IndisputableMonolith.Cosmology.StatisticsKernels
Defines the elementary statistical kernels used in RS cosmology: Gibbs weights, Bose and Fermi partition functions, and occupation numbers at chemical potential zero. Cosmologists citing the reduced pressure and energy integrals need these closed forms. The module is mostly definitional, with short positivity and algebraic identities proved from Real.exp facts.
claimFor dimensionless energy $t = E/T$ and occupation number $n \in \mathbb{N}$, the Gibbs weight is $w_n(t) = e^{-n t}$. The Bose and Fermi single-mode partitions are $Z_B(t) = \sum_{n=0}^{\infty} e^{-n t} = (1-e^{-t})^{-1}$ and $Z_F(t) = 1+e^{-t}$, with occupations $n_B = (e^{t}-1)^{-1}$ and $n_F = (e^{t}+1)^{-1}$.
background
Recognition Science cosmology reduces the relativistic ideal-gas pressure and energy in $D=3$ to one-dimensional integrals of the form $(g/2\pi^2) T^4 \int t^2 K(t),dt$. The kernel $K$ is built from Bose or Fermi statistics at vanishing chemical potential.
This module supplies those kernels in dimensionless variables. The Gibbs weight of an $n$-quanta microstate at $t=E/T$ is $e^{-n t}$. Summing geometric series yields the Bose partition $(1-e^{-t})^{-1}$ and the two-level Fermi partition $1+e^{-t}$. Occupation numbers are the usual logarithmic derivatives.
Upstream, PhaseSpaceReduction records that the prefactor $g/(2\pi^2)$ is forced by three spatial dimensions; the present kernels are the statistical content that multiplies that geometric factor.
proof idea
Definition module with lightweight supporting lemmas. Boltzmann weights, partitions, and occupations are introduced as plain defs in terms of Real.exp. Identities such as $w_n = (e^{-t})^n$, $Z_B = (1-e^{-t})^{-1}$, and $Z_F = 1+e^{-t}$ are one-line algebraic rewrites. Positivity of the partitions follows from $e^{-t}<1$ (for $t>0$) and $e^{t}>1$. No deep analysis; Mathlib exponential inequalities close the goals.
why it matters in Recognition Science
Feeds the integrand kernels inside the RS plasma pressure and energy functionals that PhaseSpaceReduction writes as $P=(g/2\pi^2)T^4\int t^2 K(t),dt$. Without explicit Bose/Fermi partitions and occupations, those integrals remain formal. The module sits in the cosmology layer that converts the forced $D=3$ phase-space measure into thermodynamic observables, consistent with the eight-tick and dimension-forcing chain (T7–T8) that fixes the geometric prefactor. No downstream theorems are wired yet in the graph; the natural consumers are the grand-potential pressure and energy theorems.
scope and limits
- Does not derive the $g/(2\pi^2)T^4$ prefactor; that lives in PhaseSpaceReduction.
- Does not treat nonzero chemical potential or interacting gases.
- Does not evaluate the momentum integrals; only supplies the statistical kernels $K(t)$.
- Does not claim RS-specific corrections beyond standard Bose/Fermi forms at $\mu=0$.
depends on (1)
declarations in this module (31)
-
def
boltzmannWeight -
def
bosePartition -
def
fermiPartition -
def
boseOccupation -
def
fermiOccupation -
lemma
boltzmannWeight_pow -
lemma
exp_neg_lt_one -
lemma
one_lt_exp -
theorem
bosePartition_eq -
theorem
fermiPartition_eq -
lemma
bosePartition_pos -
lemma
fermiPartition_pos -
theorem
boseLogKernel_eq_log_partition -
theorem
fermiLogKernel_eq_log_partition -
theorem
boseOccupation_eq -
theorem
fermiOccupation_eq -
theorem
fermiOccupation_lt_one -
theorem
boseOccupation_pos -
theorem
boseEnergyKernel_eq_occupation -
theorem
fermiEnergyKernel_eq_occupation -
theorem
boseLogKernel_hasDerivAt -
theorem
fermiLogKernel_hasDerivAt -
theorem
boseEnergyKernel_from_logKernel -
theorem
fermiEnergyKernel_from_logKernel -
theorem
mode_energy_bose -
theorem
mode_energy_fermi -
lemma
phaseSpaceDensity_congr_pos -
theorem
plasmaPressure_from_partitionFunction -
theorem
plasmaEnergy_from_occupation -
theorem
number_integrand_bose -
theorem
number_integrand_fermi