technique. - From nano science to
pharmaceutical chemistry
Makoto Sakata, Japan Science & Technology Agency
35
19 4th AOFSRR
Megapixels per hour: fast fluorescence imaging at the Australian
Synchrotron.
D. Patersona*, M. D. de Jongea, D. L. Howarda, C. G. Ryanb, D. P. Siddonsc, and R. Kirkhamb
a Australian Synchrotron, Clayton VIC 3168, Australia
b CSIRO, Clayton VIC 3168, Australia c National Synchrotron Light Source, Brookhaven National Laboratory, NY, USA
* E-mail: [email protected]
A hard x-ray micro-nanoprobe has been constructed at the Australian Synchrotron [1] to
provide microspectroscopy across an incident energy range of 425 keV. Two probes are
used to collect -XRF and -XANES for elemental and chemical microanalysis: a
Kirkpatrick-Baez mirror microprobe for micron resolution studies; and a Fresnel zone plate
nanoprobe with laser interferometry capable of 60 nm resolution. An advanced fluorescence
detector developed by BNL [2] and CSIRO [3] featuring a large solid-angle, 384-element
planar silicon array that will accept count rates greater than 107/s with real-time elemental
deconvolution and image projection has been commissioned for the X-ray Fluorescence
Microprobe beamline. On-the-fly scanning combined with event mode data acquisition
enables sub-ms/pixel dwell. Tests of a 96-element prototype with the KB microprobe have
demonstrated high definition elemental images of over 100 megapixels on a range of
geological and biological samples in practical time frames. Dwell times down to 50 s/pixel
have been realised. Ultrafast XRF acquisition will enable high definition elemental mapping,
the possibility of fluorescence tomography and practical XANES imaging.
[1] D. Paterson, et al., AIP Conf. Proc., 879, 864, (2007).
[2] P. Siddons, et al., AIP Conf. Proc., 705 (953) (2004).
[3] C. Ryan, et al., Nucl. Instr. Meth. B, 260, 1 (2007).
36
20 4th AOFSRR
Fast switching of circular polarization using APPLE-II type
undulator
Kenta Amemiya
Institute of Materials Structure Science, High Energy Accelerator Research Organization
Photon Factory BL-16A is a variable-polarization soft X-ray (200-1500 eV) undulator
beamline, which provides right/left handed circular and horizontal/vertical linear polarizations.
Fast polarization switching using two APPLE-II type undulators in a tandem configuration [1]
is planned at BL-16A. The different polarizations from the two undulators are alternately led
to the beamline optics by modulating the electron orbit through the undulators. The upstream
undulator was installed first, in March 2008, and the circular, linear and elliptical polarization
modes are available at present. The second undulator for fast polarization switching will be
installed in 2010, with financial support from the Quantum Beam Technology Program by
Ministry of Education, Culture, Sports, Science and Technology, Japan. The feasibility of this
technique has been checked prior to the installation of the second undulator, by modulating
the electron orbit at 10 Hz and monitoring the beam intensity. The modulation in the X-ray
intensity agrees well with the expected modulation estimated from an X-ray tracing
simulation. Moreover, a novel optics will be installed in order to match the energy, resolution
and photon flux for the two undulators.
[1] T. Muro et al., J. Electron Spectrosc. Relat. Phenom. 144-147 (2005) 1101; AIP Conf. Proc.
879 (2007) 571; AIP Conf. Proc. 879 (2007) 1051.
37
21 4th AOFSRR
Inter-facility Cooperation
Richard F. Garrett ANSTO, Private Mail Bag 1, Menai, NSW, 2234 Australia
The Asia-Oceania region has a comprehensive suite of synchrotron light source facilities,
which are at least the equal to the Europe and North America. Developments in the region
continue at a rapid pace in all aspects of synchrotron radiation research and instrumentation.
The AOFSRR is an important forum for high level networking between the regions facilities
and user communities, but it also presents many opportunities for collaboration and
cooperation. The regions facilities are faced with similar challenges in both technology (eg
advancements in sources, beamlines and detectors) in serving their respective user
communities, in engaging with industry and in communicating the value of synchrotron based
research to the general public. Some examples of inter-facility cooperation, and the benefits
they bring to each side, will be presented and opportunities for enhanced future collaboration
will be discussed.
38
22 4th AOFSRR
ACCELERATOR BASED PHYSICS RESEARCH AND
PROMOTION OF THE SYNCHROTRON ACTIVITY
IN VIETNAM
Tran Duc Thiep
Institute of Physics, Vietnam Academy of Science and Technology
In this report we will present the accelerator based physics research in Vietnam in
different directions of Nuclear Physics both fundamental and applied investigations as the
study of photofission, photonuclear reactions in the giant dipole resonance region; nuclear
reaction with 14 MeV neutron; study of nuclear reactions and nuclear data at electron
accelerator in the energy range from 15 MeV to 2.5 GeV; study of possibility for producing
intense neutron beam at electron accelerators; study of charge exchange reaction at
accelerator; study of decay of neutron rich nuclei; study of nuclear reaction with heavy ion
and development and application of nuclear methods as photon and neutron activation
analysis and X-ray fluorscence method.
In the report we also discuss about possibility for development and application of
synchrotron radiation in Vietnam in the framework of the collaborations between countries in
Asian Ocean region.
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23 4th AOFSRR
Synchrotron Participation by New Zealand Researchers
Professor Richard Haverkamp,
Massey University, Palmerston North, New Zealand
With the construction of the Australian Synchrotron, participation by New Zealand researchers in
synchrotron science has been growing at a rapid rate. The New Zealand Government and 11 universities
and government research organisations became founding partners in the new synchrotron and contributed
towards the construction cost and ongoing operational costs. This has been a golden opportunity for New
Zealand science, particularly for young researchers, to extend their scientific research into the realm of
synchrotron science. The very positive impact on NZ science is beginning to be felt.
40
24 4th AOFSRR
Status of Synchrotron Radiation Related Activities in Malaysia
Swee-Ping Chia Physics Department, University of Malaya
50603 Kuala Lumpur, Malaysia E-mail: [email protected]
Malaysia does not have a synchrotron radiation facility. Research utilizing
synchrotron radiation is also scarce. Nevertheless, there are some research activities
utilizing the light sources at synchrotron radiation facilities in other countries. Such
researches are usually in the area of condensed matter physics and crystallography. In
the area of nuclear medicine, cyclotron is utilized in positron emission tomography
(PET) scan. Here, the 5.11 keV -ray is used for imaging. In another area, soft X-ray
from plasma sources is also an important tool in physics research.
There is a need to encourage research in Malaysia that utilizes synchrotron
radiation. In order to achieve this, we would like to call upon countries having
synchrotron radiation facilities in the neighbourhood of Malaysia to open up their
facilities to researchers from Malaysia. Once there are sufficient users of synchrotron
radiation, it would be easier to persuade the Government to have one such facility in
Malaysia.
mailto:[email protected]
41
25 4th AOFSRR
Cheiron School Students Report Session (A)
Jingyuan Ma Shanghai Synchrotron Radiation Facility/SINAP, CAS, China
In this short presentation, a very brief introduction of the experience and gains in 3rd
Cheiron School will be represented from a postgraduate students point of view. It concludes
couples of valuable things for me during the whole school course: the knowledge learned
from the effective lectures, the views enlarged by taking site tours in Spring-8, the inspiration
get from having conversation with experts, the exercise obtained through practicing at
beamlines, and the friendship knitted up with classmates as well. All of these give me
personal realization about the importance of running Cheiron School and certain
understanding on the role of AOFSRR in the international SR community. Whats more, Id
like to show my gratitude to all the people who give me guide and help in all my experience
dealing with synchrotron radiation knowledge and technology.
(B) Somchai Tancharakorn
Research & Academic Division, Synchrotron Light Research Institute, 111 University avenue, Muang district, Nakhon ratchasima, 30000 Thailand
During November, 2nd 11th 2009, the third AOFSRR (Asian Oceania Forum on
Synchrotron Radiation Research) school or the Cheiron School 2009 was once again held at
SPring-8, Japan. In this year, seven Thai researchers/students from different institutes had
joined others from countries in Asian-Pacific region in this training.
I, on behalf of Thai participants of this school, would like to express my deep gratitude
to AOFSRR for organizing the Cheiron School. During the training, he students learned
different techniques and theories varied from synchrotron radiation to advanced technology
such as X-ray free electron laser (XFEL), the program started with the lecture session in
which basic and complicated theories were clearly illustrated. In the meet the expert session,
students had opportunities to discuss in more details of specific techniques and in the last
42
session: the beamline practical, the students gain their better understanding of synchrotron
techniques by conducting experiments themselves.
It is clear that the Cheiron School project has succeeded its aims by providing basic
knowledge and perspectives of synchrotron radiation science and technology for students.
Moreover, giving the circumstance of the well-equipped facilities and the remarkable research
environment, the project has assisted in the future research networks and collaborations
between researchers who will be the major drive for the advancement of synchrotron
researches in Asia-Pacific regions in the near future.
43
Posters
26 4th AOFSRR
Present status of ERL project in Japan
Hiroshi Kawata ERL Project Office, High Energy Accelerator Research Organization, KEK,
Oho 1-1, Tsukuba, Ibaraki, 305-0801, Japan
The Energy Recovery Linac (ERL) project is progressing at KEK in Japan as a future light
source to progress the new synchrotron radiation activities such as nm-scale imaging,
femto-second science, local-structure analyses, and material sciences under extreme
conditions, in addition to the straightforward extensions of the present researches.
Furthermore, as an option for ERL, an X-ray free-electron laser (FEL) with an oscillator
configuration, X-FELO, has been proposed very recently[1] and collects much attention. To
realize the ERL, the development of the accelerator components is in progress. After the fiscal
year of 2008, several accelerator componentsa DC photo-cathode electron gun,
superconducting cavities for the injector and main accelerator, high power RF sources,
etc.were fabricated and tested. One of the big events in 2008 was that the development of
the infrastructure for the compact ERL has been approved. Thus, the year of 2008 can be
regarded as the starting point for the construction. I would like to present the present status of
the ERL project.
References:
[1] K.-J. Kim, Y. Shvydko, S. Reiche, PRL. 100, 244802 (2008)
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27 4th AOFSRR
Status of Timing System and Its Upgrade for PLSII
B.R. Park, M.H. Chun, J.W. Lee, S.J. Park and K.R. Kim Pohang Accelerator Laboratory, POSTECH, Pohang, 790-784, Korea
The timing system for the Pohang Light Source(PLS) consists of a synchronous universal
counter, AND gate, delay generators and other commercial modules. All the timing modules
are installed in the NIM crate and controlled by EPICS with VME system for the better
operation of timing system. The timing system has been operated very well for PLS decay
operation mode. But that should be upgraded for the top-up operation of PLS to increase the
beam injection efficiency, to decrease the beam loss, and to supply the injection timing signals
for beam line users. Therefore we are improving synchronization LINAC RF and SR RF now.
Also we are going to develop event system for PLSII.
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28 4th AOFSRR STATUS OF PLS-II HIGH-LEVEL CONTROL SYSTEM UPGRADE
E.H. Lee, J.M. Kim, J.W. Lee, S.J. Park, and K.R. Kim
Pohang Accelerator Laboratory, San 31, Hyoja-dong, Nam-gu, Pohang, Kyeongbuk, Korea
The PLS(Pohang Light Source) is 2.5 GeV synchrotron radiation source. The current
PLS high-level control system including control room will be totally upgraded for the PLS-II.
The PLS-II high-level control system consists of operation system, surveillance system, and
data management system. Operation system does machine control and monitoring through a
large LCD display wall, OPI(Operator Interface) system, and monitoring system. Surveillance
system does IOC server monitoring, PV status monitoring, and PV range checking. The data
management system provides data managing servers such database server, web server,
gateway server, NFS server, and back-up server
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29 4th AOFSRR STATUS OF PLS-II BPM CONTROL SYSTEM UPGRADE
J.W. Lee, E.H. Lee, D.T. Kim, S.J. Park, and K.R. Kim
Pohang Accelerator Laboratory, San 31, Hyoja-dong, Nam-gu, Pohang, Kyeongbuk, Korea
The PLS(Pohang Light Source) is 2.5 GeV synchrotron radiation source. The number of
beam position monitors (BPMs) around the PLS storage ring chamber is 108. The 108
analog-type Bergoz BPM modules are used to process the BPM pick-up signals. There are 12
EPICS IOCs in the field to process the signals from the BPM modules. The PLS-II storage
ring has 96 BPMs around the storage ring chamber. For the PLS-II upgrade, we are going to
partially replace current analog-type Bergoz BPM modules with the state-of-art digital-type
BPM modules. The digital-type BPM module will provide advanced beam position
monitoring features such as slow acquisition (10Hz), turn-by-turn (TBT), first-turns (FT), and
fast acquisition (10KHz). The current 12 EPICS IOCs of the PLS will be recycled for the
PLS-II.
The PLS(Pohang Light Source) is 2.5 GeV Synchrotron Radiation Source and started
its operation in1995. The PLS storage ring is equipped with 108 BPMs for beam position
monitoring.
The current PLS BPM system uses analog BPM electronic modules for pick-up signal
processing. There are 12 VME/VxWorks-based EPICS IOCs for data acquisition and
processing from these BPM modules.
The PLS-II storage ring will have 96 BPMs. Current analog BPM modules will be partially
replaced with the state-of-art digital BPM modules for
pick-up signal processing. Digital BPM modules can provide advanced beam diagnostic
capabilities such as Turn-by-Turn measurement, First-Turns measurement, Fast
Acquisition (10KHz), and slow Acquisition (10Hz).
References:
1 Burns G, Dacol F H. Solid State Commun, 1982, 42: 9-12
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30 4th AOFSRR
The status of Pohang Light Source Ilmoon Hwang, pohang Accelerator Laboratory, Pohang, Korea
Activities for performance improvement have been carrying out in PLS storage ring.Major activities for performance improvement are Matlab Middle Layer implementation, LOCO application and orbit feedforward along ID gap. In this presentation, we will describethe status of performance improvement in PLS storage ring.
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31 4th AOFSRR
Improvement SR RF Control System and Control status of PLS-II
MPS/RF Control System for PLS
J. C. Yoon, H. G. Park, J. W. Lee, S. J. Park, K. R. Kim, N. S. Nam(PAL) Pohang Accelerator Laboratory, POSTECH, Pohang 790-784, Korea
PLS SR RF control system of accelerator storage ring in operation experienced
performance improved control system in summer shutdown 2009. As the RF number 5 cavity
install is completed, existing RF VME control system's improvement was required for
enhancing RF function in PLS. Improvement required existing system operated as a RF
control system was applied to hardware and application program. The PLS-II MPS/RF control
system can be designed and upgraded in some ways. The magnetic power supply (MPS)
control system will be consist of the VME based IOC and the Embedded IOC. The VME
system of the PLS will be used for the Bipolar power supply control system. The Embedded
IOCs will be used for the new Bipolar MPS and Unipolar MPS control system. According to
design status of the RF cavity type such as adding NC cavities or new super conductivity(SC)
RF cavities, the high power RF system will be different and adding some high power sources
from present status. We described design status of PLS-II MPS/RF control system using
Embedded IOC, VME IOC, an EPICS development environment, and OPI Extension
software.
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32 4th AOFSRR
Coherent Hard x-ray free-electron laser based on Echo-enabled
Staged Harmonic Generation scheme
FENG Chao1,2 & ZHAO ZhenTang1
1 Shanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai 201800, China 2 Graduate University of Chinese Academy of Sciences, Beijing 100049, China
A novel approach to producing coherent hard x-ray based on the echo-enabled staged
harmonic generation (EESHG) free-electron laser scheme is proposed. This scheme is not a
simple cascaded echo-enabled harmonic generation (EEHG), but consists of an EEHG, a
beam shifter and a conventional high-gain harmonic generation (HGHG) like configuration,
which also works in the EEHG principle. In the first stage, all over the whole electron beam is
energy modulated by a laser beam in the first modulator and then converts into separate
energy bands by a very strong dispersion section. In the second modulator, the seed laser is
adjusted so that only the tail half part of the e-beam is energy modulated, then this beam is
sent through the second dispersion section which converts the energy modulated part into a
density modulation. The radiation from the first stage serves as the seed laser of the second
stage, the beam shifter between two stages is so tuned that the head part of the electron beam
which has already been modulated and shredded to energy beamlets can exactly interact with
the radiation from the first stage in the modulator of the second stage, so the total harmonic
number of this two stage structure will be over one thousand. It is shown that fully coherent
hard x-ray radiation can be obtained directly from a conventional VUV seed laser with
reduced size and cost in comparison with the self-amplified spontaneous emission (SASE)
based hard x-ray facilities.
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33 4th AOFSRR
MAGNETIC MEASUREMENT AND SHIMMING FOR EPU100 OF
SSRF Wei Zhang, Jie Lu, Qiaogen Zhou, Hongfei Wang
Shanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai, 201800, China
An elliptically polarizing undulator EPU100 has been built in Shanghai Light Source
(SSRF) recently. This undulator with APPLE-II type magnet structure has a total length 4.3 m
with a period of 100 mm. It was designed to provide four polarization operation modes:
circular, elliptical, horizontal and vertical. The magnetic measurement has been finished by
using the 3-dimensional Hall probes and flipping coil system. This paper details the method of
the magnetic measurement and magnetic shimming for EPU100. The maximum R.M.S. phase
errors 3.8 and 2.2 are calculated from the measured magnetic fields respectively in the
horizontal polarization mode and vertical polarization mode.
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34 4th AOFSRR
The upgrade project of Hefei Light Source
Li weimin, Wang Lin, Xu Gongliang, Feng Guangyao, Zhangshancai, Wu Ziyu
National Synchrotron Radiation Laboratory of University of Science and Technology of China, Hefei 230029, China
Hefei Light Source is composed of 800 MeV storage ring, 200 MeV electron linac and
transfer line, which is designed and constructed twenty years ago. Several factors limit the
performance of HLS, for examples, less number of insertion devices and large beam
emittance. To meet the requirements of synchrotron radiation users, an upgrade project of
HLS would be carried out in the next two years. Several sub-systems will be renewed, such as
magnet system, power supply, beam diagnostics, vacuum system, etc. The upgrade scheme is
described in this paper, including magnet lattice design, nonlinear performance, collective
effects, beam injection, orbit detection and correction, injector, etc.
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35 4th AOFSRR
Optical metrology at SSRF
Luo Hongxin, Wang jie, Xiao tiqiao
Shanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai 201204, China
Mirrors used in SSRF are typically segments of far-off axis aspherics, such as cylinders,
ellipsoids, and toroid with radii of curvature from tens of millimeters to hundreds of
kilometers. Surface quality for these mirrors is generally represented by slope errors(rms) and
micro-roughness. Typical tolerances for these mirrors used in SSRF are 3rad for rms slope
error and 0.3nm for rms micro-roughness. Measuring the mirrors used in SSRF before setup
in beamline with high precision is very important. Optical metrology methods such as LTP,
interferometry and 3D profilometer used at SSRF are introduced in this paper.
Optical group of Shanghai Synchrotron Radiation Facility does its best to build a
comprehensive and reliable optical testing laboratory. Through the optical testing laboratory's
work, all staff of the beamlines are aware of the various surface parameters of their optical
elements used in their beamline and know how to maintain the normal operation of optical
elements. Moreover, our work helps them to communicate with the optical components
manufacturer effectively in order to making their products to meet better the requirements of
Shanghai Synchrotron Radiation Facility beamline construction.
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The development of Bending Machines at SSRF
Song XUE, Yuan FU, Wanqian ZHU Shanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai, 201800, China
Bending machines have important effects on beamlines. There are fives sets of big
dimension bending machines including collimator mirrors and focusing mirrors used in the
seven beamlines of SSRF. The bending machines main functions are reflecting beam,
collimating beam, focusing beam and cut-off energy. The third generation synchrotron source
requires the bending machines have high precision slope error and high stability. The mirrors
length is 1000mm. The bending machines bender type is four-cylinder bender and bender
driver is jack mode. SSRF developed the five sets of big dimension bending mirrors with the
cooperation with PAL. The bending machines consist of mirror bending system, movement
system, gravity system, cooling system, vacuum system, adjustment system and control
system. Based on the design targets, the minimum bending radius is 2 km and the radius
resolution is 50mm, the mirrors tangential slope errors are less than 3rad, the vacuum of
bending machines is better than 510-7Pa. The mirror pose adjustment mechanism can make
the 5-dimensions adjustment including X direction, Y direction, pitch angle, roll angle and
yaw angle. The key technologies of bending machines including dynamic simulation
calculation, slope error calculation and gravity compensation, mirror tangential radius and
slope error off-line test. In the final test the slope errors are less than 2 rad and targets such
as mirror adjustment range, resolution and repeatability are all better than the design targets.
The five sets of bending machines all operate in good condition.
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Present status of crystal cooling of SSRF DCM with sagittal focus
WANG Na-Xiu, LIU Shi-Lei, XU Zhong-Min, BIAN Feng-Gang Shanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai, 201800, China
Design of 1st crystal cooling geometry of SSRF DCM with sagittal focus, which is made in
China, is mainly reported. Simulation indicates that the broadening of the FWHM of Si(111)
rocking curve induced by the heat load is about 3.7 rad RMS, which is fairly good
agreement to the experimental value of 5 rad. Meanwhile according to the linearity between
the photon flux extracted from the monochromator and electron current of the storage ring, it
had been proven that this scheme is reliable.
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38 4th AOFSRR
The variable included angle plane grating monochromator
Song XUE 1 , Jiahua CHEN 1 , Renzhong TAI 1 , Yong WANG 1 , Yanqing WU 1 , Min CHEN 1 Qipeng LU 2 , Zhongqi PENG 2
1. Shanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai 201800, China 2. Changchun Institute Of Optics, Fine Mechanics and Physics, Chinese Academy of Sciences,
Changchun 130000, China
This article discusses the variable included angle plane grating monochromator on the
soft X-ray spectromicroscopy beam-line at Shanghai Synchrotron Radiation Facility(SSRF).
Operated in collimated light, the variable included angle plane grating monochromator
changes the variable included angle to select photon energy by combining simultaneous
rotation and translation of the plane mirror. The variable included angle plane grating
monochromator consists of plane mirror, plane grating, sin-bar scanning mechanism, linear
driving mechanism, grating exchange mechanism, position adjusting mechanism, water
cooling system, vacuum chamber, UHV system, driving control system. Moreover, there are
two different groove density plane gratings, installed abreast on the substrate, can be
interchanged under vacuum to meet different experiment requirements. We resolved high
precision repeatability of mechanical transmission system and effective water cooling system
of optical elements with high heat load in UHV, and set up the high precision demarcating and
detecting system. The energy range, energy resolution and energy repeatability, designed as
250eV-2000eV, 4500@244eV and 20meV@244eV respectively, are the main capacities of the
variable included angle plane grating monochromator, and the corresponding test results are
192-2182eV,17900@244eV and 4.3meV@244eV (RMS), 11meV@244eV (MAX)
respectively, measured by photodiode and measuring the Ar shell excitation spectra.
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The Motion Control System in SSRF beamlines
Zheng Lifang, Liu Ping, Zhang Zhaohong, Hu Chun, Wu Yingfeng, Mi Qingru, Li Zhong
Shanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai, 201800, China
SSRF beamline control system takes three kinds of responsibilities: motion control
system, beamline status monitor and protection system, the beam position acquiring and
diagnosing system. The motion control is the essential one. It provides the required beam in
energy, size and flux by controlling the Monochromator, mirror chamber, slits and other
optical components. There are two kinds of hardware for motion control system: VME-based
MAXv controller and SLS drivers, RS232-based controller. The control software is developed
under EPICS.
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BEAMLINE SURVEY AND ALIGNMENT IN SSRF
Ming Ke, Song Xue, Jie Wang, Chenghao Yu Shanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai, 201800, China
Shanghai Synchrotron Radiation Facility, SSRF, is a 3.5 GeV third-generation
synchrotron radiation light source with a tight alignment requirement of better than 0.25 mm
relative to the light emission point for key beamline components. This defines that all the
devices, instruments and components are adjustable; the theoretical and actual axis of all the
optical components should be in coincidence with beam line axis; the position and rotation
angle of key optical components should be accurately recorded and could be adjusted to
decrease its deviation.
During the installation stage of the first 7 beamlines, state-of-the-art techniques have
been employed. One significant high-profile is the establishment of hierarchical control
network system scattered among the experimental hall and protection hutches, which provides
a unified coordinate system and sufficient monuments for components installation and
alignment. The local control network for each beamline itself has a relative accuracy of better
than 0.12 mm among adjacent monuments by taking advantage of optimal observation
scheme and least square adjustment algorithm. It can be updated timely to reflect the
historical changes due to slab subsidence and other sources of instability; hence it delivers the
spatial information, which is really reliable and accurate. Other advanced techniques have
been used including the fiducialization of small optical components by articulated arm and
CMM etc, the rapid on site adjustment and positioning manner via laser tracker, and unique
cross check approach incorporated with precise level, theodolite, and alignment laser etc.
Except for the resourceful instrumentation and method, the survey and alignment
preparation and implementation for all the beamlines are very effective and have been
organized in a streamline way, which assured the installation has been carried out smoothly
and on schedule. According to actual alignment data, 0.2 mm positioning accuracy has been
achieved for all the key components and it has been corroborated by beam line
commissioning. Partially thanks to the high quality of survey and alignment work, all the
58
beamlines have achieved the important milestone, acquiring synchrotron radiation light at
monochromator, in less than three days.
Relative to traditional beamline survey and alignment method that exploits theodolite
and level, the 3D survey technique adopted in SSRF is more credible, effective and precise,
which has a promise perspective for the future SSRF beam line project.
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X-RAY BEAM POSITION MONITOR SYSTEM FOR SSRF Zhong LI*, Jian-ying ZHOU, Xiang-yun QING, Zhao-hong ZHANG, Chun HU, Zhi-hua WEI, Pei-rong
GONG Devision for Beamline Engineering,
Shanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai, 201800, China ail: *Em .cn [email protected]
X-ray beam position monitor (XBPM) is an eye to find the position of the X-ray beam in
synchrotron radiation facility. It is helpful for storage ring and beamline commissioning.
An X-ray position monitor system for primary seven beamlines in Shanghai Synchrotron
Radiation Facility (SSRF) is home developed. The system includes monitor, data acquirement
system, data transfer net and personal-operation-interface (POI). Quad-blade beam position
monitor (BBPM) with CVD diamond blades, fluorescent screen based on CVD diamond, and
wire-scanning beam position monitor (WBPM) are designed for beamlines with different light
source. The signal from BBPM or WBPM is amplified by a current amplifier and then
converted to digital signal which is transferred to SSRF beamline control net. POIs integrated
in a beamline control interface for each beamline and in a summary interface in the central
control room can give the value and curve depended on time for each X-ray beam position
monitor.
mailto:[email protected]
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42 4th AOFSRR
SSRF BEAMLINE INTERLOCK SYSTEM P.R.Gong, Z.X.Zhu
Shanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai, 201800, China
SSRF beamline interlock system includes Personal Safety System (PSS) and Equipment
Protection System (EPS). The PSS is to set up a logical action by using the searching buttons,
door switches, emergency buttons etc. to interlock the photon shutters and to keep the
experimenters from the unexpected radiation hazard. The EPS is to monitor all working
parameters such as temperature, vacuum, water flow to protect devices from the possible
damage while the parameters are over the pre-set threshold. Both systems are based on PLC
and communicate smoothly with measured devices and other interlock systems. The beamline
interlock system has been put into run in SSRF from the middle of 2008 and works well up to
now.
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43 4th AOFSRR
INTRODUCTION OF THE FRONT ENDS AT SSRF WU Guanyuan, ZHANG Min, CHEN Ming
Shanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai, 201800, China
In the first phase of construction, seven front ends have been constructed, that 2 from
bending magnet (BM) and 5 from insertion device (ID). The power density and total power
are 37kW/mrad2 and 10kW for in-vacuum Undulator and multi-poles Wiggler respectively.
SSRF front end is designed to confine the photon beam, absorb the unwanted heat, monitor
the beam positionprotect personnel and equipment safety. The standardization, reliable
technology, ease in installation and maintenance are design philosophy of the SSRF front
ends. With operate for two years, the front ends show that pressure has no any turbulent to the
electron orbit and its interlock system can provide a quick vacuum protection for the storage
ring in the case of a vacuum failure in the beamline, all components impinged by SR work
well, and the radiation of background level can be obtained in optical hutch when the safe
shutter closed. Here we will introduce the general design, installation and operation of these
front ends.
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Present Status of Public Beamlines at SAGA-LS
Toshihiro Okajima Kyushu Synchrotron Light Research Center, Yayoigaoka, Tosu, Saga 841-0005, Japan
SAGA-LS has been operated well since February 17th, 2006. Four beamlines, BL06, BL10,
BL11 and BL18, were newly built in the fiscal year of 2008. Nine beamlines are now
operating adding these four beamlines. Beamlines, BL10 and BL11, are public beamlines
newly built by the local government of Saga Prefecture for public users. BL11 is standard
hard X-ray beamline using a Si(111) double crystal monochromator. BL10 is a new soft X-ray
beamline using an APPLE- type undulator as a light source. The undulator supplies the
tunable polarization of the light to us. The experimental instruments for photoelectron
emission microscopy (PEEM) and high resolution angle-resolved photoemission spectroscopy
(ARPES) were prepared. Beamlines BL06 and BL18 are contract beamlines built by Kyushu
University and Nikon Corporation, respectively. Three contract beamlines are also operating
now adding these two beamlines. The new hard X-ray beamline, BL07, is also under
construction as a public beamline. The beamline was designed for using wide energy range
from 4 to 30 keV X-ray generated by the newly designed superconducting wiggler. The
X-rays will be supplied for the several experiments: e.g. XAFS, X-ray fluorescence analysis,
X-ray imaging and protein crystallography.
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Preliminary Design of Coherent Hard X-Ray Beamline
at the Taiwan Photon Source
Yu-Shan Huang*1, Chi-Yi Huang1, Chien-Hung Chang1, Mau-Tsu Tang1, Wen-Yan Peng1, Tsang-Lang Lin2, Shih-Lin Chang2, Hsin-Lung Chen2, and Chih-Hao Lee2
1 National Synchrotron Radiation Research Center, Hsinchu 30076, Taiwan 2 National Tsing Hua University, Hsinchu 30013, Taiwan
The coherent hard X-ray beamline is one of the initial phase of beamlines designed for the
Taiwan Photon Source (TPS), a new 3 GeV ring under construction at the National
Synchrotron Radiation Research Center (NSRRC). With an in-vacuum undulator, this
beamline will provide highly coherent beam mainly for X-ray photon correlation
spectroscopy (XPCS), small Q coherent diffractive imaging (CDI) and small angle X-ray
scattering (SAXS) experiments. The beamline is designed to operate in the energy range 5-20
keV, suitable for most conventional SAXS, including anomalous measurements. A vertical
focusing mirror collimates the beam to preserve the coherent photons with compatible
coherent lengths in vertical and horizontal directions. The horizontal coherence is
nevertheless filtered by pairs of well polished slits for coherent experiments. An optional
horizontal mirror focuses the incoherent beam horizontally for conventional SAXS
experiments.
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Niversity-of-Tokyo SR Outstation BL07LSU at SPring-8
Masaharu Oshima1,2 and Akito Kakizaki1),3) Synchrotron Radiation Research Organization1), University of
Tokyo School of Engineering2), Institute for Solid State Physics3) 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan
We have constructed a new soft X-ray (SX) 27m-long undulator beamline for materials
science, University-of-Tokyo SR Outstation at SPring-8 BL07LSU. Eight figure-8-type
undulators can provide us with polarization-controlled SX with photon energy ranging from
250 eV to 2 keV.
At this beamline, mainly three kinds of experiments will be performed from autumn in
2009. The first project is 3DnanoESCA where angle-resolved photoelectrons are detected
from the sample irradiated by about 50 nm size SX beam for pin-point in-depth profiles in
nano-devices. The second project is SX emission spectroscopy for biomaterials and operating
polymer electrolyte fuel cells. The third project is time-resolved photoemission spectroscopy
for photo-induced phase transition and photo-catalytic reactions.
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47 4th AOFSRR
XRD Beamline and Endstation
Zhong LI, Qing HE, Sisheng WANG, Wen WEN, Mei GAO, Xingtai ZHOU
Shanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai, 201800, China
BL14B1, X-ray diffraction beamline (XRD), one of the seven beamlines in the primary
phase of Shanghai Synchrotron Radiation Facility (SSRF), aims at the research in material
sciences, condensed physics, crystallography, and chemistry etc.. This beamline is based on a
bending magnet light source. The kernel optical devices include a pre-collimating mirror, a
sagittal double crystal monochromator (DCM) and a post-focusing mirror. The
pre-collimating mirror is a bended silicon crystal with Rhodium coating to collimate the
X-ray beam entering DCM in order to enhance the energy resolution. The DCM is a water
cooled double Si (111) crystal monochromator with a bendable second crystal for sagittal
focusing. The energy range is from 4keV to 22keV. The post-focusing mirror has two
reflection surfaces, with or without Rhodium coating, to suppress the harmonics in low energy
range. It can work at high brightness mode or high resolution mode depending on whether the
mirror is bended or not in meridional. The experimental station is equipped with a Huber
5021 diffractometer and SPEC of data acquirement software.
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SSRF SOFT X-RAY SPECTROMICROSCOPY
Renzhong TAI, Yong WANG, Zhi GUO, Rui YANXiangjun ZHEN,
Min CHEN, Yanqing WU, Jiahua CHEN, Song XUE, Hongjie XU Shanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai, 201800, China
As one of the only soft x-ray beamline in the first-phase beamlines at SSRF, this
beamline provides broad energy varies from 250 to 2000eV, covering the K-edge of C, N, O,
F, Na, Mg, Al, Si, and L edges of P, S, Cl, K, Ca, Fe, Cu, Zn, etc. Therefore, it is expected to
have wide application in biological science, environmental science, polymer, and material
science, etc. Besides, as it selected an elliptical polarized undulator as light source, it could
even be used to study x-ray-polarization-dependent materials. So far, preliminary qualitative
characterization for circular polarization has been conducted for this EPU source. More
quantitative one will be done soon.
For the beamline, a varied-included-angle plane grating monochromator was used. This
PGM was operated in a collimated mode, with its Cff value adjustable from 1.8 to 2.5,
designed and fabricated by domestic collaboration. Argon gas ionization spectrum proved the
energy resolving power is better than 18000 at photon energy of 244eV.
A scheme of a scanning transmission x-ray microscopy (STXM) was adopted at
end-station. So far, spatial resolution of better than 30 nm has been demonstrated. Therefore,
by tuning photon energy, a serious of transmitted 2D imaging including NEXAFS information
can be recorded. Moreover, 3D imaging and Total Electron Yield (TEY) functions are
preservedthough have not been tested so far.
The commissioning of the soft x-ray Spectromicroscopy beamline was formally started
from last December. The performances of the beamline have reached or surpassed the
designing goals according to the actual measurements made by domestic experts. So far, tens
of experiments have been conducted and some exciting preliminary results have been
obtained, demonstrating its conspicuous advantage as a novel experimental method, since its
first operation to users from this May 6.
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X-RAY IMAGING AND BIOMEDICAL APPLICATION BEAMLINE
AT SSRF
Tiqiao Xiao*, H