A list of particle accelerators used for particle physics experiments. Some early particle accelerators that more properly did nuclear physics, but existed prior to the separation of particle physics from that field, are also included. Although a modern accelerator complex usually has several stages of accelerators, only accelerators whose output has been used directly for experiments are listed.
Contents |
These all used single beams with fixed targets. They tended to have very briefly run, inexpensive, and unnamed experiments.
Accelerator | Location | Years of operation |
Shape | Accelerated Particle | Kinetic Energy |
Notes and discoveries made |
---|---|---|---|---|---|---|
23 cm cyclotron | University of California, Berkeley | 1931 | Circular | H2+ | 1.0 MeV | Proof of concept |
28 cm cyclotron | University of California, Berkeley | 1932 | Circular | Proton | 1.2 MeV | |
68 cm cyclotron | University of California, Berkeley | 1932-1936 | Circular | Deuteron | 4.8 MeV | Investigated deuteron-nucleus interactions |
94 cm cyclotron | University of California, Berkeley | 1937-1938 | Circular | Deuteron | 8 MeV | Discovered many isotopes |
152 cm cyclotron | University of California, Berkeley | 1939- | Circular | Deuteron | 16 MeV | Discovered many isotopes |
467 cm cyclotron | Berkeley Rad Lab[1] | 1942- | Circular | Various | >100 MeV | Research on uranium isotope separation |
Calutrons | Oak Ridge National Laboratory | 1943- | "Horseshoe" | Uranium nuclei |
Used to separate isotopes for the Manhattan project | |
95-inch cyclotron | Harvard Cyclotron Laboratory | 1949 - 2002 | Circular | Proton | 160 MeV | Used for nuclear physics 1949 - ~ 1961, development of clinical proton therapy until 2002 |
TRIUMF Cyclotron | TRIUMF, Vancouver BC | 1974 - | Circular | H- ion | 500 MeV | Not an early accelerator, but a re-envisioning of the cyclotron concept, having multiple beam extractions, and hosting many multi-year experiments. Since its inception, has been the world's largest cyclotron, at 17.9m; six sector magnet configuration, with curving outer tips of pole pieces reflecting the effect of relativity on the cyclotron relation at its full acceleration velocity |
[1] First accelerator built at the current Lawrence Berkeley National Laboratory site, then known as the Berkeley Radiation Laboratory ("Rad Lab" for short)
Accelerator | Location | Years of operation |
Shape and size |
Accelerated particle |
Kinetic Energy |
Notes and discoveries made |
---|---|---|---|---|---|---|
Cockcroft and Walton's electrostatic accelerator |
Cavendish Laboratory | 1932 | See Cockroft- Walton generator |
Proton | 0.7 MeV | First to artificially split the nucleus (Lithium) |
Accelerator | Location | Years of operation |
Shape and size |
Accelerated particle |
Kinetic Energy |
Notes and discoveries made |
---|---|---|---|---|---|---|
Cosmotron | Brookhaven National Laboratory |
1953-1968 | Circular ring (72 meters around) |
Proton | 3.3 GeV | Discovery of V particles, first artificial production of some mesons. |
Birmingham Synchrotron |
University of Birmingham | 1953-1967 | Proton | 1 GeV | ||
Bevatron | Berkeley Rad Lab i.e. LBNL | 1954-~1970 | "Race track" | Proton | 6.2 GeV | strange particle experiments, Antiproton and antineutron discovered, resonances discovered |
Bevalac, combination of SuperHILAC linear accelerator, a diverting tube, then the Bevatron | Berkeley Rad Lab i.e. LBNL | ~1970-1993 | linear accelerator followed by "Race track" | any and all sufficiently stable nuclei could be accelerated | observation of compressed nuclear matter. Depositing ions in tumors in cancer research. | |
Saturne | Saclay, France | 3 GeV | ||||
Synchrophasotron | Dubna, Russia | December 1949-present | 10 GeV | |||
Zero Gradient Synchrotron |
Argonne National Laboratory |
1963-1979 | 12.5 GeV | |||
Proton Synchrotron | CERN | 1959-present | Circular ring (600 meters around) |
Proton | 28 GeV | Used to feed ISR, SPS, LHC |
Alternating Gradient Synchrotron | Brookhaven National Laboratory |
1960- | Proton | 33 GeV | J/Ψ, muon neutrino, CP violation in kaons, injects polarized protons into RHIC |
More modern accelerators that were also run in fixed target mode; often, they will also have been run as colliders, or accelerated particles for use in subsequently built colliders.
Accelerator | Location | Years of operation |
Shape and size |
Accelerated particle |
Kinetic Energy |
Experiments | Notes |
---|---|---|---|---|---|---|---|
Cambridge Electron Accelerator | Harvard University and MIT, Cambridge, MA | 1962-1974[1] | 236 ft diameter synchrotron[2] | Electrons | 6 GeV | [1] | |
SLAC Linac | SLAC National Accelerator Laboratory | 1966-present | 3 km linear accelerator |
Electron/ Positron |
50 GeV | Repeatedly upgraded, used to feed PEP, SPEAR, SLC, and PEP-II | |
Fermilab Booster | Fermilab | 1970-2011 | Circular Synchrotron | Protons | 8 GeV | MiniBooNE | |
Fermilab Main Injector | Fermilab | 1995-2011 | Circular Synchrotron | Protons and antiprotons | 150 GeV | MINOS | |
Fermilab Main Ring | Fermilab | 1970-1995 | Circular Synchrotron | Protons and antiprotons | 400 GeV (until 1979), 150 GeV thereafter | ||
Super Proton Synchrotron | CERN | 1980-present | Circular Synchrotron | Protons and ions | 480 GeV | COMPASS, OPERA and ICARUS at Laboratori Nazionali del Gran Sasso | |
Bates Linear Accelerator | Middleton, MA | 1967-2005 | 500 MeV recirculating linac and storage ring | polarized electrons | 1 GeV | ||
Continuous Electron Beam Accelerator Facility (CEBAF) | Thomas Jefferson National Accelerator Facility, Newport News, VA | 1995-present | 6 GeV recirculating linac (upgrading to 12 GeV) | polarized electrons | 6 GeV | DVCS, PrimEx II, Qweak | First large-scale deployment of superconducting RF technology. |
ELSA | Physikalisches Institut der Universität Bonn, Germany | 1987-present | synchrotron and stretcher | (polarized) electrons | 3.5 GeV | Crystal Barrel | |
ISIS neutron source | Rutherford Appleton Laboratory, Chilton, | 1984-present | H- Linac followed by proton RCS | Protons | 800 MeV | Highest power operational pulsed proton beam in the world | |
MAMI | Mainz, Germany | 1.5 GeV accelerator | polarized electrons | ||||
Tevatron | Fermilab | 1983-2011 | Superconducting Circular Synchrotron | Protons | 980 GeV | ||
Spallation Neutron Source | Oak Ridge National Laboratory | 2006 - Present | Linear (335 m) and Circular (248 m) | Protons | 800 MeV - 1 GeV |
||
Universal Linear Accelerator (UNILAC) | GSI Helmholtz Centre for Heavy Ion Research, Darmstadt, Germany | 1974 - Present | Linear (120 m) | Ions of all naturally occurring elements | |||
Schwerionensynchrotron (SIS18) | GSI Helmholtz Centre for Heavy Ion Research, Darmstadt, Germany | 1990 - Present | Synchrotron with 271 m circumference | Ions of all naturally occurring elements | U: 50-1000 MeV/u Ne: 50-2000 MeV/u p: 4,5 GeV |
||
High Current Proton Accelerator | Neutron Materials Research, Proton Radiography, High Energy Neutron Research, Ultra Cold Neutrons | Los Alamos Neutron Science Center originally Los Alamos Meson Physics Facility | Los Alamos National Laboratory | 1972 - Present | Linear (800 meters) and Circular (30 m) | Protons | 800 MeV |
Accelerator | Location | Years of operation |
Shape and circumference |
Electron energy |
Positron energy |
Experiments | Notable Discoveries |
---|---|---|---|---|---|---|---|
AdA | Frascati, Italy; Orsay, France | 1961-1964 | Circular, 3 meters | 250 MeV | 250 MeV | Touschek effect (1963); first e−e− interactions recorded (1964) | |
Princeton-Stanford (e−e−) | Stanford, California | 1962-1967 | Two-ring, 12 m | 300 MeV | 300 MeV | e−e− interactions | |
VEP-1 (e−e−) | INP, Novosibirsk, Soviet Union | 1964-1968 | Two-ring, 2.70 m | 130 MeV | 130 MeV | e−e− scattering; QED radiative effects confirmed | |
VEPP-2 | INP, Novosibirsk, Soviet Union | 1965-1974 | Circular, 11.5 m | 700 MeV | 700 MeV | OLYA, CMD | multihadron production (1966), e+e−→φ (1966), e+e−→γγ (1971) |
SPEAR | SLAC | 1972-1990(?) | Mark I, Mark II, Mark III | Discovery of Charmonium states | |||
VEPP-2M | BINP, Novosibirsk | 1974-2000 | Circular, 17.88 m | 700 MeV | 700 MeV | ND, SND, CMD-2 | e+e− cross sections, radiative decays of ρ, ω, and φ mesons |
DORIS | DESY | 1974-1993 | Circular, 300m | 5 GeV | 5 GeV | ARGUS, Crystal Ball, DASP, PLUTO | Oscillation in neutral B mesons |
PETRA | DESY | 1978-1986 | Circular, 2km | 20 GeV | 20 GeV | JADE, MARK-J, PLUTO, TASSO | Discovery of the gluon in three jet events |
CESR | Cornell University | 1979-2002 | Circular, 768m | 6 GeV | 6 GeV | CUSB, CHESS, CLEO, CLEO-2, CLEO-2.5, CLEO-3 | First observation of B decay, charmless and "radiative penguin" B decays |
PEP | SLAC | 1980-1990(?) | Mark II | ||||
SLC | SLAC | 1988-1998(?) | Addition to SLAC Linac |
45 GeV | 45 GeV | SLD, Mark II | First linear collider |
LEP | CERN | 1989-2000 | Circular, 27km | 104 GeV | 104 GeV | Aleph, Delphi, Opal, L3 | Only 3 light (m ≤ mZ/2) weakly interacting neutrinos exist, implying only three generations of quarks and leptons |
BEPC | China | 1989-2004 | Circular, 240m | 2.2 GeV | 2.2 GeV | Beijing Spectrometer (I and II) | |
VEPP-4M | BINP, Novosibirsk | 1994- | Circular, 366m | 6.0 GeV | 6.0 GeV | KEDR | Precise measurement of Υ-meson masses |
PEP-II | SLAC | 1998-2008 | Circular, 2.2 km | 9 GeV | 3.1 GeV | BaBar | Discovery of CP violation in B meson system |
KEKB | KEK | 1999-2009 | Circular, 3km | 8.0 GeV | 3.5 GeV | Belle | Discovery of CP violation in B meson system |
DAΦNE | Frascati, Italy | 1999- | Circular, 98m | 0.7 GeV | 0.7 GeV | KLOE | Crab-waist collisions (2007) |
CESR-c | Cornell University | 2002-2008 | Circular, 768m | 6 GeV | 6 GeV | CHESS, CLEO-c | |
VEPP-2000 | BINP, Novosibirsk | 2006- | Circular, 24.4m | 1.0 GeV | 1.0 GeV | SND, CMD-3 | Round beams (2007) |
BEPC II | China | 2008- | Circular, 240m | 3.7 GeV | 3.7 GeV | Beijing Spectrometer III |
Accelerator | Location | Years of operation |
Shape and size |
Particles collided |
Beam energy |
Experiments |
---|---|---|---|---|---|---|
Intersecting Storage Rings |
CERN | 1971-1984 | Circular rings (948 m around) |
Proton/ Proton |
31.5 GeV | |
Super Proton Synchrotron/SppS |
CERN | 1981-1984 | Circular ring (6.9 km around) |
Proton/ Antiproton |
270-315 GeV | UA1, UA2 |
Tevatron Run I |
Fermilab | 1992-1995 | Circular ring (6.3 km around) |
Proton/ Antiproton |
900 GeV | CDF, D0 |
Tevatron Run II |
Fermilab | 2001-2011 | Circular ring (6.3 km around) |
Proton/ Antiproton |
980 GeV | CDF, D0 |
RHIC proton+proton mode |
BNL | 2000-present | Hexagonal rings (3.8 km circumference) |
Polarized Proton/ Proton |
100-250 GeV | PHENIX, STAR |
Large Hadron Collider |
CERN | 2008-present | Circular rings (27 km around) |
Proton/ Proton |
3.5 TeV (design: 7 TeV) |
ALICE, ATLAS, CMS, LHCb, LHCf, TOTEM |
Accelerator | Location | Years of operation |
Shape and size |
Electron energy |
Proton energy |
Experiments |
---|---|---|---|---|---|---|
HERA | DESY | 1992(-2007) | Circular ring (6336 meters around) |
27.5 GeV | 920 GeV | H1, ZEUS, HERMES, HERA-B |
Accelerator | Location | Years of operation |
Shape and size |
Ions collided |
Ion energy |
Experiments |
---|---|---|---|---|---|---|
Relativistic Heavy Ion Collider | Brookhaven National Laboratory, New York | 2000-present | Hexagonal rings (3.8 km circumference) |
d-197 Au79+; 63 Cu29+-63 Cu29+; 197 Au79+-197 Au79+ |
4.6-100 GeV per nucleon | STAR, PHENIX, Brahms, Phobos |
Large Hadron Collider, ion mode |
CERN | 2008-present | Circular rings (27 km circumference) |
208 Pb82+-208 Pb82+ |
2.76 TeV per nucleon | ALICE, ATLAS, CMS |
Besides the real accelerators listed above, there are hypothetical accelerators often used as hypothetical examples or optimistic projects by particle physicists.