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NTHU Physics Colloquium
Current Development and Prospect of
New Synchrotron Facilities
張石麟 (Shih-Lin Chang)
March 20, 2013
Outline
•Introduction
•High energy synchrotron sources
•New additions of synchrotron facilities (under
construction or recently completed)
•New synchrotron facilities in planning
•Free electron lasers (FEL’s)
•Prospect & conclusion
• 相對論效應使得電子以接近光速作圓周運動時所發射的電磁波集中在切線方向,而不像大哥大產生的電波向四面八方散去。
同步加速器光源超快速電子在磁場中偏轉所產生的電磁波
Zeroth generation sources1950’s-60’s: Electron synchrotrons (cyclic accelerators)
First generation sources (storage rings)1970’s: e+/e- colliders (Mostly parasitic on high energy physics programs)
Second generation sources1980’s: New rings and fully dedicated use of e+/e- colliders, use of wigglers & undulators
Third generation sources1990’s: Low emittance ring with many straight sections for insertion devices
Fourth generation sources2000’s: Linac-based sources
•Free-electron laser (FEL)•Energy Recovery Linac (ERL)
Diffraction-limited rings; Ultra-short bunches; New ideas
Synchrotron Radiation
• Bending Magnet– White X-rays– Wide horizontal divergence– 1 limited vertical divergence– Moderate power– Moderate power density
• Wiggler– White X-rays– Moderate horizontal divergence– 1 Limited vertical divergence– High power– High power density– Elliptically polarized/linearly polarized
• Undulator– Quasi-monochromatic X-rays– Small vertical and horizontal divergence (Central Cone)– High power– Extremely high power density– Circularly polarized/ linearly polarized
Bending magnet(偏轉磁鐵 ) & insertion device(插件 )
Storing Ring
Undulator / Wiggler
IntroductionThere are now 66 synchrotrons in operation throughout the world. Additional 11 are either under construction or in planning.
In addition to 3 high-energy synchrotrons, ESRF, APS, Spring-8, there are several low- and mid-energy 3rd generation synchrotrons.
Starting 2000, mid-energy rings have been considered as most economic and yet providing high quality beams (low emittance) for SR experiments
Many new 3rd generation synchrotron facilities are now either under construction or in the design process.
Free electron lasers
World Map of Synchrotron Facilities
Hsinchu
臺灣光源 (TLS)現況
加速器儲存環(15億電子伏特 )
增能環(15億電子伏特 )
線型加速器
傳輸線
SW6
W20
U5
EPU5.6
U9
IASW6-R2
IASW
6-R6
超導高頻共振腔
SWLS
IASW6-R4
•’93 年 : 4月完成試車 ;10月開放給用戶實驗
•’96 年 : 儲存環能量由 1.3GeV提升為1.5GeV
•’00 年 : 增能環以全能量注射到儲存環•’02 年 : 6T超導移頻磁鐵 SWLS正式使用•’04 年 : 液氦低溫與超導增頻磁鐵 SW6運
轉•’05 年 : 啟用超導高頻共振腔•’05 年 : 用戶時段施行 300mA恒定電流運
轉•’06 年 : 1st 安裝彎段超導增頻磁鐵 IASW-
R6•’09 年 : 安裝 2nd 彎段超導增頻磁鐵 IASW-
R2•’10 年 : 安裝 3rd 彎段超導增頻磁鐵 IASW-
R4 360 mA恒定電流運轉模式
TPS完成後之同步輻射研究中心俯視圖
•亞洲第一座第三代同步輻射•全球第二座使用超導高頻腔同步輻射•全球第三座全時恆定電流運轉設施•安裝的超導插件磁鐵數量及密度最高
Electron gun produces electrons
How is it Practically Produced and Used for Research?
Beam lines transport radiation into “hutches”, where instrumentation is available for experiments
Wiggler / Undulator insertion devices generate strong x-ray beams
Linear accelerator/ booster accelerate e- which are transported to storage ring
Klystrons generate high power radio wave to sustain electron acceleration, replenishing energy lost to synchrotron radiation
The storage ring circulates electrons, where they are bent, synchrotron radiation is produced
High energy synchrotron sources
Sources:The SSRL Strategic Plan: 2013 - 2018http://www-ssrl.slac.stanford.edu/content/beam-lines/maphttp://www-ssrl.slac.stanford.edu/content/about-ssrl/history-stanford-synchrotron-radiation-lightsource
SLAC Stanford Synchrotron Radiation Lightsource (SSRL) – Menlo Park, CA, USA
Aerial View of SSRL. (Courtesy: SLAC)
1973 SSRL began as the Stanford Synchrotron Radiation Project (SSRP)1974 First user run1977 SSRP became SSRL 1992 SSRL became fully dedicated synchrotron radiation source2004 Major upgrade of SPEAR completed - SPEAR3
SSRL / SSRP
The first multi-GeV storage ring based synchrotron radiation source in the world
( 2004: 3 GeV, 300-500mA, 234 m.)
6 GeV; = 11800; 884m circumference
European Synchrotron Radiation Facility (ESRF)
Advanced Photon Source (APS) – Argonne, IL, USA
Nominal Energy GeV 7.0
Natural Emittance nm-rad 2.514
Effective Emittanceat ID Location nm 3.129
Circumference m 1104.000
Sources: •http://www.aps.anl.gov/•http://www.aps.anl.gov/Beamlines/Beamlines_Map/index.html•APS Upgrade project PDR (December 2012)
Source: http://www.aps.anl.gov/About/Welcome/
Aerial view of the APS
Beamlines Map
The Advanced Photon Source (APS) provides the brightest storage ring-generated X-ray beams in the Western Hemisphere to more than 5,000 scientists
worldwide.
8 GeV; = 15,700; 1.44 km circumference
Spring-8 (Super Photon ring-8 GeV) Japan
New additions of synchrotron facilities(under construction or recently completed)
Year of Commi-
ssionLocation
Accelerator
Energy[GeV]
Emittance
[nm-rad]
Circum-ference
[m]
Straight Sectionsm*section
Unit Status
1993 USA, Berkeley ALS 1.9 6.75 196.8 6m*12 12TBA Operating
1993 Taiwan, Hsinchu TLS 1.5 18 120 6m*6 6 TBA Operating
1993 Italy, Trieste ELETTRA 2.4 7.0 259 6m*12 12 DBA Operating
1995 Korea, Pohang PLS 2.5 12.0 281 6m*12 12 TBA Operating
2001 Switzerland,Villigen SLS 2.4 4.1 28811.76m*3+7m*3+4
m*612 TBA Operating
2003 Canada, Saskatoon CLS 2.9 18.1 171 5.2m*12 12 DBA Operating
2004 USA, Stanford SPEAR3 3.0 10 2343.2m*12+4.8m*4+7.6
m*218 DBA Operating
2006 France, Orsay SOLEIL 2.75 3.7 35112m*4+7m*12+3.6
m*816 DBA Operating
2007 UK, Oxfordshire DIAMOND 3.0 2.7 56211.34m*6+8.34m*1
824 DBA Operating
2007Australia, Melbourne
AS 3.0 6.9 216 5.4m*14 14 DBA Operating
Existing Third Generation Low- & Medium-Energy Synchrotron Facilities
ALS, TLS, ELETTRA, PLS, SLS, CLS, SPEAR3, SOLEIL, Diamond, AS
Year of Operat
-ionLocation Accelerator
Energy
[GeV]
Emittance[nm-rad]
Circum-ference
[m]
Straight Sectionsm*section
UnitBeamline
sStatus
2009 China, Shanghai SSRF 3.5 3.9 432 12m*4+6.5m*16 20 DBA Operating
2010 Spain, Barcelona ALBA 3.0 4.3 268.88m*4+4.3m*12+2.3
m*816 DBA
7 on day 1
(up to 30)
Operating
2012 Korea, Pohang PLS-II 3.0 5.9 281.82 6.86m*10+3.1m*11 Operating
2012 Japan, Nagoya CJSRF 1.2 53 72 5.4m*4Under
construction
2013 China, Hefei HLS-II 0.8 36 66.13 4m*4+2.3m*4Under
construction
2014 Taiwan, Hsinchu TPS 3.0 1.6 518.4 12m*6+7m*18 24 DBA 46Under
construction
2014 USA, Brookhaven NSLS II 3.0 0.55 792 9.3m*15+6.6m*15 30 DBAspace for at least
58
Underconstruction
2015 Sweden, MAX-LabMAX-IV
(storage 1)3.0 0.2 - 0.3 528 4.728m*20+1.3m*40 20 MBA
Underconstruction
2015 Sweden, MAX-LabMAX-IV
(storage 2)1.5 6 96 3.5m*12 12 DBA
Underconstruction
2015 Jordan, Amman SESAME 2.5 26 133.12 4.4m*8+2.4m*8 12 DBAUnder
construction
2016Brazil, Campinas (LNLS)
SIRIUS 3.01.9
(Eff. Emit.)460.5 9.4m*10+5m*10 20 TBA up to 45
Underconstruction
New Additions of Synchrotron Facilities
SSRF, ALBA, PLS-II, CJSRF, HLSL-II, TPS, NSLS-II, MAX-IV, SESAME, SIRIUS
Year of Operat
-ionLocation Accelerator
Energy[GeV]
Emittance
[nm-rad]
Circum-ference
[m]
Straight Sectionsm*section
Unit Beamlines Status
2018 Iran, Tehran ILSF 3.0 3.28 297.68m*4+4m*20+2.82m*
12In planning
Armenia, Yerevan
CANDLE 3.0 8.4 216 4.8m*16 16 DBA In planning
Turkey, Kütahya TAC 4.5 1.28 991.08 8m*18+6m*18 In planning
Japan, Tohoku LSEJ 3.0 1.862 289.2 5m*12 In planning
Japan, Hyogo SPring-8 II 6.0 0.067 1436 6.6m*44+30m*4 In planning
China, Beijing BAPS 5.0 1 1200 6.9m*44+14m*4 In planning
New Additions of Synchrotron Facilities (in planning)
ILSF, CANDLE, TAC, LSEJ, Spring-II, BAPS,……….
Shanghai Synchrotron Radiation Facility (SSRF) – Shanghai, China
7 initial beamlines:
•BL17U1 – Macromolecular Crystallography
•BL14W1 – XAFS
•BL14B1 – Diffraction
•BL15U1 – Hard X-ray Micro-focus
•BL10W1 – X-ray Imaging and Biomedical Application
•BL16B1 – Small Angle X-ray Scattering
•BL08U1-A – Soft X-ray Spectromicroscopy
•BL08U1-B – X-ray Interference Lithography
6 new beamlines under construction:
•Protein Micro-crystallography
•Protein Complex Crystallography
•High-throughput Protein Crystallography
•BioSAXS
•Infrared Spectroscopy and Imaging
•Dreamline (User funded soft X-ray BL)
(Completion expected in 2013)
Accelerator Layout
http://ssrf.sinap.ac.cn/english/2/Layout.htm
Energy
[GeV]
Emittance
[nm-rad]
Circumference
[m]
Straight Sections
m*sectionUnit
3.5 3.9 43212m*4+6.5m*
1620 DBA
2009
Shanghai Synchrotron Radiation Facility (SSRF) – Shanghai, China (continued)
Campus
New programs at SSRF:
•SSRF Phase II project:
Program to build a big bunch of new beamlines
In preparation and will soon be submitted for approval by the government
•Five user funded beamlines:
In design stage
Waiting for approval
•Soft X-ray FEL facility (Shanghai Soft-X-ray Free-Electron Laser Test Facility (SXFEL))
To be built adjacent to SSRF
By 2020, there will be
•About 40 beamlines at SSRF
•FEL facility
http://ssrf.sinap.ac.cn/english/1/Campus.htm
(ALBA) – Barcelona, Spain
Energy[GeV]
Emittance
[nm-rad]
Circumference[m]
Straight Sectionsm*section
UnitBeamline
s
3.0 4.3 268.88m*4+4.3m*12+2.6
m*816
DBA
7 on day 1
(up to 30)
http://www.cells.es/Divisions/Accelerators
Machine Parameters
http://www.cells.es/AboutUs
Seven beamlines for first phase:
•BL04 - MSPD: Materials Science and Powder Diffraction
•BL09 - MISTRAL: X-Ray Microscopy
•BL11 - NCD: Non-Crystalline Diffraction
•BL13 - XALOC: Macromolecular Crystallography
•BL22 - CLÆSS: Core Level Absorption & Emission Spectroscopies
•BL24 - CIRCE: Photoemission Spectroscopy and Microscopy
•BL29 - BOREAS: Resonant Absorption and Scattering (BOREAS - Available to users on May 7, 2012)
2010
Pohang Light Source II (PLS-II) – Pohang, Korea
http://paleng.postech.ac.kr/
Aerial View of PAL
http://paleng.postech.ac.kr/
Energy[GeV]
Emittance[nm-rad]
Circumference[m]
Straight Sectionsm*section
3.0 5.9 281.82 6.86m*10+3.1m*11
http://paleng.postech.ac.kr/
http://aappsbulletin.org/myboard/read.php?id=40&Page=1&Board=featurearticles&FindIt=&FindText=
Future View of PAL with PLS-II and PAL XFEL sites.
• PLS-II project started in January 2009.
• PLS-II was opened to users on March 21, 2012.
2012
Central Japan Synchrotron Radiation Facility (CJSRF) – Nagoya, Japan
Accelerator
Six beamlines are scheduled for service in 2012:
1.Hard X-ray XAFS
2.Soft X-ray XAFS
3.Soft X-ray to ultraviolet spectroscopy
4.Small angle scattering
5.X-ray diffraction
6.X-ray fluorescence analysis
Beamline Layouthttp://www.astf-kha.jp/synchrotron/en/userguide/gaiyou/
http://www.astf-kha.jp/synchrotron/en/userguide/kougen/
Energy[GeV]
Emittance[nm-rad]
Circumference
[m]
Straight Sectionsm*section
1.2 53 72 5.4m*4
2012
National Synchrotron Light Source II (NSLS-II) – Brookhaven, USA
Research focus:
•Clean and Affordable Energy
•Molecular Electronics
•Self-assembly
•High-Temperature Superconductors
Scientific opportunities:
•Biology and Soft Matter Science
•Chemical Science and Catalysis
•Condensed Matter and Materials Physics
•Environmental and Heterogeneous Materials Science
•Materials Science and Engineering
•Nanoscience
http://www.bnl.gov/ps/nsls2/about-NSLS-II.asp
Energy [GeV]
3.0
Emittance [nm-rad]
0.55
Circumference [m]
792
Straight Sections
m*section9.3m*15+6.6m*15
Unit 30 DBA
Beamlines space for at least 58
2014
National Synchrotron Light Source II (NSLS-II) – Brookhaven, USA (continued)
Science at NSLS-II:
•Hard X-ray Nanoprobe
•Coherent X-Ray Scattering
•X-Ray Photon Correlation Spectroscopy (XPCS)
•Small Angle X-Ray Scattering (SAXS)
•Inelastic X-Ray Scattering (IXS)
•Soft X-Ray Resonant Scattering: XRMS and RIXS
•Soft X-Ray Coherent Scattering and Imaging
•Macromolecular Crystallography
•High Energy X-Rays
•Hard X-Ray Imaging
Taiwan Photon Source (TPS) – Hsinchu, Taiwan
Natural emittance: 1.6 nm-radStraight sections: 7 m (x 18); 12 m (x 6)Full capacity: 48 ports
3 GeV, 518.4 m, 500 mA
Taiwan Light Source (TLS)
Administration and Operation Center
Academic Activity Center
3D Aerial View of NSRRC
2014
Outer diameter 210 m ; Inner diameter 129 mBuilding
No. 101, Hsin-Ann Road, Hsinchu, TaiwanLocation
750 kW (3 SRF cavities) RF power
2.8~3.5 MV (3 SRF cavities) RF gap voltage
500 MHz RF frequency
1 % Coupling
1.6 nm·rad at 3 GeV (Distributed dispersion) Emittance
48 Bending magnets
12 m x 6 ( σv = 12 μm, σh = 160 μm) 7 m x 18 ( σv = 5 μm, σh = 120 μm)
Straight sections
24-cell DBA Lattice
496.8 m (h = 828 = 22·32·23, dia.= 158.1 m) BR circumference
518.4 m (h = 864 = 25·33 , dia.= 165.0 m) SR circumference
500 mA at 3 GeV (Top-up injection) Current
3 GeV (maximum 3.3 GeV) Energy
Major Parameters of Taiwan Photon Source
Taiwan Photon Source (TPS) – Hsinchu, Taiwan (continued)
TPS & TLS Lattice Diagram
Taiwan Photon Source (TPS) – Hsinchu, Taiwan (continued)
Brightness Comparison of TLS and TPS
The X-ray spectrum (photon energy 8 keV~70 keV):
the brilliance of bending magnet increases by >102.
the brilliance of bending IDs increases by 4~6 orders of mag.
TPSTLS
Taiwan Photon Source (TPS) – Hsinchu, Taiwan (continued)
101 102 103 1041012
1013
1014
1015
1016
1017
1018
1019
Bri
llian
ce (P
hoto
n/s/
0.1%
bw/m
m2 /m
r2 /0.3
6A)
Photon Energy (eV)
W200
SWLS
U50
SW60
EPU56
U90
IASW
102 103 104
1019
1020
1021
EPU46 -3.8m
EPU48-3.25m x2
IU22-2m
IU22-3m x2
Bri
llian
ce (
Phot
on/s
/0.1
%bw
/mm
2 /mr2 /0
.5A
)
Photon Energy (eV)
IU22 @ gap=5 mm
Taiwan Photon Source (TPS) – Hsinchu, Taiwan (continued)
µ-focus macromolecular crystallography (2013)(微聚焦巨分子結晶學光束線 )
High resolution inelastic soft-x-ray scattering (2013)(高解析非彈性軟 X光散射學光束線 )
Sub-µ soft x-ray photoelectron & fluorescence emission (2013)(次微米軟 X 光能譜學光束線 )
Coherent x-ray scattering (SAXS/XPCS) (2014)(軟物質小角度散射學光束線 )
Sub-µ x-ray diffraction (2014)(次微米繞射光束線光束線 )
Nano-probe (2014)(奈米探針光束線 )
Temporal coherent x-ray scattering (2014)(時間同調性散射光束線 )
TPS Phase I Beamlines
Taiwan Photon Source (TPS) – Hsinchu, Taiwan (continued)
101年 10月 3日
MAX IV – Sweden 2015
Graphical Overview of MAX IV Project
Initial MAX IV beamline program:
•BioMAX: for macromolecular crystallography
•VERITAS: for soft X-ray Resonant Inelastic X-ray Scattering (RIXS)
•HIPPIE: for electron spectroscopy
•NanoMAX: for micro- and nanobeams
•FemtoMAX: to facilitate studies of the structure and dynamics of materials
•ARPES: for angle resolved photo electron spectroscopy (ARPES)
•XAS: for in-situ hard X-ray spectroscopy
(Start of user operation planned for 2016) Initial MAX IV Beamlines Layout
https://www.maxlab.lu.se/node/647
https://www.maxlab.lu.se/sites/default/files/Oversikt_MIV_100226_eng.pdfEnergy[GeV]
Emittance
[nm-rad]
Circumference
[m]
Straight Sectionsm*section
Unit
3.0 0.2 - 0.3 5284.728m*20+1.3m*4
020 MBA
1.5 6 96 3.5m*12 12 DBA
MAX IV – Sweden (continued)
Overview of MAX IV Facility
The future:
•Multi-bend achromats
•The free electron laser
https://www.maxlab.lu.se/node/206
https://www.maxlab.lu.se/about
Synchrotron-light for Experimental Science and Applications in the Middle East (SESAME) – Amman, Jordan 2015
SESAME Building
Beamline Clock
Phase I beamlines:
1.Protein crystallography
2.X-ray absorption fine structure and X-ray fluorescence spectroscopy
3.Infrared
4.Powder diffraction
5.Small and wide angle X-ray scattering
6.Extreme ultraviolet
7.Soft X-ray ultraviolet
Long-term:
Up to 18 further beamlines can be added
http://www.sesame.org.jo/sesame/
http://www.sesame.org.jo/sesame/images/SESAME_Brochures_and_Posters/X_Proof_Brochure_No07_from_CLD_FINAL.pdf
Energy
[GeV]
Emittance[nm-rad]
Circumference[m]
Straight Sections
m*sectionUnit
2.5 26 133.124.4m*8+2.4m*
812
DBA
Dalian Coherent Extreme-Ultraviolet User Facility – Dalian, China 2015
• Location: Dalian BEST City
• Budget: RMB$1.4 billion
• Range: 50 – 150 nm
• Schedule:
Approval of FEL project: 2011
Official launch of project: March 2012
Completion of device: 2015
• After completion, it will be unique in the world of basic science experiment platform.
SIRIUS – Campinas, Brazil 2016
• Up to 45 beamlines
• The conceptual design of the 13 lines of light began at the end of 2011
SIRIUS will replace the current source operated by the Brazilian
Synchrotron Light Laboratory (LNLS) in Campinas
CNPEM campus
http://www.lnls.br/
http://www.lnls.br/blog/2011/10/24/sirius-new-brazilian-synchrotron-light-source/
Energy[GeV]
Emittance[nm-rad]
Circumference
[m]
Straight Sectionsm*section
Unit Beamlines
3.01.9
(Eff. Emit.)460.5 9.4m*10+5m*10 20 TBA up to 45