
We propose a quantity, ${\mathcal{A}\!\!\!/}$, as a measure describing the nonadiabaticity of a thermodynamic process. For this purpose, we use a schematic method to find the measure of the `degree of nonadiabaticity'. The method utilizes an `invariant' thermal state constructed from the Ermakov-Lewis-Riesenfeld invariant. Specifically, we study a frequency-modulated quantum harmonic oscillator as a thermodynamic system. Naturally, we write the first law of thermodynamics with ${\mathcal{A}\!\!\!/}$ as a measurable quantity. We discuss universality for the method and some possible applications.
12 pages, 3 figures
High Energy Physics - Theory, Quantum Physics, Classical and relativistic thermodynamics, non-adiabaticity, thermodynamic first law, temperature, FOS: Physical sciences, General Relativity and Quantum Cosmology (gr-qc), General Relativity and Quantum Cosmology, High Energy Physics - Theory (hep-th), squeezed oscillators, Ermakov-Lewis-Riesenfeld invariant, Coherent states, Quantum Physics (quant-ph), Probabilistic methods for one variable harmonic analysis
High Energy Physics - Theory, Quantum Physics, Classical and relativistic thermodynamics, non-adiabaticity, thermodynamic first law, temperature, FOS: Physical sciences, General Relativity and Quantum Cosmology (gr-qc), General Relativity and Quantum Cosmology, High Energy Physics - Theory (hep-th), squeezed oscillators, Ermakov-Lewis-Riesenfeld invariant, Coherent states, Quantum Physics (quant-ph), Probabilistic methods for one variable harmonic analysis
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