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Super Proton Synchrotron

Coordinates:46°14′06″N6°02′33″E / 46.23500°N 6.04250°E /46.23500; 6.04250
From Wikipedia, the free encyclopedia
Particle accelerator at CERN, Switzerland

Particle accelerator
Super Proton Synchrotron
Test beamline delivered from the SPS. In photo 20 GeV positrons are used to calibrate theAlpha Magnetic Spectrometer.
General properties
Accelerator typeSynchrotron
Beam typeprotons, heavy ions
Target typeInjector forLHC, fixed target
Beam properties
Maximum energy450 GeV
Physical properties
Circumference6.9 kilometres (4.3 mi)
Coordinates46°14′06″N6°02′33″E / 46.23500°N 6.04250°E /46.23500; 6.04250
InstitutionCERN
Dates of operation1976–present
Preceded bySppS
CERN Complex
Current particle and nuclear facilities
LHCAcceleratesprotons and heavyions
LEIRAcceleratesions
SPSAccelerates protons and ions
PSBAccelerates protons
PSAccelerates protons or ions
Linac 3Injects heavy ions intoLEIR
Linac4Acceleratesions
ADDeceleratesantiprotons
ELENADecelerates antiprotons
ISOLDEProduces radioactive ion beams
MEDICISProduces isotopes for medical purposes

TheSuper Proton Synchrotron (SPS) is aparticle accelerator of thesynchrotron type atCERN. It is housed in a circular tunnel, 6.9 km (4+13 miles) in circumference,[1] straddling the border of France and Switzerland nearGeneva, Switzerland.[2]

History

[edit]
Aprotonantiproton collision from theUA5 experiment at the SPS in 1982

The SPS was designed by a team led byJohn Adams,director-general of what was then known asLaboratory II. Originally specified as a300 GeV accelerator, the SPS was actually built to be capable of400 GeV, an operating energy it achieved on the official commissioning date of 17 June 1976. However, by that time, this energy had been exceeded byFermilab, which reached an energy of500 GeV on 14 May of that year.[3]

The SPS has been used to accelerateprotons andantiprotons,electrons andpositrons (for use as the injector for theLarge Electron–Positron Collider (LEP)[4]), andheavy ions.

From 1981 to 1991, the SPS operated as a hadron (more precisely, proton–antiproton) collider (as such it was calledSppS), when its beams provided the data for theUA1 andUA2 experiments, which resulted in the discovery of theW and Z bosons. These discoveries and a new technique forcooling particles led to a Nobel Prize forCarlo Rubbia andSimon van der Meer in 1984.

From 2006 to 2012, the SPS was used by theCNGS experiment to produce aneutrinobeam to be detected at theGran Sasso laboratory in Italy, 730 km (450 miles) from CERN.

Later operations

[edit]
See also:List of Super Proton Synchrotron experiments

The SPS is used as the final injector for high-intensity proton beams for theLarge Hadron Collider (LHC), which began preliminary operation on 10 September 2008, for which it accelerates protons from26 to 450 GeV. The LHC itself then accelerates them to severalteraelectronvolts (TeV).

Operation as an injector allows continuation of the ongoingfixed-target research program, where the SPS provides400 GeV proton beams for a number of active fixed-target experiments, includingCOMPASS,NA61/SHINE andNA62.

The SPS has served, and continues to be used as a test bench for new concepts in accelerator physics. In 1999 it served as an observatory for theelectron cloud phenomenon.[5] In 2002 and 2004, SPS producedgold nuclei fromlead targets.[6][7][8] In 2003, SPS was the first machine where theHamiltonian resonance driving terms were directly measured.[9] And in 2004, experiments to cancel the detrimental effects of beam encounters (like those in the LHC) were carried out.[10]

The SPSRF cavities operate at a center frequency of200.2 MHz.

Major discoveries

[edit]

Major scientific discoveries made by experiments that operated at the SPS include the following.

Upgrade for high luminosity LHC

[edit]

TheLarge Hadron Collider will requirean upgrade to considerably increase itsluminosity during the 2020s. This would require upgrades to the entire linac/pre-injector/injector chain, including the SPS.

As part of this, the SPS will need to be able to handle a much higher intensity beam. One improvement considered in the past was increasing the extraction energy to1 TeV.[13] However, the extraction energy will be kept at450 GeV while other systems are upgraded. Theacceleration system will be modified to handle the higher voltages needed to accelerate a higher intensity beam. The beam dumping system will also be upgraded so it can accept a higher intensity beam without sustaining significant damage.[14]

Notes and references

[edit]
  1. ^"SPS Presentation at AB-OP-SPS Home Page". Archived fromthe original on 5 October 2011. Retrieved15 September 2008.
  2. ^Information on CERN SitesArchived 8 July 2012 atarchive.today.CERN. Updated 26 January 2010.
  3. ^CERN courier
  4. ^The LEP Collider – from Design to Approval and CommissioningArchived 18 June 2014 at theWayback Machine, by S. Myers, section 3.8. Last accessed 28 February 2010.
  5. ^"observation of e-cloud"(PDF). Archived fromthe original(PDF) on 29 September 2011. Retrieved20 July 2006.
  6. ^Cecchini, S.; Giacomelli, G.; Giorgini, M.; Mandrioli, G.; Patrizii, L.; Popa, V.; Serra, P.; Sirri, G.; Spurio, M. (2002)."Fragmentation cross sections of 158AGeV Pb ions in various targets measured with CR39 nuclear track detectors".Nuclear Physics A.707 (3–4):513–524.arXiv:hep-ex/0201039.doi:10.1016/S0375-9474(02)00962-4. Retrieved13 May 2025.
  7. ^Scheidenberger, C.; Pshenichnov, I. A.; Sümmerer, K.; Ventura, A.; Bondorf, J. P.; Botvina, A. S.; Mishustin, I. N.; Boutin, D.; Datz, S.; Geissel, H.; Grafström, P.; Knudsen, H.; Krause, H. F.; Lommel, B.; Møller, S. P.; Münzenberg, G.; Schuch, R. H.; Uggerhøj, E.; Uggerhøj, U.; Vane, C. R.; Vilakazi, Z. Z.; Weick, H. (29 July 2004)."Charge-changing interactions of ultrarelativistic Pb nuclei"(PDF).Physical Review C.70 (1).doi:10.1103/PhysRevC.70.014902.ISSN 0556-2813. Retrieved13 May 2025.
  8. ^"ALICE detects the conversion of lead into gold at the LHC".CERN. 8 May 2025. Retrieved13 May 2025.
  9. ^Measurement of resonance driving termsArchived 16 July 2011 at theWayback Machine
  10. ^"wire compensation"(PDF). Archived fromthe original(PDF) on 29 September 2011. Retrieved24 July 2006.
  11. ^"CERN.ch La". Public.web.cern.ch. Retrieved20 November 2010.
  12. ^Fanti, V.; et al. (1999). "A new measurement of direct CP violation in two pion decays of the neutral kaon".Physics Letters B.465 (1–4):335–348.arXiv:hep-ex/9909022.Bibcode:1999PhLB..465..335F.doi:10.1016/S0370-2693(99)01030-8.S2CID 15277360.
  13. ^Super-SPS
  14. ^Hanke, Klaus; Damerau, Heiko; Deleu, Axelle; Funken, Anne; Garoby, Roland; Gilardoni, Simone; Gilbert, Nicolas; Goddard, Brennan; Holzer, Eva Barbara; Lombardi, Alessandra; Manglunki, Django; Meddahi, Malika; Mikulec, Bettina; Shaposhnikova, Elena; Vretenar, Maurizio (2014)."Status of the LIU Project at CERN".Proceedings of the 5th Int. Particle Accelerator Conf. IPAC2014. Petit-Jean-Genaz Christine (Ed.), Arduini Gianluigi (Ed.), Michel Peter (Ed.), Schaa, Volker RW (Ed.): 3 pages, 0.320 MB.doi:10.18429/JACOW-IPAC2014-THPME070.

External links

[edit]
Large Hadron Collider (LHC)
Large Electron–Positron Collider (LEP)
Super Proton Synchrotron (SPS)
Proton Synchrotron (PS)
Linear accelerators
Other accelerators
ISOLDE facility
Non-accelerator experiments
Future projects
Related articles
EMU experiments
NA experiments
UA experiments
WA experiments
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