Abstract
Two-particle scattering in Ising field theory in a weak magnetic field h is studied in the regime T>Tc, using perturbation theory in h2. We calculate explicitly the cross-section of the process 2→3 to the order h2. To this order, σ2→3 dominates σtot (the probability of all inelastic processes) at all energies E. We show that at high energy the h2-term in σtot grows as 16G3h2logE, where G3 is exactly the third moment of the Euclidean spin-spin correlation function. Going beyond the leading order, we argue that at small h2 the probability of the 2→2 process decays as E-16G3h2 as E→infin;.
| Original language | English |
|---|---|
| Pages (from-to) | 654-674 |
| Number of pages | 21 |
| Journal | Nuclear Physics, Section B |
| Volume | 849 |
| Issue number | 3 |
| DOIs | |
| State | Published - Aug 21 2011 |
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