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"LEP" redirects here. For other uses, see LEP (disambiguation).
The Large Electron–Positron Collider (LEP) was one of the largest particle accelerators ever constructed. It was built at CERN, a multi-national center for research in nuclear and particle physics near Geneva, Switzerland. LEP was a circular collider with a circumference of 27 kilometers built in a tunnel straddling the border of Switzerland and France. It was used from 1989 until 2000. To date, LEP is the most powerful accelerator of leptons ever built.
HistoryWhen the LEP collider started operation in August 1989 it accelerated the electrons and positrons to a total energy of 45 GeV each to enable production of the Z boson, which has a mass of approximately 91 GeV. The accelerator was upgraded later to enable production of a pair of W bosons, each weighing approximately 80 GeV. LEP collider energy eventually topped at 209 GeV at the end in 2000. At the end of 2000, LEP was shut down and then dismantled in order to make room in the tunnel for the construction of the Large Hadron Collider (LHC). OperationThe Super Proton Synchrotron (an older ring collider) was used to accelerate electrons and positrons to nearly the speed of light. These are then injected into the ring. As in all ring colliders, the LEP's ring consists of many magnets which force the charged particles into a circular trajectory (so that they stay inside the ring), RF accelerators which accelerate the particles with radio frequency (RF) waves, and quadrupoles that focus the particle beam (i.e. keep the particles together). Rather than increasing the particles' velocities (which are already very close to the speed of light), the function of the accelerators is really to increase the particles' energies so that heavy particles can be created when the particles collide. When the particles are accelerated to maximum energy (and focused to so-called bunches), an electron and a positron bunch is made to collide with each other at one of the collision points of the detector. When an electron and a positron collide, they annihilate to a virtual particle, either a photon or a Z boson. The virtual particle almost immediately decays into other elementary particles, which are then detected by huge particle detectors. DetectorsThe Large Electron–Positron Collider had four detectors, built around the four collision points within underground halls. Each was the size of a small house and was capable of registering the particles by their energy, momentum and charge, thus allowing physicists to infer the particle reaction that had happened and the elementary particles involved. By performing statistical analysis of this data, knowledge about elementary particle physics is gained. The four detectors of LEP were called Aleph, Delphi, Opal, and L3. They were built differently to allow for complementary experiments. AlephALEPH stands for Apparatus for LEP PHysics at CERN. The detector determined the mass of the W-boson and Z-boson to within one part in a thousand. The number of families of particles with light neutrinos was determined to be 2.982±.013, which is consistent with the standard model value of 3. The running of the quantum chromodynamics (QCD) coupling constant was measured at various energies and found to run in accordance with perturbative calculations in QCD. DelphiMain article: DELPHI experiment
DELPHI stands for DEtector with Lepton, Photon and Hadron Identification OpalOPAL stands for Omni-Purpose Apparatus for LEP. The detector was dismantled in 2000 to make way for LHC equipment. The name was a pun since some of the founding members of the scientific collaboration which first proposed the design had previously worked on the JADE detector at DESY in Hamburg. L3ResultsThe results of the LEP experiments allowed precise values of many quantities of the Standard Model—most importantly the mass of the Z boson and the W boson (which were discovered in 1983 at an earlier CERN collider) to be obtained—and so confirm the Model and put it on a solid basis of empirical data.
Precision measurements of the shape of the Z boson mass peak constrained the number of light neutrinos in the standard model to exactly three. Near the end of the scheduled run time, data suggested very tentative but inconclusive hints that the Higgs particle might have been observed, a sort of Holy Grail of current high-energy physics. The run-time was extended for a few months, to no avail. See alsoExternal links
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