7 S ep 2 00 6 Ludwig Edward Boltzmann

ar X iv : h ep - p h / 06 09 07 7 v 1 7 S ep 2 00 6 Hadron multiplicities in e + e − annihilation with heavy primary quarks

ar X iv : h ep - p h / 06 05 10 7 v 2 24 O ct 2 00 6 Monopole confinement by flux tube

M ar 2 00 6 Ludwig Boltzmann , Transport Equation and the Second Law

Ludwig Boltzmann had a hunch that irreversibility exhibited by a macroscopic system arises from the reversible dynamics of its microscopic constituents. He derived a nonlinear integro-differential equation now called the Boltzmann equation for the phase space density of the molecules of a dilute fluid. He showed that the Second Law of thermodynamics emerges from Newton’s equations of motion. Ho...

2 00 6 Ludwig Boltzmann , Transport Equation and the Second law

Ludwig Boltzmann had a hunch that irreversibility exhibited by a macroscopic system arises from the reversible dynamics of its microscopic constituents. He derived a nonlinear integro-differential equation now called the Boltzmann equation for the phase space density of the molecules of a dilute fluid. He showed that the Second law of thermodynamics emerges from Newton’s equations of motion. Ho...

ar X iv : h ep - t h / 03 09 06 8 v 1 6 S ep 2 00 3 Integrable Lattice Models for Conjugate A ( 1 ) n Roger

A new class of A (1) n integrable lattice models is presented. These are interaction-round-a-face models based on fundamental nimrep graphs associated with the A (1) n conjugate modular invariants, there being a model for each value of the rank and level. The Boltzmann weights are parameterized by elliptic theta functions and satisfy the Yang-Baxter equation for any fixed value of the elliptic ...