Derives semiclassical propagators for Boltzmann-Gibbs, S± and Tsallis statistics via integrated Quantropy, yielding modified wave functions consistent with q-Schrödinger equation for free particle and corrections for harmonic oscillator.
The reason for this normalization is also understood by an argument presented in the following, motivated by Feynmann and Hibbs procedure [12] and discussed next
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Quantum implications of non-extensive statistics
Derives semiclassical propagators for Boltzmann-Gibbs, S± and Tsallis statistics via integrated Quantropy, yielding modified wave functions consistent with q-Schrödinger equation for free particle and corrections for harmonic oscillator.