<p>We derive Planck’s law from a classical variational principle over probability densities, without invoking quantum states, quantized oscillator energies, or a canonical ensemble over discrete oscillator energy levels. We construct a generalized free energy functional involving entropy and Fisher information, with weights determined by the dimensionless ratio <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\( \gamma = \hbar \omega / k_B T \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>γ</mi> <mo>=</mo> <mi>ħ</mi> <mi>ω</mi> <mo stretchy="false">/</mo> <msub> <mi>k</mi> <mi>B</mi> </msub> <mi>T</mi> </mrow> </math></EquationSource> </InlineEquation>. When extremized under a Gaussian ansatz, this functional yields the exact Planck distribution. The only quantum input is a minimal threshold assumption: that an oscillator emits a photon of energy <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\( \hbar \omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ħ</mi> <mi>ω</mi> </mrow> </math></EquationSource> </InlineEquation> only when a thermal fluctuation delivers at least that much energy. We also present a complementary kinetic derivation, based on threshold-activated thermal <i>emission cascades</i>, that yields the same result through classical stochastic reasoning. Together, these approaches suggest that Planck’s law—long considered a hallmark of quantum theory—may instead arise from classical thermodynamic principles supplemented by minimal constraints. This reframing has potential implications for understanding the emergence of quantum behavior from classical statistical systems.</p>

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Planck’s law from a classical free energy extremum involving fisher information

  • Carlos Gomez-Uribe

摘要

We derive Planck’s law from a classical variational principle over probability densities, without invoking quantum states, quantized oscillator energies, or a canonical ensemble over discrete oscillator energy levels. We construct a generalized free energy functional involving entropy and Fisher information, with weights determined by the dimensionless ratio \( \gamma = \hbar \omega / k_B T \) γ = ħ ω / k B T . When extremized under a Gaussian ansatz, this functional yields the exact Planck distribution. The only quantum input is a minimal threshold assumption: that an oscillator emits a photon of energy \( \hbar \omega \) ħ ω only when a thermal fluctuation delivers at least that much energy. We also present a complementary kinetic derivation, based on threshold-activated thermal emission cascades, that yields the same result through classical stochastic reasoning. Together, these approaches suggest that Planck’s law—long considered a hallmark of quantum theory—may instead arise from classical thermodynamic principles supplemented by minimal constraints. This reframing has potential implications for understanding the emergence of quantum behavior from classical statistical systems.