List of accelerators in particle physics

Last updated

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

Early accelerators

These all used single beams with fixed targets. They tended to have very briefly run, inexpensive, and unnamed experiments.

Cyclotrons

AcceleratorLocationYears of
operation
ShapeAccelerated ParticleKinetic
Energy
Notes and discoveries made
9-inch cyclotron University of California, Berkeley 1931CircularH+
2
1.0 MeV Proof of concept
11-inch cyclotron University of California, Berkeley1932Circular Proton 1.2 MeV
27-inch cyclotronUniversity of California, Berkeley1932–1936Circular Deuteron 4.8 MeVInvestigated deuteron-nucleus interactions
37-inch cyclotronUniversity of California, Berkeley1937–1938CircularDeuteron8 MeVDiscovered many isotopes
60-inch cyclotronUniversity of California, Berkeley1939–1962[1]CircularDeuteron16 MeVDiscovered many isotopes.
88-inch cyclotronBerkeley Rad Lab, now Lawrence Berkeley National Laboratory1961–PresentCircular (Isochronous)Hydrogen through uraniumMeV to several GeVDiscovered many isotopes. Verified two element discoveries. Performed the world's first single event effects radiation testing in 1979, and tested parts and materials for most US spacecraft since then.
184-inch cyclotronBerkeley Rad Lab1942–1993CircularVariousMeV to GeVResearch on uranium isotope separation
Calutrons Y-12 Plant, Oak Ridge, TN1943–"Horseshoe"Uranium nucleiUsed to separate Uranium 235 isotope for the Manhattan project. After the end of World War II used for separation of medical and other isotopes.
95-inch cyclotron Harvard Cyclotron Laboratory 1949–2002CircularProton160 MeVUsed for nuclear physics 1949 – ~ 1961, development of clinical proton therapy until 2002
JULICForschungszentrum Juelich, Germany1967–presentCircularProton, deuteron75 MeVNow used as a preaccelerator for COSY and irradiation purposes

[1] The magnetic pole pieces and return yoke from the 60-inch cyclotron were later moved to UC Davis and incorporated into a 76-inch isochronous cyclotron which is still in use today [1]

Other early accelerator types

AcceleratorLocationYears of
operation
Shape
and size
Accelerated
particle
Kinetic
Energy
Notes and discoveries made
Linear particle accelerator Aachen University, Germany1928Linear BeamlineIon50 keVProof of concept
Cockcroft and Walton's
electrostatic accelerator
Cavendish Laboratory 1932See Cockroft-
Walton generator
Proton0.7 MeVFirst to artificially split the nucleus (Lithium)
Betatron Siemens-Schuckertwerke, Germany1935CircularElectron1.8 MeVProof of concept

Synchrotrons

AcceleratorLocationYears of
operation
Shape and sizeAccelerated
particle
Kinetic EnergyNotes and discoveries madeINSPIRE link
Cosmotron BNL 1953–1968Circular ring
(72 meters around)
Proton3.3 GeV Discovery of V particles, first artificial production of some mesons INSPIRE
Birmingham Synchrotron University of Birmingham 1953–1967Proton1 GeV
Bevatron Berkeley Rad Lab 1954–~1970"Race track"Proton6.2 GeV Strange particle experiments, antiproton and antineutron discovered, resonances discovered INSPIRE
Bevalac, combination of SuperHILAC linear accelerator, a diverting tube, then the Bevatron Berkeley Rad Lab ~1970–1993Linear accelerator followed by "race track"Any and all sufficiently stable nuclei could be acceleratedObservation of compressed nuclear matter. Depositing ions in tumors in cancer research. INSPIRE
Saturne Saclay, France3 GeV INSPIRE
Synchrophasotron Dubna, RussiaDecember 1957 – 200310 GeV INSPIRE
Zero Gradient Synchrotron ANL 1963–197912.5 GeV INSPIRE
U-70 Proton Synchrotron IHEP, Russia 1967–presentCircular ring
(perimeter around 1.5 km)
Proton70 GeV INSPIRE
Proton Synchrotron CERN 1959–presentCircular ring
(628 meters around)
Proton26 GeVUsed to feed ISR (until 1984), SPS, LHC, AD INSPIRE
Proton Synchrotron Booster CERN 1972–presentCircular SynchrotronProtons1.4 GeVUsed to feed PS, ISOLDE INSPIRE
Super Proton Synchrotron CERN 1976–presentCircular SynchrotronProtons and ions450 GeV COMPASS, OPERA and ICARUS at Laboratori Nazionali del Gran Sasso INSPIRE
Alternating Gradient Synchrotron BNL 1960–presentCircular ring
(808 meters)
Proton (unpolarized and polarized), deuteron, helium-3, copper, gold, uranium33 GeV J/ψ, muon neutrino, CP violation in kaons, injects heavy ions and polarized protons into RHIC INSPIRE
Proton Synchrotron (KEK) KEK 1976–2007Circular ringProton12 GeV
COSY Juelich, Germany1993–presentCircular ring (183.47 m)Protons, Deuterons2.88 GeV The legacy of the experimental hadron physics programme at COSY INSPIRE
ALBA Cerdañola del Vallés, Spain2011–presentCircular ring (270 m)Electrons3 GeV INSPIRE
Sirius São Paulo State, Brazil 2018–presentCircular ring (518.4 m)Electrons, Au, Sn, TiO23 GeV INSPIRE
Australian Synchrotron Monash University, Melbourne 2007–presentCircular ring (216 m)Electrons3 GeV INSPIRE

Fixed-target accelerators

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.

High intensity hadron accelerators (Meson and neutron sources)

AcceleratorLocationYears of
operation
Shape and sizeAccelerated ParticleKinetic EnergyNotes and discoveries madeINSPIRE link
High Current Proton Accelerator Los Alamos Neutron Science Center (originally Los Alamos Meson Physics Facility) Los Alamos National Laboratory 1972–PresentLinear (800 m)
and
Circular (30 m)
Protons800 MeVNeutron materials research, proton radiography, high energy neutron research, ultra cold neutrons INSPIRE
PSI, HIPA High Intensity 590 MeV Proton Accelerator PSI, Villigen, Switzerland1974–present0.8 MeV CW, 72 MeV Injector 2,

590 MeV Ringcyclotron

Protons590 MeV, 2.4 mA, =1.4 MWHighest beam power, used for meson and neutron production with applications in materials science INSPIRE
TRIUMF Cyclotron TRIUMF, Vancouver BC1974–presentCircularH-ion500 MeVWorld's largest cyclotron, at 17.9m INSPIRE
ISIS neutron source Rutherford Appleton Laboratory, Harwell Science and Innovation Campus,

Oxfordshire, United Kingdom

1984–presentH- Linac followed by proton RCSProtons800 MeV INSPIRE
Spallation Neutron Source Oak Ridge National Laboratory 2006–PresentLinear (335 m) and
Circular (248 m)
Protons800 MeV – 1 GeVProduces the most intense pulsed neutron beams in the world for scientific research and industrial development. INSPIRE
J-PARC RCS Tōkai, Ibaraki 2007–PresentTriangular, 348m circumferenceProtons3 GeVUsed for material and life sciences and input to J-PARC main ring INSPIRE

Electron and low intensity hadron accelerators

AcceleratorLocationYears of
operation
Shape
and size
Accelerated
particle
Kinetic
Energy
ExperimentsNotesINSPIRE link
Antiproton Accumulator CERN 1980–1996 Design study INSPIRE
Antiproton collector CERN1986–1996Antiprotons Design study INSPIRE
Nuclotron JINR 1992–presentCircular ringProton and heavy ions12.6 GeV (protons), 4.5 Gev/n (heavy ions) INSPIRE
Antiproton Decelerator CERN2000–presentStorage ringProtons and antiprotons26 GeV ATHENA, ATRAP, ASACUSA, ACE, ALPHA, AEGIS Design study INSPIRE
Low Energy Antiproton Ring CERN1982–1996Antiprotons PS210 Design study INSPIRE
Cambridge Electron Accelerator Harvard University and MIT, Cambridge, MA 1962–1974 [2] 236 ft diameter synchrotron [3] Electrons6 GeV [2]
SLAC Linac SLAC National Accelerator Laboratory 1966–present3 km linear
accelerator
Electron/
Positron
50 GeVRepeatedly upgraded, used to feed PEP, SPEAR, SLC, and PEP-II. Now split into 1 km sections feeding LCLS, FACET & LCLS-II. INSPIRE
Fermilab Booster Fermilab 1970–presentCircular synchrotronProtons8 GeV MiniBooNE INSPIRE
Fermilab Main InjectorFermilab1995–presentCircular synchrotronProtons and antiprotons150 GeV MINOS, MINERνA, NOνA INSPIRE
Fermilab Main RingFermilab1970–1995Circular synchrotronProtons and antiprotons400 GeV (until 1979), 150 GeV thereafter
Electron Synchrotron of Frascati Laboratori Nazionali di Frascati 1959–? (decommissioned)9m circular synchrotronElectron1.1 GeV
Bates Linear AcceleratorMiddleton, MA1967–2005500 MeV recirculating linac and storage ringPolarized electrons1 GeV INSPIRE
Continuous Electron Beam Accelerator Facility (CEBAF) Thomas Jefferson National Accelerator Facility, Newport News, VA1995–present6 GeV recirculating linac (recently upgraded to 12 GeV)Polarized electrons6–12 GeVDVCS, PrimEx II, Qweak, GlueXFirst large-scale deployment of superconducting RF technology. INSPIRE
ELSA Physikalisches Institut der Universität Bonn, Germany1987–presentSynchrotron and stretcher(Polarized) electrons3.5 GeV Crystal Barrel INSPIRE
MAMI Mainz, Germany1975–PresentMultilevel racetrack microtronPolarized electrons1.5 GeV accelerator A1 – Electron Scattering, A2 – Real Photons, A4 – Parity Violation, X1 – X-Ray Radiation INSPIRE
Tevatron Fermilab1983–2011Superconducting circular synchrotronProtons980 GeV INSPIRE
Universal Linear Accelerator (UNILAC) GSI Helmholtz Centre for Heavy Ion Research, Darmstadt, Germany1974–PresentLinear (120 m)Ions of all naturally occurring elements2–11.4  MeV/u INSPIRE
Schwerionensynchrotron (SIS18) GSI Helmholtz Centre for Heavy Ion Research, Darmstadt, Germany1990–PresentSynchrotron with 271 m circumferenceIons of all naturally occurring elementsU: 50–1000 MeV/u
Ne: 50–2000 MeV/u
p: 4,5 GeV
INSPIRE
Experimental Storage Ring (ESR) GSI Helmholtz Centre for Heavy Ion Research, Darmstadt, Germany1990–PresentIons of all naturally occurring elements0.005 – 0.5  GeV/u
J-PARC Main Ring Tōkai, Ibaraki 2009–PresentTriangular, 500m diameterProtons30 GeVJ-PARC Hadron Experimental Facility, T2K Can also provide 8 GeV beam INSPIRE
Low Energy Neutron Source (LENS) Indiana University, Bloomington, Indiana (USA)2004–PresentLinearProtons13 MeV [4] SANS, SESAME, MIS LENS Website Archived 2019-09-28 at the Wayback Machine
Cornell BNL ERL Test Accelerator (CBETA) [5]
Cornell University, Ithaca / NY (USA)2019–PresentEnergy recovery linac with SRF cavities, 4 turns, and all beams in one fixed field alternating-gradient lattice of permanent magnetsElectrons150 MeVA prototype facility for Electron Ion Colliders INSPIRE

Colliders

Electron–positron colliders

AcceleratorLocationYears of
operation
Shape
and circumference
Electron
energy
Positron
energy
ExperimentsNotable DiscoveriesINSPIRE link
AdA LNF, Frascati, Italy; Orsay, France1961–1964Circular, 3 meters250 MeV250 MeV Touschek effect (1963); first e+e interactions recorded (1964) INSPIRE
Princeton-Stanford (ee)Stanford, California1962–1967Two-ring, 12 m300 MeV300 MeVee interactions
VEP-1 (ee) INP, Novosibirsk, Soviet Union1964–1968Two-ring, 2.70 m130 MeV130 MeVee scattering; QED radiative effects confirmed INSPIRE
VEPP-2 INP, Novosibirsk, Soviet Union1965–1974Circular, 11.5 m700 MeV700 MeVOLYA, CMD multihadron production (1966), e+e→φ (1966), e+e→γγ (1971) INSPIRE
ACO LAL, Orsay, France1965–1975Circular, 22 m550 MeV550 MeVρ0, K+K3C, μ+μ, M2N and DM1Vector meson studies; then ACO was used as synchrotron light source until 1988 INSPIRE
SPEAR SLAC1972–1990(?)Circular3 GeV3 GeV Mark I, Mark II, Mark III Discovery of Charmonium states and Tau lepton INSPIRE
VEPP-2M BINP, Novosibirsk 1974–2000Circular, 17.88 m700 MeV700 MeV ND, SND, CMD-2 e+e cross sections, radiative decays of ρ, ω, and φ mesons INSPIRE
DORIS DESY 1974–1993Circular, 300m5 GeV5 GeV ARGUS, Crystal Ball, DASP, PLUTO Oscillation in neutral B mesons INSPIRE
PETRA DESY 1978–1986Circular, 2 km20 GeV20 GeV JADE, MARK-J, CELLO, PLUTO, TASSO Discovery of the gluon in three jet events INSPIRE
CESR Cornell University1979–2002Circular, 768m6 GeV6 GeV CUSB, CHESS, CLEO, CLEO-2, CLEO-2.5, CLEO-3 First observation of B decay, charmless and "radiative penguin" B decays INSPIRE
PEP SLAC 1980–1990(?)Mark II INSPIRE
SLC SLAC 1988–1998(?)Addition to
SLAC Linac
45 GeV45 GeV SLD, Mark IIFirst linear collider INSPIRE
LEP CERN 1989–2000Circular, 27 km104 GeV104 GeV Aleph, Delphi, Opal, L3 Only 3 light (m ≤ mZ/2) weakly interacting neutrinos exist, implying only three generations of quarks and leptons INSPIRE
BEPC Beijing, China1989–2004Circular, 240m2.2 GeV2.2 GeV Beijing Spectrometer (I and II) INSPIRE
VEPP-4M BINP, Novosibirsk 1994–Circular, 366m6.0 GeV6.0 GeV KEDR [ permanent dead link ]Precise measurement of psi-meson masses, two-photon physics
PEP-II SLAC 1998–2008Circular, 2.2 km9 GeV3.1 GeV BaBar Discovery of CP violation in B meson system INSPIRE
KEKB KEK 1999–2009Circular, 3 km8.0 GeV3.5 GeV Belle Discovery of CP violation in B meson system
DAΦNE LNF, Frascati, Italy1999–presentCircular, 98m0.7 GeV0.7 GeV KLOE Crab-waist collisions (2007) INSPIRE
CESR-c Cornell University 2002–2008Circular, 768m6 GeV6 GeV CHESS, CLEO-c INSPIRE
VEPP-2000 BINP, Novosibirsk 2006–Circular, 24.4m1.0 GeV1.0 GeV SND, CMD-3 Round beams (2007)
BEPC II Beijing, China2008–Circular, 240m1.89 GeV1.89 GeV Beijing Spectrometer III
VEPP-5 BINP, Novosibirsk 2015–
ADONE LNF, Frascati, Italy1969–1993Circular, 105m1.5 GeV1.5 GeV
TRISTAN KEK 1987–1995Circular, 3016m30 GeV30 GeV
SuperKEKB KEK 2016–Circular, 3 km7.0 GeV4.0 GeV Belle II

Hadron colliders

AcceleratorLocationYears of
operation
Shape
and size
Particles
collided
Beam
energy
ExperimentsINSPIRE
Intersecting
Storage Rings
CERN1971–1984Circular rings
(948 m around)
Proton/
Proton
31.5 GeV INSPIRE
Super
Proton Synchrotron
/SppS
CERN1981–1984Circular ring
(6.9 km around)
Proton/
Antiproton
270–315 GeV UA1, UA2 INSPIRE
Tevatron
Run I
Fermilab 1992–1995Circular ring
(6.3 km around)
Proton/
Antiproton
900 GeV CDF, D0 INSPIRE
Tevatron
Run II
Fermilab 2001–2011Circular ring
(6.3 km around)
Proton/
Antiproton
980 GeV CDF, D0 INSPIRE
Relativistic Heavy Ion Collider (RHIC)
polarized proton mode
Brookhaven National Laboratory, New York2001–presentHexagonal rings
(3.8 km circumference)
Polarized Proton/
Proton
100–255 GeV PHENIX, STAR INSPIRE
Relativistic Heavy Ion Collider (RHIC)
ion mode
Brookhaven National Laboratory, New York2000–presentHexagonal rings
(3.8 km circumference)
d-197
Au
79+;

63
Cu
29+63
Cu
29+;
63
Cu
29+197
Au
79+;
197
Au
79+197
Au
79+;
238
U
92+238
U
92+

3.85–100 GeV
per nucleon
STAR, PHENIX, BRAHMS, PHOBOS INSPIRE
Large Hadron Collider (LHC)
proton mode
CERN2008–presentCircular rings
(27 km circumference)
Proton/
Proton
6.8 TeV
(design: 7 TeV)
ALICE, ATLAS, CMS, LHCb, LHCf, TOTEM INSPIRE
Large Hadron Collider (LHC)
ion mode
CERN2010–presentCircular rings
(27 km circumference)
208
Pb
82+208
Pb
82+;

Proton-208
Pb
82+

2.76 TeV
per nucleon
ALICE, ATLAS, CMS, LHCb INSPIRE

Electron-proton colliders

AcceleratorLocationYears of
operation
Shape
and size
Electron
energy
Proton
energy
ExperimentsINSPIRE link
HERA DESY 1992–2007Circular ring
(6336 meters around)
27.5 GeV920 GeV H1, ZEUS, HERMES experiment, HERA-B INSPIRE

Light sources

Hypothetical accelerators

Besides the real accelerators listed above, there are hypothetical accelerators often used as hypothetical examples or optimistic projects by particle physicists.

See also

Related Research Articles

<span class="mw-page-title-main">Electron</span> Elementary particle with negative charge

The electron is a subatomic particle with a negative one elementary electric charge. Electrons belong to the first generation of the lepton particle family, and are generally thought to be elementary particles because they have no known components or substructure. The electron's mass is approximately 1/1836 that of the proton. Quantum mechanical properties of the electron include an intrinsic angular momentum (spin) of a half-integer value, expressed in units of the reduced Planck constant, ħ. Being fermions, no two electrons can occupy the same quantum state, per the Pauli exclusion principle. Like all elementary particles, electrons exhibit properties of both particles and waves: They can collide with other particles and can be diffracted like light. The wave properties of electrons are easier to observe with experiments than those of other particles like neutrons and protons because electrons have a lower mass and hence a longer de Broglie wavelength for a given energy.

<span class="mw-page-title-main">Particle physics</span> Study of subatomic particles and forces

Particle physics or high-energy physics is the study of fundamental particles and forces that constitute matter and radiation. The field also studies combinations of elementary particles up to the scale of protons and neutrons, while the study of combination of protons and neutrons is called nuclear physics.

<span class="mw-page-title-main">Cyclotron</span> Type of particle accelerator

A cyclotron is a type of particle accelerator invented by Ernest Lawrence in 1929–1930 at the University of California, Berkeley, and patented in 1932. A cyclotron accelerates charged particles outwards from the center of a flat cylindrical vacuum chamber along a spiral path. The particles are held to a spiral trajectory by a static magnetic field and accelerated by a rapidly varying electric field. Lawrence was awarded the 1939 Nobel Prize in Physics for this invention.

<span class="mw-page-title-main">DESY</span> German national research center

DESY, short for Deutsches Elektronen-Synchrotron, is a national research centre for fundamental science located in Hamburg and Zeuthen near Berlin in Germany. It operates particle accelerators used to investigate the structure, dynamics and function of matter, and conducts a broad spectrum of interdisciplinary scientific research in four main areas: particle and high energy physics; photon science; astroparticle physics; and the development, construction and operation of particle accelerators. Its name refers to its first project, an electron synchrotron. DESY is publicly financed by the Federal Republic of Germany and the Federal States of Hamburg and Brandenburg and is a member of the Helmholtz Association.

<span class="mw-page-title-main">SLAC National Accelerator Laboratory</span> Research center at Stanford University

SLAC National Accelerator Laboratory, originally named the Stanford Linear Accelerator Center, is a federally funded research and development center in Menlo Park, California, United States. Founded in 1962, the laboratory is now sponsored by the United States Department of Energy and administrated by Stanford University. It is the site of the Stanford Linear Accelerator, a 3.2 kilometer (2-mile) linear accelerator constructed in 1966 that could accelerate electrons to energies of 50 GeV.

<span class="mw-page-title-main">Tevatron</span> Defunct American particle accelerator at Fermilab in Illinois (1983–2011)

The Tevatron was a circular particle accelerator in the United States, at the Fermi National Accelerator Laboratory, east of Batavia, Illinois, and was the highest energy particle collider until the Large Hadron Collider (LHC) of the European Organization for Nuclear Research (CERN) was built near Geneva, Switzerland. The Tevatron was a synchrotron that accelerated protons and antiprotons in a 6.28 km (3.90 mi) circumference ring to energies of up to 1 TeV, hence its name. The Tevatron was completed in 1983 at a cost of $120 million and significant upgrade investments were made during its active years of 1983–2011.

<span class="mw-page-title-main">Synchrotron radiation</span> Electromagnetic radiation emitted by charged particles accelerated perpendicular to their velocity

Synchrotron radiation is the electromagnetic radiation emitted when relativistic charged particles are subject to an acceleration perpendicular to their velocity. It is produced artificially in some types of particle accelerators or naturally by fast electrons moving through magnetic fields. The radiation produced in this way has a characteristic polarization, and the frequencies generated can range over a large portion of the electromagnetic spectrum.

<span class="mw-page-title-main">Large Electron–Positron Collider</span> Particle accelerator at CERN, Switzerland

The Large Electron–Positron Collider (LEP) was one of the largest particle accelerators ever constructed. It was built at CERN, a multi-national centre for research in nuclear and particle physics near Geneva, Switzerland.

<span class="mw-page-title-main">Synchrotron</span> Type of cyclic particle accelerator

A synchrotron is a particular type of cyclic particle accelerator, descended from the cyclotron, in which the accelerating particle beam travels around a fixed closed-loop path. The magnetic field which bends the particle beam into its closed path increases with time during the accelerating process, being synchronized to the increasing kinetic energy of the particles. The synchrotron is one of the first accelerator concepts to enable the construction of large-scale facilities, since bending, beam focusing and acceleration can be separated into different components. The most powerful modern particle accelerators use versions of the synchrotron design. The largest synchrotron-type accelerator, also the largest particle accelerator in the world, is the 27-kilometre-circumference (17 mi) Large Hadron Collider (LHC) near Geneva, Switzerland, built in 2008 by the European Organization for Nuclear Research (CERN). It can accelerate beams of protons to an energy of 7 tera electronvolts (TeV or 1012 eV).

<span class="mw-page-title-main">UA2 experiment</span> Particle physics experiment at CERN

The Underground Area 2 (UA2) experiment was a high-energy physics experiment at the Proton-Antiproton Collider — a modification of the Super Proton Synchrotron (SPS) — at CERN. The experiment ran from 1981 until 1990, and its main objective was to discover the W and Z bosons. UA2, together with the UA1 experiment, succeeded in discovering these particles in 1983, leading to the 1984 Nobel Prize in Physics being awarded to Carlo Rubbia and Simon van der Meer. The UA2 experiment also observed the first evidence for jet production in hadron collisions in 1981, and was involved in the searches of the top quark and of supersymmetric particles. Pierre Darriulat was the spokesperson of UA2 from 1981 to 1986, followed by Luigi Di Lella from 1986 to 1990.

<span class="mw-page-title-main">International Linear Collider</span> Proposed linear accelerator for subatomic particles

The International Linear Collider (ILC) is a proposed linear particle accelerator. It is planned to have a collision energy of 500 GeV initially, with the possibility for a later upgrade to 1000 GeV (1 TeV). Although early proposed locations for the ILC were Japan, Europe (CERN) and the USA (Fermilab), the Kitakami highland in the Iwate prefecture of northern Japan has been the focus of ILC design efforts since 2013. The Japanese government is willing to contribute half of the costs, according to the coordinator of study for detectors at the ILC.

<span class="mw-page-title-main">KEK</span> Japanese high-energy physics organization

The High Energy Accelerator Research Organization, known as KEK, is a Japanese organization whose purpose is to operate the largest particle physics laboratory in Japan, situated in Tsukuba, Ibaraki prefecture. It was established in 1997. The term "KEK" is also used to refer to the laboratory itself, which employs approximately 695 employees. KEK's main function is to provide the particle accelerators and other infrastructure needed for high-energy physics, material science, structural biology, radiation science, computing science, nuclear transmutation and so on. Numerous experiments have been constructed at KEK by the internal and international collaborations that have made use of them. Makoto Kobayashi, emeritus professor at KEK, is known globally for his work on CP-violation, and was awarded the 2008 Nobel Prize in Physics.

<span class="mw-page-title-main">Proton Synchrotron</span> CERNs first synchrotron accelerator

The Proton Synchrotron is a particle accelerator at CERN. It is CERN's first synchrotron, beginning its operation in 1959. For a brief period the PS was the world's highest energy particle accelerator. It has since served as a pre-accelerator for the Intersecting Storage Rings (ISR) and the Super Proton Synchrotron (SPS), and is currently part of the Large Hadron Collider (LHC) accelerator complex. In addition to protons, PS has accelerated alpha particles, oxygen and sulfur nuclei, electrons, positrons, and antiprotons.

Radiation damping in accelerator physics is a phenomenum where betatron oscillations and longitudinal oscilations of the particle are damped due to energy loss by synchrotron radiation. It can be used to reduce the beam emittance of a high-velocity charged particle beam.

<span class="mw-page-title-main">Electron scattering</span> Deviation of electrons from their original trajectories

Electron scattering occurs when electrons are displaced from their original trajectory. This is due to the electrostatic forces within matter interaction or, if an external magnetic field is present, the electron may be deflected by the Lorentz force. This scattering typically happens with solids such as metals, semiconductors and insulators; and is a limiting factor in integrated circuits and transistors.

<span class="mw-page-title-main">Cosmotron</span> Particle accelerator

The Cosmotron was a particle accelerator, specifically a proton synchrotron, at Brookhaven National Laboratory. Its construction was approved by the U.S. Atomic Energy Commission in 1948, reaching its full energy in 1953, and continuing to run until 1966. It was dismantled in 1969.

SPEAR was a collider at the SLAC National Accelerator Laboratory. It began running in 1972, colliding electrons and positrons with an energy of 3 GeV. During the 1970s, experiments at the accelerator played a key role in particle physics research, including the discovery of the
J/ψ
meson, many charmonium states, and the discovery of the tau.

<span class="mw-page-title-main">Particle accelerator</span> Research apparatus for particle physics

A particle accelerator is a machine that uses electromagnetic fields to propel charged particles to very high speeds and energies, and to contain them in well-defined beams.

<span class="mw-page-title-main">Tests of relativistic energy and momentum</span>

Tests of relativistic energy and momentum are aimed at measuring the relativistic expressions for energy, momentum, and mass. According to special relativity, the properties of particles moving approximately at the speed of light significantly deviate from the predictions of Newtonian mechanics. For instance, the speed of light cannot be reached by massive particles.

<span class="mw-page-title-main">Laboratori Nazionali di Frascati</span>

The INFN National Laboratory of Frascati (LNF) was founded in 1954 with the objective of furthering particle physics research, and more specifically to host the 1.1 GeV electrosynchrotron, the first accelerator ever built in Italy. The Laboratory later developed the first ever electron-positron collider: from the first prototype AdA, which demonstrated the feasibility, to the ring ADONE and later on to DAΦNE, still operative today (2022). LNF was also the proposed site of the cancelled particle accelerator SuperB.

References

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  2. 1 2 "Cambridge Electron Accelerator (Cambridge, Mass.) Records of the Cambridge Electron Accelerator : an inventory". Harvard University Library. November 15, 2006. Archived from the original on July 9, 2010. Retrieved January 2, 2012.
  3. Rothenberg, Peter J. (October 16, 1958). "An MIT-Harvard Project: The Electron Accelerator". The Harvard Crimson. Retrieved January 2, 2012.
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