Resonances
When a system of two interacting particles have the same quantum numbers (invariant mass, spin, charge, ) as a particle, they can form that particle as a resonance. The maximum total coupling strength for a given particle is the unitarity limit, so if the resonant particle can couple to more than one final state, then the branching ratios and cross sections for a particular final state are proportional to the coupling strength.
Breit Wigner Resonance Scattering Cross Section
(The Breit-Wigner energy distribution is simply the Fourier transform of an exponential decay time distribution.)
p+p total cross section: D++(1236)
Mass: M = 1232 MeV Full Width: G=120 MeV
Spin: 3/2
Branching Ratio : BR(D++Æ p+p)=99.5%
p+p Æp+p cross section at peak of resonance:
e+ e- -->r0,w0 -->p+ p- (F&H Figure 10.20)
r0 | w0 | h0 | |
Mass: | 769 MeV | 782 MeV | 547 MeV |
Full Width: | G=151 MeV | 8.4 MeV | 0.0012 MeV |
SpinParity: | 1- | 1- | 0- |
Branching Ratios : | |||
BR(p+ p-) | ~100% | 2.2% | - |
BR(e + e-) | 4.5x10-5 | 7.2x10-5 | 10-10 (theory) |
|Fp|2at peak (if no interference) | 38 | 1.3 | - |
The non-resonant QED (Quantum Electrodynamic) cross section for the production of pions is
where p/3s is the cross section for massless point pions, b3 is the threshold dependence for massive pions (139.6 MeV/c2), and Fp2 is the form factor for real composite pions.
The h meson is not observed because it is a pseudoscalar meson and it cannot mix with a single virtual photon to mediate a decay into an electron-positron pair.
e+ e- -->f -->K+ K- (F&H Figure 10.21)
Mass: M(f) = 1019.4 MeV M(K±)=493.7 MeV
Full Width: G=4.41 MeV
Spin: 1-
Branching Ratio : BR(f--> e +e-)=3.1x10-4,
BR(f--> K +K-)=50%
Cross section:
speak=2.2mb (xphase
space)
e+ e- --> J/y Æhadrons (F&H Figure 10.23)
Mass: M(J/y) = 3097 MeV
Full Width: G=0.07 MeV
Spin: 1-
Branching Ratio : BR(J/y --> e +e-)=6.9%,
BR(J/y --> hadrons)=86%
Cross section: speak=90mb
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