J/psi particle

An elementary particle with an unusually long lifetime or, from the Heisenberg uncertainty principle, with an extremely narrow width &Ggr; = 91.0 ± 3.2 keV, and a large mass m = 3096.916 ± 0.011 MeV. It is a bound state containing a charm quark and an anticharm quark. The discovery of the J/psi particle is one of the cornerstones of the standard model.

Since its discovery in 1974, more than 10⁹ J/psi particles have been produced. More than 100 different decay modes and new particles radiating from the J/psi particle have been observed. The J/psi particle has been shown to be a bound state of charm quarks. The long lifetime of the J/psi results from its mass being less than the masses of particles which separately contain a charm and an anticharm quark. This situation permits the J/psi to decay only into noncharm quarks, and empirically this restriction was found to lead to a suppression of the decay rate resulting in a long lifetime and narrow width. The subsequent discovery of the b quark and the intermediate vector bosons Z⁰ and W^±, and studies of Z⁰ decays into charm, b, and other quarks, show that the theory of the standard model is in complete agreement with experimental data to an accuracy of better than 1%. See Charm, Elementary particle, Intermediate vector boson, Quarks, Standard model, Upsilon particles

单词	j/psi particle
释义	J/psi particle J/psi particle n (Nuclear Physics) a type of elementary particle (meson) thought to be formed from charmed quarks. See charm¹⁷ J/psi particle J/psi particle An elementary particle with an unusually long lifetime or, from the Heisenberg uncertainty principle, with an extremely narrow width &Ggr; = 91.0 ± 3.2 keV, and a large mass m = 3096.916 ± 0.011 MeV. It is a bound state containing a charm quark and an anticharm quark. The discovery of the J/psi particle is one of the cornerstones of the standard model. Since its discovery in 1974, more than 10⁹ J/psi particles have been produced. More than 100 different decay modes and new particles radiating from the J/psi particle have been observed. The J/psi particle has been shown to be a bound state of charm quarks. The long lifetime of the J/psi results from its mass being less than the masses of particles which separately contain a charm and an anticharm quark. This situation permits the J/psi to decay only into noncharm quarks, and empirically this restriction was found to lead to a suppression of the decay rate resulting in a long lifetime and narrow width. The subsequent discovery of the b quark and the intermediate vector bosons Z⁰ and W^±, and studies of Z⁰ decays into charm, b, and other quarks, show that the theory of the standard model is in complete agreement with experimental data to an accuracy of better than 1%. See Charm, Elementary particle, Intermediate vector boson, Quarks, Standard model, Upsilon particles
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