Around 1968
Sheldon Glashow,
Steven Weinberg, and
Abdus Salam came up with the
electroweak theory, which unified the
electromagnetic and
weak interactions, and for which they shared the 1979
Nobel Prize in Physics. The theory postulated the existence of
W and Z bosons. It was experimentally established in two stages, the first being the discovery of
neutral currents in
neutrino scattering by the
Gargamelle collaboration at
CERN, a process that required the existence of a neutral particle to carry the weak force—the Z boson. The results from the Gargamelle collaboration made calculations of the masses of the W and Z bosons possible. It was predicted that the W boson had a mass value in the range of 60 to , and the Z boson in the range from 75 to —energies too large to be accessible by any
accelerator in operation at that time. The second stage of establishing the electroweak theory would be the discovery of the W and Z bosons, requiring the design and construction of a more powerful accelerator. During the late 70s, CERN's prime project was the construction of the
Large Electron–Positron Collider (LEP). Such a machine was ideal to produce and measure the properties of W and Z bosons. However, due to the pressure to find the W and Z bosons, the CERN community felt like it could not wait for the construction of LEP—a new accelerator was needed, whose construction could not be at the expense of LEP.{{cite web |last=Darriulat |first=Pierre |date=1 April 2004 |title=The W and Z particles: a personal recollection |url=http://cerncourier.com/cws/article/cern/29053 W and Z bosons are produced mainly as a result of quark-antiquark annihilation. In the
parton model, the momentum of a proton is shared between the proton's constituencies: a portion of the proton
momentum is carried by the
quarks, and the remainder by
gluons. It would not be sufficient to accelerate protons to a momentum equal to the mass of the boson, as each quark would only carry a portion of the momentum. To produce bosons in the estimated intervals of 60 to (W boson) and 75 to (Z boson), one would therefore need a proton-antiproton collider with a center-of-mass energy of approximately six times the boson masses, about 500–. The design of the SpS was determined by the need to detect the decay . As the
cross-section for Z production at is , and the fraction of decay is ~3%, a
luminosity of L = would give an event rate of ~1 per day. To achieve such luminosity, one would need an antiproton source capable of producing antiprotons each day, distributed in a few bunches with angular and momentum acceptance of the SPS. ==History==