QCD
Quarkonium
- OZI rule: φ decays
- Discovery of charm: J/Ψ
In November 1974 a strong cross section enhancement in electron-positron annihilation
into hadrons (SPEAR, SLAC) and in the electron-positron invariant mass in the reaction
p Be -> e+e- X (BNL) around 3.1 GeV CMS energy have been observed.
The width of this resonance was smaller than the experimental resolution.
The new particle was named by the two groups J and Ψ, respectively, and in the following
additional narrow resonances have been found. The determined leptonic decay widths have
values typical for vector mesons (J/Ψ: 5.36 keV).
However, the total decay width of the J/Ψ has a value of only 86 keV!
This observation was interpreted as the discovery of a new quark flavour called charm.
In 1977, a second series of narrow resonances, called uspilon's (Υ), with masses
of 9.46 GeV and higer, have been discovered and interpreted as the discovery of a fifth
quark flavour called 'beauty' or also 'bottom'.
INTERPRETATION OF THE RESONANCE
The J/Ψ has been interpreted as a bound charm-anticharm state with JPC=1--)
that is with quark spins being anti-parallel and no relative angular momentum.
The small decay width is explained as follows:
The mass of the J/Ψ is smaller than the sum of the masses of the two lightest
charmed mesons (D+, D0).
As a consequence, the OZI-allowed decays are kinematically forbidden and hence
only OZI-forbidden decays to light hadrons are allowed leading to the small
decay width.
The discovery of the charm quark was not a total surprise:
The gauge theory of weak interactions was demanding for a fourth quark with
a mass of order 1.5 GeV (see 'GIM mechanism').
- OZI rule in QCD
- αs from quarkonia decays