The Self-Referential Scalar Family: e, the Half-Turn, and the Unification of Information Theory, Statistics, Thermodynamics, and QND Measurement in the Adelic Picture

Author: Rowan Brad Quni-Gudzinas | Date: 2026-08-20 | License: CC-BY-4.0

Abstract

Standard information theory measures uncertainty at the archimedean place; the adelic

program extends it to all completions of the rationals, carrying a p-adic valuation

entropy alongside Shannon entropy. This paper shows that the two most familiar

distributions of statistical mechanics are already hidden inside that p-adic structure.

The p-adic maximum-entropy distribution — the geometric distribution on the valuation —

is exactly the Bose–Einstein occupation distribution at fugacity $1/p$, that is, at

inverse temperature $\ln p$ at the p-adic place; its mean, $1/(p-1)$, is the p-adic

entropy itself. The squarefree restriction of the integers, which excludes repeated

prime factors just as the Pauli exclusion forbids double occupation, is its Fermi–Dirac

counterpart, with occupation probability $1/(p+1)$ at the same temperature. A quantum

non-demolition measurement of a p-adic-valued observable preserves this entropy exactly:

it is the equality case of the adelic data-processing inequality, the measurement that

reads without demolition. These identifications are exact and computationally verified.

They are assembled under a single structural thesis: the constants $e$, $\pi$, and the

exchange phase $R = (e^{i\pi})^{2s}$ form one self-referential scalar family generated by

the act of drawing a distinction — $e$ as the fixed point of the operator $Df = f$, the

Gaussian as the fixed point of the Fourier transform, the Boltzmann factor as the fixed

point of the maximum-entropy principle, and the half-turn $e^{i\pi} = -1$ as the

generator of quantum statistics. The Planckian bound $2\pi k_B T/\hbar$ and the

architectural optimum $\ln(2\pi)$ carry the same circle-trace $\pi$. The premises end

where the identification of a physical temperature at the p-adic place begins: the

algebra is exact, the dictionary is proposed, and the falsification conditions are

written.

1. Introduction

A compound question motivates this work: what is the relationship between information

theory, statistics, thermodynamics, and quantum non-demolition (QND) measurement —

especially as it bears on the self-reference of the constant $e$ and on patterns of

distinction such as re-entry — and how do recent results on spin statistics and on

standard-model/condensed-matter unification tie in?

The answer developed here is a single structural claim: **the scalar family generated by

the re-entrant mark — $e$ as the fixed point of $Df = f$, $\pi$ as the trace of the

identity on the circle type, and the exchange phase $R = (e^{i\pi})^{2s}$ as the

$(2s)$-fold half-turn — is the common skeleton of all four domains.** Information theory,

statistics (in both senses: probability distributions and quantum statistics),

thermodynamics, and QND measurement each turn out to be a face of the same

self-referential fixed-point structure.

Three results are established, all computationally verified:

• R1 (statistics = information, non-archimedean). The p-adic maximum-entropy

distribution of Adelic Shannon Theory [1], $P(v_p(X) = k) = (1 - 1/p)\,p^{-k}$, is

exactly the Bose–Einstein occupation distribution with fugacity $z = e^{-\beta_p} =

1/p$, i.e. at inverse temperature $\beta_p = \ln p$ at the p-adic place. Its mean is

the Bose–Einstein occupation number $\langle n \rangle = 1/(e^{\beta(\varepsilon-\mu)}

• 1) = 1/(p-1)$, precisely the p-adic entropy $H_p^{\max}$.
• R2 (statistics = information, fermionic). The squarefree restriction of the

integers ($vp \in \{0,1\}$ — the p-adic Pauli exclusion) yields $P(vp = 1) =

1/(p+1)$, exactly the Fermi–Dirac occupation number at the same inverse temperature

$\beta_p = \ln p$. Verified numerically over 1.2 million squarefree integers (max

deviation $8.53\times10^{-6}$).

• R3 (QND = equality case of the data-processing inequality). An ideal QND

measurement of a p-adic-valued observable preserves $H_p$ exactly: it is the equality

case of the adelic data-processing inequality — the measurement family (any channel

commuting with the observable, reading its eigenbasis) that extracts information

without increasing the measured observable's entropy.

Why a reader should care. The p-adic valuation entropy is not an exotic side

structure: it is literally the occupation statistics of statistical mechanics, with the

prime setting the temperature. That identification gives quantum engineers a per-prime

uncertainty budget conserved by QND readout, gives energy benchmarking a per-prime cost

scale, and gives foundations a concrete unification: $e$, $\pi$, and the exchange phase

organize information theory, statistics, thermodynamics, and measurement as one

structure. The claims are graded, verified computationally, and falsifiable.

Where the premises end. The results rest on imported machinery — the Adelic Shannon

formalism $Hp = \mathbb{E}[vp]$ [1], the exchange-phase reading $R = (e^{i\pi})^{2s}$

[2, 3], the Planckian bound [15] — and on two conjectural steps of this paper: that

$\beta_p = \ln p$ is a physical temperature (exact algebra, proposed physics) and that

the four domains are one family (the unification thesis). Both are stated with

falsification conditions in Section 7.

2. The Three Faces of e

The constant $e$ appears in this program three times, and each appearance is a fixed

point of a self-referential operation:

1. $e$ as the fixed point of differentiation (re-entrant calculus [3, 7]): the

re-entrant mark under linear discipline solves $Df = f$, $f(0) = 1$, with unique

solution $f(x) = e^x$. The function equal to its own rate of change — self-reference

in its purest local form.

1. $e^{-\pi x^2}$ as the fixed point of the Fourier transform (Adelic Shannon

Theory [1]): the Gaussian is the unique function (up to scaling) with

$\mathcal{F}[g] = g$, an eigenfunction of the Fourier transform with eigenvalue 1.

This is self-reference in its purest global (duality) form. The Poisson summation

formula $\sumn f(n) = \sumn \hat{f}(n)$ holds because the Gaussian is this fixed

point — source-channel equality at every place simultaneously.

1. $e^{-\beta E}$ as the fixed point of the maximum-entropy variational principle

(thermodynamics): the Boltzmann factor is the unique distribution maximizing entropy

subject to fixed mean energy — the distribution equal to its own max-entropy

solution. The Gaussian is the continuous case; the Boltzmann factor is the general

case; both are fixed points of the entropy functional under moment constraints.

The re-entrant calculus [3, 7] already identified faces 1 and the half-turn

$e^{i\pi} = -1$; Adelic Shannon Theory [1] identified face 2; thermodynamics has always

known face 3. The unification claim of this paper is that these are **the same

self-reference at different levels of the adelic hierarchy**: local ($D$), global

($\mathcal{F}$), and variational (max-entropy). The half-turn $e^{i\pi} = -1$ is the

bridge: it is the rotation fixed point (a $2\pi$ rotation of the circle is the

identity — the circle's self-reference), and it generates the exchange phase

$R = (e^{i\pi})^{2s}$. The Gaussian's differential entropy

$h = \tfrac12\ln(2\pi e \sigma^2)$ carries both constants at once (verified: $\sigma=1

\to 1.4189\ldots$, $\sigma=\tfrac12 \to 0.7258\ldots$, $\sigma=2 \to 2.1121\ldots$), and

the Jacobi theta constant $\vartheta_3(0;i) = 1.0864\ldots$ is the finite "total adelic

information" of the Gaussian — the sum over the lattice of the fixed point (verified to

12 digits; the Jacobi identity $\theta(t) = t^{-1/2}\theta(1/t)$ holds to $10^{-14}$ at

$t \in \{0.5, 1, 2, 3, 5\}$).

3. Statistics: The Missing Link

The word "statistics" is used in physics in two senses, and the adelic picture reveals

they are the same thing at different places:

• Quantum statistics (spin-statistics): the exchange phase $R = e^{2\pi i s}$ of

identical particles; bosons ($s$ integer, $R = +1$) and fermions ($s$ half-integer,

$R = -1$) as the parity of $2s$ [2, 3, 13, 14, 17].

• Probability statistics (distribution theory): the occupation-number distributions

of statistical mechanics — Bose–Einstein and Fermi–Dirac.

The link: **both are fixed points of maximum-entropy principles, distinguished by the

exchange phase.** The Bose–Einstein distribution is the max-entropy distribution of

occupation numbers with fixed mean energy; the Fermi–Dirac distribution is the same with

the Pauli restriction $n \in \{0,1\}$. What the exchange phase $R = e^{2\pi i s}$ does

is select which exponential modality applies — the symmetric algebra (bosonic) or the

exterior algebra (fermionic) — exactly the two modal exponentials whose braiding was

formalized in the spin-statistics program [2, T1].

3.1 New result R1: p-adic maximum-entropy ≡ Bose–Einstein

Adelic Shannon Theory [1] defines p-adic entropy

$Hp(X) = \sumx p(x)\, vp(x) = \mathbb{E}[vp(X)]$ and identifies the maximum-entropy

distribution as the geometric distribution on the valuation:

with $H_p^{\max} = 1/(p-1)$.

Now write the geometric distribution as a Bose–Einstein occupation distribution. The BE

occupation-number distribution with fugacity $z = e^{-\beta(\varepsilon-\mu)}$ is

Setting $z = 1/p$ gives $P(k) = (1 - 1/p)\,p^{-k}$ — identical. The mean occupation is

$\langle n \rangle = \frac{1/p}{1 - 1/p} = 1/(p-1)$ — identical to $H_p^{\max}$. **The

p-adic maximum-entropy distribution is the Bose–Einstein distribution at fugacity

$z = 1/p$, i.e. at inverse temperature $\beta_p = \ln p$.** The p-adic entropy is the

mean occupation number of a bosonic mode at a temperature set by the prime itself.

[ESTABLISHED — exact algebraic identity; verified numerically for $p = 2, 3, 5, 7$;

means match $1/(p-1)$ to $10^{-12}$.]

3.2 New result R2: squarefree restriction ≡ Fermi–Dirac

The fermionic counterpart of the valuation structure is the squarefree restriction:

an integer is squarefree iff $v_p(x) \in \{0,1\}$ for every prime $p$ — each prime

divides at most once. This is the p-adic analogue of the Pauli exclusion (occupation

number per mode at most 1). Among squarefree integers, the probability that $p$ divides

$x$ is

(a standard density fact: the squarefree density is $6/\pi^2$, and the p-divisibility

condition removes the $p^2$ factor; the exact identity $(p-1)/(p^2-1) = 1/(p+1)$ is

elementary). The Fermi–Dirac occupation number at fugacity $z = 1/p$ is

Identical. The squarefree integers realize Fermi–Dirac statistics at the p-adic

place, with the same inverse temperature $\beta_p = \ln p$. [ESTABLISHED — verified

numerically over $N = 2{,}000{,}000$, 1,215,877 squarefree integers; the frequency of

$p \mid n$ matches $1/(p+1)$ for $p = 2,3,5,7$ with max deviation $8.53\times10^{-6}$.]

3.3 The dictionary

The p-adic "energy" is the valuation $k$; the p-adic "temperature" is the reciprocal

prime logarithm; the p-adic "chemical potential" is implicitly absorbed into the

fugacity normalization. The statistics dichotomy (boson/fermion) is mirrored exactly:

unrestricted valuations = symmetric algebra = bosons; squarefree valuations = exterior

algebra = fermions. The exchange phase $R = (e^{i\pi})^{2s}$ is the selector of the

exponential modality at every place.

3.4 Tie-in to spin statistics and the tree program

The recent spin-statistics work established two things the adelic picture now absorbs:

1. $R = e^{2\pi i s} = (e^{i\pi})^{2s}$ as a logical scalar: the exchange phase is

the $(2s)$-fold half-turn of the re-entrant mark [3]. In the present dictionary, the

half-turn $e^{i\pi} = -1$ is the fermion sign at the archimedean place: $R = -1$

for $s = 1/2$, exactly as the squarefree restriction realizes the fermionic

occupation channel at the p-adic places. The two statistics dichotomies are the same

dichotomy in two places: the half-turn (archimedean exchange) and the valuation

restriction (p-adic occupation) both select the exterior algebra over the symmetric

algebra. [MAP — the arithmetic is exact; the physical identification is the model.]

1. The p-adic anyon embedding: the p-adic anyon program realizes braiding phases at

roots of unity $\zeta_{2p^k} \mapsto e^{2\pi i/(2p^k)} = (e^{i\pi})^{1/p^k}$, i.e.

rational spins $s = m/(2p^k)$ [3, §8]. Verified computationally: $\zeta_4 = i$,

$\zeta6 = e^{i\pi/3}$, $\zeta8 = e^{i\pi/4}$ — the $(1/p^k)$-th roots of the

half-turn. The rational-spin subsector of $R = (e^{i\pi})^{2s}$ is exactly the

p-adic braiding phase lattice. [ESTABLISHED arithmetic; consistency of the two

programs confirmed.]

The companion record One Table, Two Regimes [10] reads statistics as a

tree-automorphism phase on the Bruhat–Tits tree, unifying the standard-model particle

catalog with the condensed-matter excitation zoo. The valuation-restriction dictionary

of this paper — unrestricted valuations = bosonic, squarefree = fermionic — is the

companion occupation-statistics reading of the same non-archimedean statistics

dichotomy; the two readings are consistent and mutually supporting.

4. Thermodynamics: The 2π and the Planckian Bound

4.1 The thermal Gaussian and LCI_opt

The Gaussian $e^{-\pi x^2}$ maximizes differential entropy at fixed variance —

$h = \tfrac12\ln(2\pi e \sigma^2)$ (verified: $\sigma=1 \to 1.4189\ldots$,

$\sigma=\tfrac12 \to 0.7258\ldots$, $\sigma=2 \to 2.1121\ldots$). The constant $2\pi e$

appears as the entropy scale. The Quantum Architectonics program [4] derived the

Lossless Complexity Index optimum $\mathrm{LCI}_{\mathrm{opt}} = \ln(2\pi) \approx

1.8379$ — the natural log of the circle trace. Both the Gaussian entropy and the

architectural optimum carry the circle constant; in the re-entrant calculus, $\pi$ is

the trace of the identity on the circle type — the same $\pi$. [ESTABLISHED arithmetic;

LCI_opt verified: $\ln(2\pi) = 1.837877\ldots$]

4.2 Planckian dissipation and the MSS bound

The Planckian dissipation bound (Maldacena–Shenker–Stanford [15]) states

with the Planckian scattering time $\tau\hbar \approx \hbar/kB T$. The numerical

values (verified): at $T = 300\ \mathrm{K}$, $\lambda_{\max} = 2.468\times10^{14}\

\mathrm{s}^{-1}$, $\tau_\hbar = 2.546\times10^{-14}\ \mathrm{s}$; at $T = 77\

\mathrm{K}$, $\lambda_{\max} = 6.334\times10^{13}\ \mathrm{s}^{-1}$; at $T = 4\

\mathrm{K}$, $\lambda_{\max} = 3.29\times10^{12}\ \mathrm{s}^{-1}$.

The structural observation for the present synthesis: **the $2\pi$ in the MSS bound is

the trace of the identity on the circle type.** The maximal Lyapunov exponent is

$2\pi \times k_B T/\hbar$ — one circle-trace per thermal unit. The bound is the

statement that dissipation cannot exceed one re-entrant turn per thermal time. The

Planckian wall is the wall of the half-turn: $\tau\hbar = \hbar/kB T$ is the time in

which the phase $e^{-iEt/\hbar}$ accumulates one radian of thermal rotation; the $2\pi$

bound is the full turn. [MAP — dimensional and structural identification; the

identification of the MSS $2\pi$ with the circle trace is a reading, not a derivation.]

The companion program From Distinction to Dissipation [12] supplies the

thermodynamics–statistics interface of the same program: second-law-gated braids and

boundary costs, with a capacity ceiling $\lfloor \Delta S / (k_B \ln 2) \rfloor$ and a

$2kT \ln 2$ inversion toll. The thermodynamic arm of this paper ($\beta_p$, Planckian

$2\pi$) extends that bridge to the p-adic place.

4.3 The p-adic temperature as a thermodynamic scale

The new results R1/R2 give the p-adic place a genuine thermodynamic reading:

$\beta_p = \ln p$ is an inverse temperature. The p-adic entropy

$Hp^{\max} = 1/(p-1) = \langle n \rangle{\mathrm{BE}}(\beta_p)$ is a physical

occupation number. The thermodynamic program of the Joules-per-Solution benchmark [5] —

the energy cost of a correct quantum answer — gains a per-prime cost scale: the energy

to resolve a p-adic digit is set by $kB Tp$ with $T_p = 1/\ln p$ (in units where

$\beta = 1/kB T$). The prime $p = 2$ (binary digit) has $T2 = 1/\ln 2 \approx 1.4427$

— the temperature of the smallest prime, hence the highest of all p-adic temperatures;

higher primes are colder ($T3 \approx 0.91$, $T5 \approx 0.62$). [CONJECTURE — the

thermodynamic interpretation of $\beta_p$ as a physical temperature is proposed here for

the first time; it is falsifiable via the conditions of Section 7.]

5. QND Measurement: The Equality Case

5.1 What QND is

A quantum non-demolition measurement measures an observable $A$ without disturbing it:

the measurement Hamiltonian commutes with $A$, so repeated measurements of $A$ give the

same result (the back-action is confined to the conjugate variable). QND is the

workhorse of continuous quantum measurement and quantum metrology — cavity QED,

gravitational-wave interferometry, and superconducting-qubit readout [18, 19, 20].

5.2 New result R3: QND = equality case of the DPI

The adelic data-processing inequality (Adelic Shannon Theory [1], Theorem 1′) states:

for a p-adically contractive channel $T$, $Hp(T(X)) \le Hp(X)$ — information cannot

be created by p-adic processing. An ideal QND measurement of a p-adic-valued observable

$A$ is the equality case: the post-measurement distribution of $A$ equals the

pre-measurement distribution (the measurement does not disturb $A$), so

Verified computationally: for the distribution

$p = \{0.5, 0.25, 0.13, 0.06, 0.03, 0.02, 0.01\}$ over $v2$, $Hp = 0.97$ before and

after an ideal QND readout — invariant by construction, and this invariance is

precisely the equality case of the inequality. The v1.1 verification adds a

non-tautological contrast: over 200,000 seeded shots, the QND readout reproduces the

exact pre-measurement valuation on every shot (readout fidelity 1.0), whereas a

demolishing channel that redraws from the same marginal matches the true value only

with probability $\sum_k p(k)^2 \approx 0.336$ — the demolition is information-lossy

while QND is not. [ESTABLISHED — definitional; the content is the identification, which

is exact, plus the contrast demonstration.]

The same holds at the archimedean place: QND preserves the full information vector

$\mathbf{I}(X) = (I\infty, I2, I_3, \ldots)$ of the measured observable. **QND is the

measurement family that saturates the data-processing inequality componentwise:** among

measurement channels acting on $A$, the equality case (post-measurement distribution of

$A$ equal to its pre-measurement distribution) is precisely the non-demolition case. It

is the information-conserving measurement: it extracts the readout without paying

entropy in the measured channel. The category-theoretic record Valuation Without R [11]

supplies a valuation-first foundation for finite measurement that is directly

complementary to this reading.

5.3 The Born-rule boundary

The pre-registered falsification of deterministic measurement-triggered relaxation [6]

showed that a deterministic map from a fixed initial state yields a degenerate outcome

channel — measured probabilities take only the values 0 or 1 (max deviation 0.5,

verified). Born statistics require one of three ingredients: an ensemble over initial

states, stochasticity in the dynamics, or contextual hidden variables.

The QND connection: QND measurement is the fourth possibility that the

falsification's three-ingredient taxonomy implicitly leaves open — not a relaxation at

all, but an information-conserving readout of a pre-existing value. QND does not try to

reproduce the Born rule from deterministic relaxation; it reads what is there and

changes nothing. The Born statistics of a QND measurement are inherited from the

preparation ensemble (ingredient 1) — which is why QND works: it adds zero measurement

noise to the measured observable. The p-adic entropy conservation of R3 is the

quantitative statement of this "zero measurement noise."

5.4 QND and the entropic number

The Measurement Stratigraphy [9] and Adelic Entropic Numbers [8] program defined the

entropic number $(x, \mathbf{I}(X))$: a best estimate plus its full adelic information

vector. The present synthesis gives QND measurement its natural data type: **a QND

measurement of $x$ returns the entropic number $(x, \mathbf{I}(X))$ with

$\mathbf{I}(X)$ unchanged — the honest number, read without demolition.** The Gaussian

$e^{-\pi x^2}$ is the universal entropic number (max-entropy at every place); QND is

the measurement that preserves it. The two programs meet: entropic numbers are the data

type of QND metrology. [MAP — structural identification; the experimental realization

is future work.]

6. The Unification Map

Every row is a fixed point of a self-referential operation; every scalar is a member of

the re-entrant family ($e$ as fixed point of $D$, $\pi$ as circle trace,

$R = (e^{i\pi})^{2s}$ as monodromy power); the half-turn $e^{i\pi} = -1$ is the shared

generator (statistics at the archimedean place, fermion sign, the exchange dichotomy);

the p-adic places realize the same structure with $\beta_p = \ln p$.

The relationship, in one sentence: information theory, statistics, thermodynamics,

and QND measurement are the four faces of the self-referential scalar family of the

re-entrant mark — $e$ (local self-reference: $Df = f$), $\pi$ (global self-reference:

the circle's trace), and their combination $e^{i\pi} = -1$ (the half-turn), whose

$(2s)$-fold power is the exchange phase that selects the statistics, whose thermal

realization is the Boltzmann/max-entropy family with the Planckian bound as its

dissipation ceiling, and whose measurement theory is the QND channel that conserves the

information vector exactly.

7. Falsifiability and Status Ladder

Status ladder

Falsifiability conditions

• F1 (thermal p-adic scale). If a physical process is exhibited whose energy cost

per resolved p-adic digit scales other than $\sim kB Tp = k_B/\ln p$ (or with a

different prime ordering than $T2 > T3 > T_5 > \ldots$), the thermodynamic reading

of $\betap$ is disconfirmed. The ordering $T2 \approx 1.44 > T_3 \approx 0.91 >

T_5 \approx 0.62$ is the sharpest prediction.

• F2 (QND conservation). If a measurement is exhibited that is QND for a

p-adic-valued observable (commutes with it, repeatable) yet changes $H_p$ of that

observable, R3 is disconfirmed. (This is definitionally impossible for ideal QND; the

test applies to any claimed "effective QND" realization.)

• F3 (statistics–valuation dictionary). If a physical system with p-adic-valued

observables exhibits occupation statistics at the p-adic place that are neither

geometric (bosonic) nor squarefree-Bernoulli (fermionic) — e.g. a $q$-analogue with

$q \ne 1/p$ — the dictionary of Section 3.3 is disconfirmed for that system. (The

dictionary remains a classification claim: it does not predict which systems realize

which statistics.)

• F4 (unification thesis). If a member of the scalar family $(e, \pi, R)$ is shown

to arise in one of the four domains from a non-self-referential origin that is

incompatible with the re-entrant generation, the unification thesis is weakened to a

correspondence. The thesis is strengthened by each independent derivation of the same

constant from distinction.

8. What a Practitioner Can Do With This

1. QND metrology with p-adic observables. Any quantum sensor whose observable has

number-theoretic structure (photon numbers, flux quanta, harmonic-oscillator levels)

can carry a per-prime uncertainty budget: $H_p$ is conserved by QND readout, so the

p-adic digits of the measurement are the noise-free channel. The information vector

$\mathbf{I}(X) = (I\infty, I2, I_3, \ldots)$ is the complete metrological error

budget — a concrete specification for sensor calibration.

1. p-adic noise models in quantum engineering. The AUM channel with

$\betap = \ln p$ gives a closed-form capacity $Cp = \logp(1 + \mathrm{SNR}p)$

for noise whose valuation structure is prime-specific; the doubling

$C2 = 2C\infty$ (verified for all SNR) is a design rule for binary-resolved

systems.

1. Energy benchmarking per prime digit. The Joules-per-Solution metric [5] gains a

place-wise decomposition: the energy to resolve a p-adic digit is set by

$kB Tp = k_B/\ln p$; a benchmark that reports energy per prime digit is directly

comparable across architectures.

1. Planckian design rule. The MSS bound $\lambdaL \le 2\pi kB T/\hbar$ with the

circle-trace reading gives architects of strongly correlated systems a dimensionless

target: $\mathrm{LCI} = \ln(2\pi)$ is the optimal structural complexity; the $2\pi$

is not a convention but the trace of the identity on the circle type — the same

constant in the re-entrant calculus and in the dissipative bound.

1. Measurement-channel accounting. The QND equality case gives a practical audit

rule for measurement chains: any measurement that reduces $H_p$ of the measured

observable is non-QND (it has demolition back-action); the information loss is

exactly $Hp(\text{before}) - Hp(\text{after})$, computable in situ.

9. Relation to the Prior Work

• Adelic Shannon Theory [1]: supplied $H_p$, the AUM channel, the product-formula coding

theorem, the Gaussian as universal max-entropy function. This paper adds the

statistical-mechanical reading (R1, R2), the QND equality case (R3), and the

thermodynamic arm ($\betap$, $Tp$).

• The Exchange Phase as a Logical Scalar [3] and The Boson/Fermion Distinction [2]:

supplied $R = (e^{i\pi})^{2s}$, the two-modal-exponential construction, the p-adic

anyon embedding. This paper ties those to the occupation-number distributions (the

exponentials are the BE/FD distributions at the p-adic place) and to the Planckian

bound.

• One Table, Two Regimes [10]: reads statistics as a tree-automorphism phase on the

Bruhat–Tits tree, unifying the standard-model particle catalog with the

condensed-matter excitation zoo. This paper's valuation-restriction dictionary is the

companion occupation-statistics reading of the same non-archimedean statistics

dichotomy; the two records are consistent and mutually supporting.

• Valuation Without R [11]: supplies a category-theoretic foundation for finite

measurement without the real numbers. This paper's R3 is the measurement-theoretic

statement in the same valuation-first direction; the two records should be cited

together.

• From Distinction to Dissipation [12]: second-law-gated braids and boundary costs at

the thermodynamics–statistics interface of the same program. This paper's

thermodynamic arm ($\beta_p$, Planckian $2\pi$) extends that bridge to the p-adic

place.

• The Calculus of Re-Entrant Distinctions [7]: supplied $e$ and $\pi$ as logical scalars

of the mark. This paper adds the third and fourth faces (Fourier fixed point;

max-entropy fixed point) and the thermodynamic $2\pi$.

• Measurement Stratigraphy [9] and Adelic Entropic Numbers [8]: supplied entropic

numbers and the observer-relativity reading. This paper identifies QND as the

measurement that realizes entropic numbers without demolition.

• Quantum Architectonics / Planckian Dissipation [4]: supplied

$\mathrm{LCI}_{\mathrm{opt}} = \ln(2\pi)$ and the Signal-Worker ontology. This paper

connects $\mathrm{LCI}_{\mathrm{opt}}$ to the circle trace and the MSS $2\pi$ to the

half-turn.

• A Pre-Registered Falsification of Deterministic Measurement-Triggered Relaxation [6]:

supplied the three-ingredient taxonomy of Born statistics. This paper adds QND as the

information-conserving fourth path and the $H_p$-conservation criterion.

• External anchors: Shannon [16], Pauli [13], Leinaas–Myrheim [14], Wilczek [17],

Maldacena–Shenker–Stanford [15]; QND characterization and certification [18, 19, 20].

10. Conclusion

Information theory, statistics, thermodynamics, and QND quantum measurement are

organized by one self-referential scalar family — $e$, $\pi$, and $R = (e^{i\pi})^{2s}$

— generated by the re-entrant mark and realized at every place of the rationals. The

p-adic maximum-entropy distribution is a Bose–Einstein distribution at $\beta_p = \ln

p$; the squarefree integers are its Fermi–Dirac counterpart; the exchange phase selects

the statistics; the Planckian bound is the circle trace in thermal units; and QND

measurement is the equality case of the data-processing inequality — the channel that

conserves the information vector exactly. The premises end where the identification of a

physical temperature at the p-adic place begins: the algebra is exact, the physics is

proposed, and the falsification conditions are written.

Declarations

• Funding: This research received no external funding.
• Conflicts of interest: The author declares no conflicts of interest.
• Verification: All numerical claims verified by

artifacts/verification/adelic-stats-verification.py (deposited source; stdlib-only

CPython 3; deterministic — seeded Monte Carlo (seed 20260820, 200,000 shots) only for

the QND readout-fidelity contrast; squarefree sieve N = 2×10⁶; output

adelic-stats-verification-2026-08-20.json, 38 checks, all pass). Reproducibility:

python artifacts/verification/adelic-stats-verification.py re-generates the JSON

byte-identically (run log: run-2026-08-20.txt).

• AI assistance: AI-assisted drafting and verification orchestration; all

computational results produced by the deposited executed code.

• Preprint policy: Self-archived working paper; not submitted for journal peer

review (standing venue policy: Zenodo).

References

[1] Quni-Gudzinas, R. B. (2026). Adelic Shannon Theory: From Problem Statement to

Constructive Foundations. 10.5281/zenodo.22024240 (concept 21698975).

[2] Quni-Gudzinas, R. B. (2026). The Boson/Fermion Distinction: Spin-Statistics as

Structural Invariant. 10.5281/zenodo.21964598 (concept 21938970).

[3] Quni-Gudzinas, R. B. (2026). The Exchange Phase as a Logical Scalar:

$R = e^{2\pi i s}$ from the Re-Entrant Calculus. 10.5281/zenodo.21964104 (concept

21941184).

[4] Quni-Gudzinas, R. B. (2026). Structural Mediation of Planckian Dissipation in

Strongly Correlated Electron Systems: A Universal Architectonic Approach.

10.5281/zenodo.18465372.

[5] Quni-Gudzinas, R. B. (2026). The Joules-per-Solution Metric.

10.5281/zenodo.21637028.

[6] Quni-Gudzinas, R. B. (2026). A Pre-Registered Falsification of Deterministic

Measurement-Triggered Relaxation. 10.5281/zenodo.22026562.

[7] Quni-Gudzinas, R. B. (2026). The Calculus of Re-Entrant Distinctions: A Unified

Treatise on the Loop, the Tree, and the Constants of Self-Reference.

10.5281/zenodo.21964453 (concept 21904762).

[8] Quni-Gudzinas, R. B. (2026). Adelic Entropic Numbers: When the Adelic Information

Vector Becomes the Entropic Number. 10.5281/zenodo.21698978.

[9] Quni-Gudzinas, R. B. (2026). The History and Future of Measurement Stratigraphy,

Number Theory, and Valuation Theory. 10.5281/zenodo.21705220 (concept 21698493).

[10] Quni-Gudzinas, R. B. (2026). One Table, Two Regimes: Standard-Model Particles and

Condensed-Matter Excitations as Patterns on the Bruhat–Tits Tree.

10.5281/zenodo.22024856.

[11] Quni-Gudzinas, R. B. (2026). Valuation Without R: A Category-Theoretic Foundation

for Finite Measurement. 10.5281/zenodo.21803677.

[12] Quni-Gudzinas, R. B. (2026). From Distinction to Dissipation: Companion Essay and

Executable Toy-Model Suite for the Boson/Fermion Distinction Program.

10.5281/zenodo.21940822 (also 21943007).

[13] Pauli, W. (1940). The Connection Between Spin and Statistics. Physical Review 58,

716–722. 10.1103/PhysRev.58.716.

[14] Leinaas, J. M., and J. Myrheim (1977). On the theory of identical particles. Il

Nuovo Cimento B 37, 1–23. 10.1007/BF02727953.

[15] Maldacena, J., S. H. Shenker, and D. Stanford (2016). A bound on chaos. JHEP 08,

1. 10.1007/JHEP08(2016)106.

[16] Shannon, C. E. (1948). A Mathematical Theory of Communication. Bell System

Technical Journal 27, 379–423. 10.1002/j.1538-7305.1948.tb01338.x.

[17] Wilczek, F. (1982). Quantum Mechanics of Fractional-Spin Particles. Physical

Review Letters 49, 957–959. 10.1103/PhysRevLett.49.957.

[18] Unnikrishnan, C. S. (2018). Quantum non-demolition measurements: Concepts, theory

and practice. arXiv:1811.09613.

[19] Sewell, R. J., M. Napolitano, N. Behbood, G. Colangelo, and M. W. Mitchell (2013).

Certified quantum non-demolition measurement of a macroscopic material system. Nature

Photonics 7, 517–520. 10.1038/nphoton.2013.100; arXiv:1303.2490.

[20] Ralph, T. C., S. D. Bartlett, J. L. O'Brien, G. J. Pryde, and H. M. Wiseman (2004).

Quantum Non-demolition Measurements on Qubits. arXiv:quant-ph/0412149.