1
Synchrotron radiation (SR) is an important tool not only for basic research, but also for engineering and industry-oriented research and development. For this purpose, an SR facility project has been proposed at Nagoya University since 1991. In the meantime, the Aichi Prefectural government has been planning a new research and development complex “Knowledge Hub” for industries in the Central area of Japan and the SR facility proposed at Nagoya University has been considered to be one of the leading facilities for “Knowledge Hub.” Therefore, the prefecture, industries, universities, and research institute in the Aichi area are working together to realize this plan. Introductoin Table1. Parameters of Accelerators Storage Ring Beam energy 1.2 GeV Current >300 mA Circumference 72.0 m Normal bend 1.4 T, 39 o x 8 Super bend 5 T, 12 o x 4 RF frequency 500 MHz Natural emittance 53 nmrad Magnetic lattice Triple Bend Cell x 4 Straight sectoin 5.2 m x 1, 4.3 m x 1 Booser synchrotron Beam energy 1.2 GeV Circumference 48.0 m RF frequency 500 MHz Injector linac Beam energy 40 MeV Current 60 mA RF frequency 2856 MHz Table 2. Parameters of the superbend York type C type Length < 950 mm Peak field > 5 T Hight < 3000 mm Bending angle 12 o (1.2 GeV) Width < 900 mm Figure 2. Schematic view of the superbend Accelerators & Beamlines The key facility of the plan is a compact electron storage ring, which is able to supply hard X-rays. The SR facility, consisting of accelerators, beamlines, peripheral equipments and housing, has been designed at the Nagoya University Synchrotron Radiation Research Center. The configuration of NSSR (Nagoya University Small Synchrotron Radiation Ring) is based on the Triple Bend with twelve bending magnets. Eight of them are normal conducting magnets of 1.4 T and four of them are 5 T superconducting magnets (superbends), respectively. The bending angle of them is 12 degrees and two or three hard X-ray beamlines can be constructed at each superbend, so that more than 10 hard X-ray beamlines can be constructed in our facility. The number of beamlines from normal conducting bending magnets is more than 16. In addition, we will install an undulator or a wiggler in straight sections. Table 3. Six beamlines constructed in the first phase Beamlines Energy Range Acceptance Angle Flux Energy Resolution (keV) (mrad) (photons/sec) (E/ΔE) Hard X-ray XAFS 5 - 20 2 1×10 11 7,000 Soft X-ray XAFS 0.8 - 6 7.5 7×10 10 2,000 VUV & Photoemission Spectroscopy 0.03 - 0.9 0.5 - - Small angle X-ray Scattering 15 2 7×10 10 2,000 X-ray Diffraction 5 - 20 2 4×10 10 1,700 X-ray Fluorescence & Reflectivity 5 - 20 2 1×10 11 2,000 Figure 3. Spectra of photon flux from bending magnets (a) and brilliance from undulator (b) 10 8 10 9 10 10 10 11 10 12 10 13 10 14 10 4 10 5 4 5 4 5 NSSR nb NSSR sb PF b UVSOR-II b SAGA b SPring-8 b NewSUBARU b Rits Photon energy (eV) Flux (ph/s/mrad/0.1%b.w.) 10 3 10 2 PF bending magnet (400mA) (300mA) UVSOR bending Magnet (350mA) SPring-8 bending magnet (100mA) NSSR 5T Superbend NSSR normal bend (300mA) SAGA-LS bending magnet (300mA) Rits (300mA) NewSUBARU 10 13 10 14 10 15 10 16 10 17 10 1 10 2 10 3 Photon energy (eV) Brilliance (ph/s/mrad 2 /mm 2 /0.1 % b.w.) 1st 3rd Linear mode spectrum Helical mode 1st 5th (a) (b) SAGA Light Source (1.4 GeV, 1.9 keV) HiSOR (700 MeV, 0.38 keV) SPring-8 (8 GeV, 28.9 keV) New SUBARU (1.5 GeV, 2.3 keV) AURORA (575 MeV, 0.84 keV) UVSOR-II (750 MeV, 0.43 keV) KEK PF (2.5 GeV, 4.0 keV) KEK PF-AR (6.5 GeV, 26.4 keV) Toyota city Toyohashi city Pref. Nagoya Airport Chubu Centrair Int’l Airport JR Sinkansen Subway Expressway Linimo(Linear motor car ) Nagoya city Nagoya univ. SRcenterSubway UVSOR-II Central Japan Synchrotoron Radiation Facility (1.2 GeV, 4.8 keV) Figure 1. Central Japan Synchrotoron Radiation Facility and SR facilities in japan Construction Schedule 2009. Site formation for the buildings construction 2012. First synchrotron light Management Central Japan Synchrotron Radiation Research Facility Project Naoto Yamamoto 1 , Yoshifumi Takashima 1 , Masahito Hosaka 1 , Masahiro Katoh 2,1 , Nobuhisa Watanabe 1 and Yoshikazu Takeda 1 1. Synchrotron Radiation Research Center, Nagoya University, Nagoya, 464-8603 Japan 2. UVSOR, Institute for Molecular Science, Okazaki, 444-8585 Japan E-mail : [email protected], URL : http://www.nusrc.nagoya-u.ac.jp The 13th Hiroshima International Symposium on Synchrotron Radiation, March 10-11th, 2009 Aichi Science & Technology Foudation is responsible for the operation and management.

Central Japan Synchrotron Radiation Research Facility ProjectPref. Nagoya Airport Chubu Centrair Int’l Airport JR Sinkansen Subway Expressway Linimo(Linear motor car ) Nagoya city

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Page 1: Central Japan Synchrotron Radiation Research Facility ProjectPref. Nagoya Airport Chubu Centrair Int’l Airport JR Sinkansen Subway Expressway Linimo(Linear motor car ) Nagoya city

  Synchrotron radiation (SR) is an important tool not only for basic research, but also for engineering and industry-oriented research and development.

For this purpose, an SR facility project has been proposed at Nagoya University since 1991. In the meantime, the Aichi Prefectural government has been

planning a new research and development complex “Knowledge Hub” for industries in the Central area of Japan and the SR facility proposed at Nagoya

University has been considered to be one of the leading facilities for “Knowledge Hub.” Therefore, the prefecture, industries, universities, and research

institute in the Aichi area are working together to realize this plan.

Introductoin

Table1. Parameters of AcceleratorsStorage Ring

Beam energy 1.2 GeVCurrent >300 mACircumference 72.0 mNormal bend 1.4 T, 39o x 8Super bend 5 T, 12o x 4RF frequency 500 MHzNatural emittance 53 nmradMagnetic lattice Triple Bend Cell x 4Straight sectoin 5.2 m x 1, 4.3 m x 1

Booser synchrotronBeam energy 1.2 GeVCircumference 48.0 mRF frequency 500 MHz

Injector linacBeam energy 40 MeVCurrent 60 mARF frequency 2856 MHz

Table 2. Parameters of the superbend York type C type Length < 950 mm Peak field > 5 T Hight < 3000 mm Bending angle 12o (1.2 GeV) Width < 900 mm

Figure 2. Schematic view of the superbend

Accelerators & Beamlines

  The key facility of the plan is a compact electron storage ring, which is able to supply hard X-rays. The SR facility,

consisting of accelerators, beamlines, peripheral equipments and housing, has been designed at the Nagoya University

Synchrotron Radiation Research Center. The configuration of NSSR (Nagoya University Small Synchrotron Radiation

Ring) is based on the Triple Bend with twelve bending magnets. Eight of them are normal conducting magnets of 1.4 T

and four of them are 5 T superconducting magnets (superbends), respectively. The bending angle of them is 12 degrees

and two or three hard X-ray beamlines can be constructed at each superbend, so that more than 10 hard X-ray beamlines

can be constructed in our facility. The number of beamlines from normal conducting bending magnets is more than 16.

In addition, we will install an undulator or a wiggler in straight sections.

Table 3. Six beamlines constructed in the first phaseBeamlines Energy Range Acceptance Angle Flux Energy Resolution (keV) (mrad) (photons/sec) (E/ΔE)Hard X-ray XAFS 5 - 20 2 1×1011 7,000Soft X-ray XAFS 0.8 - 6 7.5 7×1010 2,000VUV & Photoemission Spectroscopy 0.03 - 0.9 0.5 - - Small angle X-ray Scattering 15 2 7×1010 2,000X-ray Diffraction 5 - 20 2 4×1010 1,700X-ray Fluorescence & Reflectivity 5 - 20 2 1×1011 2,000

Figure 3. Spectra of photon flux from bending magnets (a) and brilliance from undulator (b)

108

109

1010

1011

1012

1013

1014

104 1054 54 5

NSSR nbNSSR sbPF bUVSOR-II bSAGA bSPring-8 bNewSUBARU bRits

Photon energy (eV)

Flux

(ph/

s/m

rad/

0.1%

b.w

.)

103102

PF bending magnet (400mA)

(300mA)UVSOR bendingMagnet (350mA)

SPring-8 bendingmagnet (100mA)

NSSR 5TSuperbend

NSSRnormal bend(300mA)

SAGA-LSbending magnet(300mA)

Rits (300mA)

NewSUBARU

1013

1014

1015

1016

1017

101 102 103

Photon energy (eV)

Bril

lianc

e (p

h/s/

mra

d2 /mm

2 /0.1

% b

.w.)

1st

3rd

Linear modespectrum

Helical mode 1st5th

(a) (b)

SAGA Light Source(1.4 GeV, 1.9 keV)

HiSOR(700 MeV, 0.38 keV)

SPring-8 (8 GeV, 28.9 keV)New SUBARU (1.5 GeV, 2.3 keV)

AURORA(575 MeV, 0.84 keV)

UVSOR-II(750 MeV, 0.43 keV)

KEK PF (2.5 GeV, 4.0 keV)KEK PF-AR (6.5 GeV, 26.4 keV)

Toyota city

Toyohashi city

Pref. Nagoya Airport

Chubu CentrairInt’l Airport

JR Sinkansen

Subway

Expressway

Linimo(Linear motor car )

Nagoya city

Nagoya univ.(SRcenter)

Subway

UVSOR-II

Central Japan Synchrotoron Radiation Facility (1.2 GeV, 4.8 keV)

Figure 1. Central Japan Synchrotoron Radiation Facility and SR facilities in japan

Construction Schedule 2009. Site formation for the buildings construction 2012. First synchrotron light

Management

Central Japan Synchrotron Radiation Research Facility Project

Naoto Yamamoto1, Yoshifumi Takashima1, Masahito Hosaka1, Masahiro Katoh2,1, Nobuhisa Watanabe1 and Yoshikazu Takeda1

1. Synchrotron Radiation Research Center, Nagoya University, Nagoya, 464-8603 Japan2. UVSOR, Institute for Molecular Science, Okazaki, 444-8585 Japan

E-mail : [email protected], URL : http://www.nusrc.nagoya-u.ac.jp

The 13th Hiroshima International Symposium on Synchrotron Radiation, March 10-11th, 2009

 Aichi Science & Technology Foudation is responsible for the operation and management.