List of synchrotron radiation facilities

Last updated

This is a table of synchrotrons and storage rings used as synchrotron radiation sources, and free electron lasers.

Facility nameLocationCountryEnergy (GeV)Circumference or length (m)Commissioned for synchrotron radiation studiesDecommissioned
National Synchrotron Light Source (NSLS-II) Brookhaven National Laboratory US37922015
Synchrotron Ultraviolet Radiation Facility (SURF) National Institute of Standards and Technology, Gaithersburg, Maryland US0.181961
SURF II storage ring, Synchrotron Ultraviolet Radiation Facility National Institute of Standards and Technology, Gaithersburg, Maryland US0.251974
SURF III Synchrotron Ultraviolet Radiation Facility National Institute of Standards and Technology, Gaithersburg, Maryland US0.4165.272000
Frascati Synchrotron Radiation Collaboration 1 GeV electronsynchrotron (built in 1958) at

Laboratori Nazionali di Frascati

Italy11219631970
Institute for Nuclear Studies-Synchrotron Orbital Radiation (INS-SOR)TokyoJapan0.751965
Storage ring of INS-SOR (Institute for Nuclear Studies-Synchrotron Orbital Radiation) TokyoJapan0.31974
DESY (Deutsches Elektronen Synchrotron) DESY Germany7.419671987
DORIS (Doppel-Ring-Speicher) DESY Germany3.5 (5 in 1978)28919741993
DORIS III DESY Germany528919932012
PETRA II DESY Germany12230419952007
PETRA III DESY Germany6.023042009
European X-ray Free Electron Laser (EuXFEL) Schenefeld, near DESY Germany17.534002017
Tantalus at the Synchrotron Radiation Center University of Wisconsin US0.249.3819681987
Synchrotron Radiation Center(SRC) University of Wisconsin US112119872014
Solidi Roma Synchrotron Radiation Facility Recycled 1GeV electronsynchrotron at Laboratori Nazionali di Frascati Italy11219721975
Stanford Synchrotron Radiation Lightsource (SSRL)SPEAR storage ring at SLAC National Accelerator Laboratory US32341973
Linac Coherent Light Source (LCLS) SLAC National Accelerator Laboratory US830002007
Anneau de Collisions d'Orsay (ACO) Orsay France0.5419731988
Cornell High Energy Synchrotron Source (CHESS) Cornell University, Ithaca, NYUS6.07681979
Progetto Utilizzazione Luce di Sincrotrone (PULS)recycled Adone storage ring with wiggler (built in 1968) at Laboratori Nazionali di Frascati Italy1.533.519801993
Synchrotron Radiation Source Daresbury Laboratory UK29619812008
DCI storage ring – LURE (Laboratoire pour l'Utilisation du Rayonnement Electromagnétique) Orsay France119812006
National Synchrotron Light Source (NSLS) Brookhaven National Laboratory US2.817019822014
Photon Factory (PF) at KEK Tsukuba Japan2.51871982
Super ACO-Laboratoire pour l'Utilisation du Rayonnement Electromagnétique (LURE) Orsay France0.819872006
ASTRID Aarhus University Denmark0.584019912012
ASTRID 2 Aarhus University Denmark0.5845.72013
National Synchrotron Radiation Laboratory (NSRL) University of Science and Technology China, Hefei China0.866.131991
Beijing Synchrotron Radiation Facility (BSRF) Institute of High Energy Physics, Chinese Academy of Sciences, BeijingChina2.51991
European Synchrotron Radiation Facility (ESRF) Grenoble France684419922019
European Synchrotron Radiation Facility – Extremely Brilliant Source (ESRF-EBS) Grenoble France68442020
Advanced Light Source (ALS) Lawrence Berkeley Laboratory US1.9196.81993
ELETTRA Trieste Italy2-2.42601993
Advanced Photon Source (APS) Argonne National Laboratory, Argonne, ILUS7.011041995
Kurchatov Synchrotron Radiation Source (SIBIR-1, SIBIR-2) Kurchatov Institute, MoscowRussia2.51241999
LNLS LNLS in Campinas, São Paulo Brazil1.3793.219972019
SPring-8 RIKEN Japan814361997
MAX-I MAX-lab Sweden0.553019862015
MAX-II MAX-lab Sweden1.59019972015
MAX-III MAX-lab Sweden0.73620082015
MAX IV 1.5 GeV Storage Ring MAX IV Sweden1.5962016
MAX IV 3 GeV Storage Ring MAX IV Sweden35282016
BESSY II Helmholtz-Zentrum Berlin in BerlinGermany1.72401998
Indus 1 Raja Ramanna Centre for Advanced Technology, Indore India0.4518.961999
DAFNE light Istituto Nazionale di Fisica Nucleare, Frascati Italy0.51321999
Karlsruhe Research Accelerator (KARA) Karlsruhe Institute of Technology Germany2.5110.42000
Swiss Light Source Paul Scherrer Institute Switzerland2.42882001
SwissFEL Paul Scherrer Institute Switzerland2018
Canadian Light Source University of Saskatchewan Canada2.91712004
Synchrotron Light Research Institute  [ th ] (SLRI) Nakhon Ratchasima Thailand1.281.42004
Indus 2 Raja Ramanna Centre for Advanced Technology, Indore India2.51732005
Australian Synchrotron Melbourne Australia32162006
SOLEIL Saint-Aubin, Essonne France 2.753542006
Diamond Light Source Rutherford Appleton Laboratory UK3561.62006
Shanghai Synchrotron Radiation Facility (SSRF)ShanghaiChina3.54322007
Taiwan Light Source National Synchrotron Radiation Research Center, Hsinchu Science Park R.O.C. (Taiwan)1.51201993
Taiwan Photon Source National Synchrotron Radiation Research Center, Hsinchu Science Park R.O.C (Taiwan)3518.42015
Metrology Light Source  [ de ] (MLS) Berlin Germany [1] 0.6482008
Beijing Electron–Positron Collider II (BEPC II) Institute of High Energy Physics, Chinese Academy of Sciences, BeijingChina3.72402008
ALBA Barcelona Synchrotron Park, Cerdanyola del Vallès near Barcelona Spain32702010
Sirius LNLS in Campinas, São Paulo Brazil3518.22018
Synchrotron-Light for Experimental Science and Applications in the Middle East (SESAME) Al Balqa Jordan2.51332016
Iranian Light Source Facility (ILSF) Qazvin Iran3489.6Under Design
Center for Advanced Microstructures and Devices (CAMD) LSU, Louisiana US1.5
Pohang Light Source II  [ ko ] Pohang University of Science and Technology South Korea3.0281.822011
CANDLE Yerevan Armeniaproposed
Centre Laser Infrarouge d'Orsay (CLIO) Laboratoire de Chimie Physique (LCP), Orsay France0.041991
DELTA Technical University of Dortmund Germany1.5115.21999
Hiroshima Synchrotron Radiation Center (HSRC) Hiroshima University, Hiroshima Japan0.7221997
Institute of Free Electron Laser (iFEL) Osaka University, Osaka Japan
IR FEL Research Center (FELSUT) Tokyo University of Science Japan
Medical Synchrotron Radiation Facility National Institute of Radiological Sciences, Inage-ku, Chiba Japan
Nagoya University Small Synchrotron Radiation Facility (NSSR) Nagoya University Japan
Photonics Research Institute Tsukuba Science City Japan
Saga Light Source (SAGA-LS) Tosu, Saga Japan
Ultraviolet Synchrotron Orbital Radiation Facility (UVSOR) National Institutes of Natural Sciences, Okazaki Japan
VSX Light Source University of Tokyo Japan
Free Electron Laser for Infrared eXperiments (FELIX) Radboud University, Nijmegen Netherlands0.015–0.0601991
Dubna Electron Synchrotron (DELSY) JINR, Dubna Russia
Siberian Synchrotron Radiation Centre (SSRC) Budker Institute of Nuclear Physics, Novosibirsk Russia2 - 6 [2] 366 [3] 1973 [2]
Technical Storage Ring Complex (TNK) F.V Lukin Institute, Zelenograd, Moscow [4] Russia0.45 - 2.2 [4]
Singapore Synchrotron Light Source (SSLS) National University of Singapore Singapore0.710.82000
Solaris (synchrotron) Kraków Poland1.5962016
UCSB Center for Terahertz Science and Technology (CTST) University of California, Santa Barbara, Santa Barbara, California US
Duke Free Electron Laser Laboratory (DFELL) Duke University, Durham, North Carolina US0.2 - 1.2107.461994
Jefferson Laboratory Free Electron Laser (Jlab) Thomas Jefferson National Accelerator Facility, Newport News, Virginia US
W. M. Keck Vanderbilt Free-electron Laser Center Vanderbilt University, Nashville, Tennessee US
The African Light Source (AfLS) Conceptual stage

Related Research Articles

<span class="mw-page-title-main">Lodewijk van den Berg</span> Dutch-born American chemical engineer and astronaut (1932–2022)

Lodewijk van den Berg was a Dutch-born American chemical engineer. He studied crystal growth and flew on a 1985 Space Shuttle Challenger mission as a payload specialist.

<span class="mw-page-title-main">Geant4</span> Scientific software for particle physics

Geant4 is a platform for "the simulation of the passage of particles through matter" using Monte Carlo methods. It is the successor of the GEANT series of software toolkits developed by The Geant4 Collaboration, and the first to use object oriented programming. Its development, maintenance and user support are taken care by the international Geant4 Collaboration. Application areas include high energy physics and nuclear experiments, accelerator and space physics studies. The software is used by a number of research projects around the world.

<span class="mw-page-title-main">DELPHI experiment</span>

DELPHI was one of the four main detectors of the Large Electron–Positron Collider (LEP) at CERN, one of the largest particle accelerators ever made. Like the other three detectors, it recorded and analyzed the result of the collision between LEP's colliding particle beams. The specific focus of DELPHI was on particle identification, three-dimensional information, high granularity (detail), and precise vertex determination.

<span class="mw-page-title-main">Lazarus effect</span>

The Lazarus effect refers to semiconductor detectors; when these are used in harsh radiation environments, defects begin to appear in the semiconductor crystal lattice as atoms become displaced because of the interaction with the high-energy traversing particles. These defects, in the form of both lattice vacancies and atoms at interstitial sites, have the effect of temporarily trapping the electrons and holes which are created when ionizing particles pass through the detector. Since it is these electrons and holes drifting in an electric field which produce a signal that announces the passage of a particle, when large amounts of defects are produced, the detector signal can be strongly reduced leading to an unusable (dead) detector.

A wavelength shifter is a photofluorescent material that absorbs higher frequency photons and emits lower frequency photons. The material absorbs one photon, and emits one or multiple lower-energy photons. The relaxation time of the excited molecule is usually in the order of nanoseconds.

A clover detector is a gamma-ray detector that consists of 4 coaxial N-type high purity germanium (Ge) crystals each machined to shape and mounted in a common cryostat to form a structure resembling a four-leaf clover.

<span class="mw-page-title-main">Detection of internally reflected Cherenkov light</span>

In particle detectors a detection of internally reflected Cherenkov light (DIRC) detector measures the velocity of charged particles and is used for particle identification. It is a design of a ring imaging Cherenkov detector where Cherenkov light that is contained by total internal reflection inside the solid radiator has its angular information preserved until it reaches the light sensors at the detector perimeter.

<span class="mw-page-title-main">Clab</span>

The Clab, also known as Centralt mellanlager för använt kärnbränsle is an interim radioactive waste repository located at Oskarshamn Nuclear Power Plant about 25 km north of Oskarshamn. Clab used to be owned by Oskarshamnsverkets Kraftgrupp AB (OKG) but is now owned by Svensk Kärnbränslehantering Aktiebolag (SKB). It was opened in 1985 for the storage of spent nuclear fuel from all Swedish nuclear power plants. The fuel is stored for 30 to 40 years, in preparation for final storage.

FLUKA is a fully integrated Monte Carlo simulation package for the interaction and transport of particles and nuclei in matter. FLUKA has many applications in particle physics, high energy experimental physics and engineering, shielding, detector and telescope design, cosmic ray studies, dosimetry, medical physics, radiobiology. A recent line of development concerns hadron therapy.

Allchar deposit is a low-temperature hydrothermal gold–arsenic–antimony–thallium deposit in Kavadarci Municipality of North Macedonia. For some time, the thallium-rich part of the deposit was mined. The Crven Dol mine yielded thallium and the ore body still holds estimated amount of 500 t of thallium. The mineral lorandite from this ore deposit can be used to determine the solar neutrino flux.

Neutron spectroscopy is a spectroscopic method of measuring atomic and magnetic motions by measuring the kinetic energy of emitted neutrons. The measured neutrons may be emitted directly, or they may scatter off cold matter before reaching the detector. Inelastic neutron scattering observes the change in the energy of the neutron as it scatters from a sample and can be used to probe a wide variety of different physical phenomena such as the motions of atoms, the rotational modes of molecules, sound modes and molecular vibrations, recoil in quantum fluids, magnetic and quantum excitations or even electronic transitions.

<span class="mw-page-title-main">Neutron imaging</span>

Neutron imaging is the process of making an image with neutrons. The resulting image is based on the neutron attenuation properties of the imaged object. The resulting images have much in common with industrial X-ray images, but since the image is based on neutron attenuating properties instead of X-ray attenuation properties, some things easily visible with neutron imaging may be very challenging or impossible to see with X-ray imaging techniques.

Gadolinium oxyorthosilicate is a type of scintillating inorganic crystal used for imaging in nuclear medicine and for calorimetry in particle physics.

The Virtual Instrumentation Tool for the ESS (VITESS) is an open source software package for the simulation of neutron scattering experiments. The software is maintained and developed by the Helmholtz-Zentrum Berlin für Materialien und Energie (HZB), the former Hahn-Meitner-Institur HMI, and available for Windows, Linux and Macintosh on the VITESS homepage. It is widely used for simulation of existing neutron scattering instruments as well as for the development of new instruments.

<span class="mw-page-title-main">Kim Sun-kee</span>

Kim Sun-kee is a South Korean physicist. He is professor in Seoul National University and director of the Korea Invisible Mass Search. He was the first director of the Rare Isotope Science Project within the Institute for Basic Science and is a member of the Korean Academy of Science and Technology.

Self Powered Neutron Detector (SPND) is a neutron detector used in nuclear fission reactors. It is a compact device extensively used worldwide for mapping of neutron flux, helping the reactor-operators in maintaining the neutron economy. It gives a direct current signal proportional to the incident flux of neutrons, due to production of negative beta particles or Compton electrons in the heart of the device.

<span class="mw-page-title-main">AMY (scientific instrument)</span>

The AMY detector was used by particle physicists at the TRISTAN electron-positron collider at KEK in Japan between 1984 and 1995 to search for new particles and perform precision studies of the strong and electroweak forces.

Hybrid pixel detectors are a type of ionizing radiation detector consisting of an array of diodes based on semiconductor technology and their associated electronics. The term “hybrid” stems from the fact that the two main elements from which these devices are built, the semiconductor sensor and the readout chip, are manufactured independently and later electrically coupled by means of a bump-bonding process. Ionizing particles are detected as they produce electron-hole pairs through their interaction with the sensor element, usually made of doped silicon or cadmium telluride. The readout ASIC is segmented into pixels containing the necessary electronics to amplify and measure the electrical signals induced by the incoming particles in the sensor layer.

Linda Gail Stutte is an experimental elementary particle physicist. After an appointment as a postdoc at Caltech in 1974–76, Stutte was a research staff scientist at the Fermi National Accelerator Laboratory from 1976 through her retirement in 2007. She is known for work on neutrino experiments and her expertise with Fermliab neutrino beam facilities.

Associated particle imaging (API), sometimes referred to as the tagged neutron method (TNM), is a three dimensional imaging technique that maps the distribution of elements within an object. In associated particle imaging, deuterium-tritium fusion reactions each produce a fast neutron and an associated particle, which travel in opposite directions in the center-of-mass frame. By measuring the timing and position of the associated particle, the trajectory of the neutron may be inferred. The neutron may then enter an object of interest where it is likely to undergo inelastic scattering. This produces one or more gamma-rays of specific energies dependent on the element that the neutron scatters off of. By measuring the gamma-ray energy, the element may be identified. The timing of the gamma-ray coinciding with an associated particle allows the 3D imaging of an object's elemental composition. This technique has applications in agriculture, national security, and diamond detection, among other areas.

References

  1. "7.14 Synchrotron Radiation Sources". www.ptb.de. 2017-01-23. Retrieved 2018-08-13.
  2. 1 2 Ancharov, A.I.; Baryshev, V.B.; Chernov, V.A.; Gentselev, A.N.; Goldenberg, B.G.; Kochubei, D.I.; Korchuganov, V.N.; Kulipanov, G.N.; Kuzin, M.V.; Levichev, E.B.; Mezentsev, N.A.; Mishnev, S.I.; Nikolenko, A.D.; Pindyurin, V.F.; Sheromov, M.A.; Tolochko, B.P.; Sharafutdinov, M.R.; Shmakov, A.N.; Vinokurov, N.A.; Vobly, P.D.; Zolotarev, K.V. (2005-05-01). "Status of the Siberian synchrotron radiation center". Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment. 543 (1): 1–13. Bibcode:2005NIMPA.543....1A. doi:10.1016/j.nima.2005.01.021. ISSN   0168-9002.
  3. "STATUS OF VEPP-4M COLLIDER" (PDF). Proceedings of IPAC2016, Busan, Korea.
  4. 1 2 Belokrinitsky, S.; Churkin, I.; Oleynik, A.; Pekshev, D.; Philipchenko, A.; Rouvinsky, I.; Steshov, A.; Ushakov, V. (2009-05-11). "Modeling and magnetic measurements of TNK synchrotron radiation source magnets". Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment. 603 (1–2): 16–18. Bibcode:2009NIMPA.603...16B. doi:10.1016/j.nima.2008.12.119. ISSN   0168-9002.
  1. Robinson, Arthur L. "HISTORY of SYNCHROTRON RADIATION". X-Ray Data Booklet. Center for X-ray Optics and Advanced Light Source, Lawrence Berkeley National Laboratory. Retrieved 1 May 2015.