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Subatomic Physics

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310 The Electromagnetic Interaction<br />

Table 10.1: Vector Mesons. ηP is the parity and ηc the charge parity<br />

of the vector mesons.<br />

Rest Dominant<br />

Energy Width Decay<br />

Meson I J ηP ηc Y (MeV) (MeV) Mode<br />

ρ 0 1 1 −1 −1 0 770 153 ππ<br />

ω 0 0 1 −1 −1 0 783 10 π + π − π 0<br />

φ 0 0 1 −1 −1 0 1020 4 KK<br />

peak was identified with the rho meson. Why does the rho turn up here? Before<br />

answering this question, two more experiments will be discussed to provide additional<br />

information. In Fig. 10.16, the cross section for the process e + e − → K + K −<br />

is shown as a function of the total energy 2E0 at energies near 1 GeV. Again a<br />

resonance peak appears but this time with a peak energy of about 1020 MeV and a<br />

width of about 4 MeV. The φ 0 meson has these two properties. Observation of the<br />

reaction e + e − → π + π − π 0 yields a peak at about 780 MeV (see inset of Fig. 10.15)<br />

with a width of about 10 MeV. These values point to the ω 0 . The virtual photon<br />

in the reaction e + e − → hadrons produces resonances at the positions of the ρ 0 ,<br />

the ω 0 ,andtheφ 0 . To see what these three mesons have in common, we list their<br />

properties in Table 10.1.<br />

The three mesons in Table<br />

10.1 satisfy the conditions<br />

set out above: They have<br />

spin J = 1, negative parity,<br />

negative charge parity, and<br />

strangeness 0. Since a vector<br />

has negative parity and<br />

the same number of independent<br />

components as a spin-1<br />

particle, the mesons are called<br />

vector mesons. The rho has<br />

isospin1andisanisovector,<br />

whereas the two others are<br />

isoscalars.<br />

Figure 10.17: The transformation of a virtual photon into<br />

a vector meson gives rise to the resonances and their decays<br />

observed in colliding beam experiments.<br />

As pointed out in Section 8.6, after Eq. (8.30), the electric charge operator is<br />

composed of an isoscalar and the third component of an isovector. The photon, as<br />

carrier of the electromagnetic force, should have the same transformation properties,<br />

and it matches the vector mesons in their isospin properties. The diagrams for the<br />

production of the three vector mesons listed in Table 10.1 are given in Fig. 10.17.

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