All statistical information about heat can be obtained with the probability distribution of the heat functional. This paper derives analytically the expression for the distribution of the heat, through path integral, for a diffusive system in a logarithm potential. We apply the found distribution to the first passage problem and find unexpected results for the reversibility of the distribution, giving a fluctuation theorem under specific conditions of the strength parameters.

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In the Stochastic Thermodynamics theory, heat is a random variable with a probability distribution associated. Studies in the distribution of heat are mostly in the overdamped regime. Here we solve the heat distribution in the underdamped regime for three different cases: the free particle, the linear potential, and the harmonic potential. The results are exact and generalize known results in the literature.

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