k Computer reconstruction of Zzero decay Computer reconstruction of the decay of a Znaught particle, observed with the Mark II Vertex Detector of the Stanford Linear Collider SLC. The Z naught is one of the gauge bosons, and is the carrier of the electroweak nuclear force. It is created by an electronpositron anihilation at energies of 93 GeV giga electron volts. The Z naught has decayed into hadrons red tracks, which themselves have decayed into secondary hadrons yellow tracks and a muon green track. The blue tracks show lowenergy background events. The Znaught was discovered at the European LEP accelerator in 1983. Stock Photo - Afloimages
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Computer reconstruction of Z zero decay Computer reconstruction of the decay of a Z naught particle, observed with the Mark II Vertex Detector of the Stanford Linear Collider  SLC . The Z  naught is one of the gauge bosons, and is the  carrier  of the electroweak nuclear force. It is created by an electron positron anihilation at energies of 93 GeV  giga electron volts . The Z  naught has decayed into hadrons  red tracks , which themselves have decayed into secondary hadrons  yellow tracks  and a muon  green track . The blue tracks show low energy background events. The Z naught was discovered at the European LEP accelerator in 1983.
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Computer reconstruction of Z-zero decay

Computer reconstruction of the decay of a Z-naught particle, observed with the Mark II Vertex Detector of the Stanford Linear Collider (SLC). The Z- naught is one of the gauge bosons, and is the 'carrier' of the electroweak nuclear force. It is created by an electron/positron anihilation at energies of 93 GeV (giga electron volts). The Z- naught has decayed into hadrons (red tracks), which themselves have decayed into secondary hadrons (yellow tracks) and a muon (green track). The blue tracks show low-energy background events. The Z-naught was discovered at the European LEP accelerator in 1983.

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