Encyclopedia Cosmology Cosmology Radiation Entropy Relation Bose Entropy Integral Value

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Cosmology Radiation Entropy Relation Bose Entropy Integral Value

A single integral over the Bose-Einstein distribution yields the exact entropy of radiation, and its value is 4π⁴/45.

The radiation entropy integral

For a gas of massless particles, the entropy density s is not an independent quantity. Statistical mechanics ties it to the energy density ρ and the temperature T through the relation s = (4/3)·ρ/T. The factor 4/3 has long been a standard input in textbooks. The declaration bose_entropy_integral_value proves that this factor is not an assumption: it emerges from the microscopic entropy functional of quantum statistics.

The proof works with dimensionless integrals where x = E/T. For a gas of bosons, the entropy integrand is σ_B(x) = x²[(1+f)ln(1+f) − f ln f], with f = 1/(eˣ−1) the Bose-Einstein occupation number. The theorem shows that the integral of σ_B from 0 to ∞ equals 4π⁴/45. This value is exactly 4/3 times the energy integral ∫₀^∞ x³/(eˣ−1) dx = π⁴/15. A companion theorem proves the analogous result for fermions, with the entropy integral equal to 7π⁴/90 and the same 4/3 factor relative to its energy integral.

The method splits each entropy integrand into the energy kernel plus a logarithmic kernel. The logarithmic kernel expands into a Mercator series in e^(−x), and its Mellin transform at s = 3 evaluates to Γ(3)·ζ(4) = π⁴/45 for bosons and Γ(3)·η(4) = 7π⁴/360 for fermions. Adding the energy integrals gives the totals. The theorem also yields the entropy coefficient: the integral divided by 2π² equals 2π²/45, the prefactor in the standard formula s_γ = (2π²/45)·g·T³.

What the theorem does not claim: the phase-space normalization g/(2π²), the units ℏ=c=k_B=1, and the identification of the physical entropy density with the ideal-gas entropy functional are definitional bridges, not proved results. The theorem proves the functional and numerical content of s = (4/3)ρ/T and the 7/8 fermion-to-boson entropy weight, but it does not derive the degeneracy count g or the physical interpretation of the entropy functional itself.

THEOREM bose_entropy_integral_value · IndisputableMonolith/Cosmology/RadiationEntropyRelation.lean
/-- **THEOREM (Bose entropy integral).**
`∫₀^∞ t²[(1+f)ln(1+f) − f ln f] dt = 4π⁴/45` with `f = 1/(eᵗ−1)`. -/
theorem bose_entropy_integral_value :
    (∫ t in Ioi (0 : ℝ), boseEntropyIntegrand t) = 4 * π ^ 4 / 45 := by
  have hsplit : (∫ t in Ioi (0 : ℝ), boseEntropyIntegrand t)
      = ∫ t in Ioi (0 : ℝ),
          (t ^ 3 / (Real.exp t - 1) + t ^ 2 * (-Real.log (1 - Real.exp (-t)))) := by
    refine setIntegral_congr_fun measurableSet_Ioi fun t ht => ?_
    exact bose_entropy_pointwise ht
  rw [hsplit, integral_add integrableOn_bose_energy integrableOn_boseLog,
    FermionWeightIntegral.bose_integral_value, boseLog_integral_value]
  ring
THEOREM bose_entropy_eq_four_thirds_energy · IndisputableMonolith/Cosmology/RadiationEntropyRelation.lean
bose_entropy_eq_four_thirds_energy · IndisputableMonolith/Cosmology/RadiationEntropyRelation.lean:412
/-- **THEOREM (s = (4/3)ρ/T, Bose).** The Bose entropy integral is exactly
`4/3` of the Bose energy integral.  This is the dimensionless content of the
thermodynamic relation `s = (4/3)·ρ/T` for a massless boson gas, derived from
the microscopic entropy functional (never assumed). -/
theorem bose_entropy_eq_four_thirds_energy :
    (∫ t in Ioi (0 : ℝ), boseEntropyIntegrand t)
      = 4 / 3 * ∫ t in Ioi (0 : ℝ), t ^ 3 / (Real.exp t - 1) := by
  rw [bose_entropy_integral_value, FermionWeightIntegral.bose_integral_value]
  ring
THEOREM entropy_coeff_from_functional · IndisputableMonolith/Cosmology/RadiationEntropyRelation.lean
/-- **THEOREM (the 2π²/45 entropy coefficient from the functional).**
`s_γ = (g/2π²)·T³·∫σ_B = (2π²/45)·g·T³`: dividing the derived entropy
integral by the phase-space normalization `2π²` yields exactly the `2π²/45`
prefactor of the photon entropy density, with the `4/3` factor never
assumed. -/
theorem entropy_coeff_from_functional :
    (∫ t in Ioi (0 : ℝ), boseEntropyIntegrand t) / (2 * π ^ 2) = 2 * π ^ 2 / 45 := by
  rw [bose_entropy_integral_value]
  rw [div_eq_iff (by positivity)]
  ring
THEOREM fermi_div_bose_entropy · IndisputableMonolith/Cosmology/RadiationEntropyRelation.lean
/-- **THEOREM (7/8 at the entropy layer).** The Fermi entropy integral is
exactly `7/8` of the Bose one: the fermionic statistics weight of
`EntropyPerPhoton.fermionWeight` holds directly for entropy, not only for
energy. -/
theorem fermi_div_bose_entropy :
    (∫ t in Ioi (0 : ℝ), fermiEntropyIntegrand t)
      / (∫ t in Ioi (0 : ℝ), boseEntropyIntegrand t) = 7 / 8 := by
  rw [bose_entropy_integral_value, fermi_entropy_integral_value]
  rw [div_eq_iff (by positivity)]
  ring

What this page does not claim

The theorem does not derive the phase-space normalization factor g/(2π²) or the choice of units ℏ=c=k_B=1. The theorem does not prove that the physical entropy density is given by the ideal-gas entropy functional. The theorem does not establish the value of the fine-structure constant or any other coupling constant.

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