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arxiv: 2604.22752 · v1 · submitted 2026-04-24 · 📊 stat.ME

From Physics to Statistics: A Simple Route to Exponential Families via Maximum Entropy

Pith reviewed 2026-05-08 11:06 UTC · model grok-4.3

classification 📊 stat.ME
keywords exponential familiesmaximum entropyinformation entropycanonical statisticssufficient statisticsbase distributionuniform basestatistical modeling
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The pith

Exponential families maximize entropy subject to fixed expectations of canonical statistics.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper presents a direct derivation showing that exponential families arise as the unique distributions that achieve maximum entropy under constraints fixing the expected values of a set of statistics. It establishes two results: families built on an arbitrary base distribution maximize relative entropy with respect to that base, while those on a uniform base maximize ordinary entropy. The argument relies only on basic properties of entropy and avoids Lagrange multipliers or other optimization machinery. A reader would care because this grounds a core statistical structure in the maximum-entropy principle from physics, making the motivation accessible with modest prerequisites and underscoring why entropy ideas belong in introductory statistics teaching.

Core claim

Exponential families with a general base maximise information entropy with respect to that base subject to fixed expectations of canonical statistics, and exponential families with a uniform base maximise standard information entropy under the same constraints. Maximum entropy therefore supplies a principled, first-principles foundation for exponential families that requires only modest background in information entropy.

What carries the argument

The maximum entropy principle applied directly to distributions whose expectations of canonical statistics are held fixed, using entropy properties to identify the exponential form without constrained optimisation.

If this is right

  • Exponential families are the unique maximum-entropy distributions under the stated moment constraints.
  • The same uniqueness holds both for relative entropy with any base measure and for absolute entropy with the uniform base.
  • The derivation uses only elementary entropy identities and does not invoke Lagrange multipliers or convex analysis.
  • Maximum entropy supplies a transparent justification for employing exponential families throughout statistics and machine learning.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Introducing entropy concepts earlier in statistics curricula could render generalized linear models and related structures more intuitive from the outset.
  • The same direct entropy argument may extend to other constrained families arising in machine learning, such as energy-based models.
  • The physics-to-statistics link invites examination of whether additional structures from statistical mechanics translate into new statistical estimators.

Load-bearing premise

A direct argument based on entropy properties can replace constrained optimisation while remaining rigorous and self-contained with only modest background in information entropy.

What would settle it

Exhibiting any probability distribution that matches the same fixed expectations of the canonical statistics yet attains strictly higher entropy than the corresponding exponential-family member.

read the original abstract

Exponential families form the backbone of modern statistics and machine learning, but textbooks seldom derive them from first principles in an accessible way. Although minimal sufficiency and the principle of maximum entropy, originating in physics, provide core motivation, they are often presented as technical and requiring advanced prerequisites. Here, a short, self-contained derivation of exponential families based on maximum entropy is presented that is straightforward to carry out, requires only a modest background in information entropy, and avoids technicalities like constrained optimisation. Two propositions are demonstrated in this fashion: i) exponential families with a general base maximise information entropy with respect to that base subject to fixed expectations of canonical statistics, and ii) exponential families with a uniform base maximise standard information entropy under the same constraints. Maximum entropy therefore provides a principled foundation for exponential families with minimal prerequisites, highlighting the value of teaching entropy in statistics courses.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 2 minor

Summary. The manuscript presents a short, self-contained derivation claiming that exponential families arise directly from the maximum entropy principle. It demonstrates two propositions: (i) exponential families with general base measure h(x) maximize relative entropy with respect to that base subject to fixed expectations of canonical statistics T(x), and (ii) those with uniform base maximize Shannon entropy under the same constraints. The argument is asserted to rely only on elementary entropy properties (non-negativity of relative entropy, chain rule) without constrained optimization or advanced prerequisites.

Significance. If the derivation is fully rigorous and gap-free, the paper would supply a pedagogically useful route to exponential families that links the physics maximum-entropy principle to statistical modeling with minimal background. This could strengthen the case for teaching entropy concepts in statistics curricula. The self-contained nature of the argument is a positive feature when it succeeds.

major comments (1)
  1. [Derivation of Propositions 1 and 2] The central derivation (appearing after the abstract's statement of the two propositions) must be examined for whether it obtains the explicit form p(x) = h(x) exp(λ · T(x) − A(λ)) solely from elementary entropy inequalities without an implicit variational step equivalent to Lagrange multipliers. The abstract gives no indication of the intermediate steps; if the argument relies on an unstated inequality that presupposes the exponential ansatz or requires measure-theoretic handling of the base measure, the claim of avoiding technicalities fails. This is load-bearing for both propositions.
minor comments (2)
  1. [Introduction and Proposition statements] Clarify the precise statement of the constraints (fixed expectations of T(x)) and the domain of the base measure h(x) at the outset of each proposition to avoid ambiguity in the entropy expressions.
  2. [Derivation section] Add a short remark on how the log-partition function A(λ) emerges naturally from normalization within the entropy argument, rather than being introduced separately.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their careful reading of the manuscript and for identifying the need to verify that the central derivation is fully rigorous and free of hidden technical steps. We address the single major comment below and have revised the manuscript to improve clarity on this point while preserving the elementary character of the argument.

read point-by-point responses
  1. Referee: [Derivation of Propositions 1 and 2] The central derivation (appearing after the abstract's statement of the two propositions) must be examined for whether it obtains the explicit form p(x) = h(x) exp(λ · T(x) − A(λ)) solely from elementary entropy inequalities without an implicit variational step equivalent to Lagrange multipliers. The abstract gives no indication of the intermediate steps; if the argument relies on an unstated inequality that presupposes the exponential ansatz or requires measure-theoretic handling of the base measure, the claim of avoiding technicalities fails. This is load-bearing for both propositions.

    Authors: We are grateful for this comment, which highlights the importance of transparency in the logical steps. The derivation obtains the stated form without presupposing the exponential ansatz and without any variational or Lagrange-multiplier step, implicit or explicit. It begins with an arbitrary distribution p that satisfies the moment constraints E_p[T(x)] = μ. The relative entropy D(p || q) is then introduced for a comparison distribution q constructed as q(x) ∝ h(x) exp(λ · T(x)), where the parameter λ is fixed by the requirement that q itself obeys the same moment constraints (this is always possible because the log-partition function A(λ) is strictly convex). Non-negativity of D(p || q) together with the chain rule for entropy immediately yields H(p) ≤ A(λ) − λ · μ + E_p[log(1/h(x))], with equality if and only if p = q almost everywhere. Consequently the exponential family member saturates the bound and is the unique maximizer. No optimization problem is solved and no measure-theoretic subtleties beyond the standard definition of relative entropy are invoked. To remove any residual ambiguity we have inserted a short, numbered outline of these steps immediately after the statements of the two propositions. revision: yes

Circularity Check

0 steps flagged

Derivation is self-contained via external maximum entropy principle and standard entropy properties

full rationale

The paper presents a short derivation of the exponential family form from the maximum entropy principle using only elementary properties of entropy (non-negativity of relative entropy, chain rule, etc.) without invoking constrained optimization or self-referential equations. No steps reduce by construction to fitted parameters, self-citations, or imported uniqueness theorems from the authors' prior work. The central propositions are shown directly from the stated entropy axioms and the fixed-expectation constraints, remaining independent of the target functional form. This qualifies as an honest non-finding of circularity.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The central claim rests on the maximum entropy principle as the selection criterion and on the definition of information entropy; no free parameters or new entities are introduced.

axioms (2)
  • domain assumption The principle of maximum entropy selects the distribution that is maximally uncertain given the constraints.
    Invoked as the foundational motivation and selection rule for deriving the exponential family form.
  • standard math Information entropy is defined in the standard way with respect to a base measure.
    Used to state the objective being maximized in both propositions.

pith-pipeline@v0.9.0 · 5439 in / 1191 out tokens · 44329 ms · 2026-05-08T11:06:29.332025+00:00 · methodology

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Reference graph

Works this paper leans on

35 extracted references · 35 canonical work pages

  1. [1]

    Akaike, H. (1985). Prediction and entropy. In Atkinson, A. and Fienberg, S., editors, A Celebration of Statistics , chapter 1, pages 1--24. Springer

  2. [2]

    Amari, S. (2016). Information Geometry and Its Applications . Springer

  3. [3]

    Barankin, E. W. and Maitra, A. P. (1963). Generalization of the Fisher - Darmois - Koopman - Pitman theorem on sufficient statistics. Sankhy\= a A , 25:217--244

  4. [4]

    Cover, T. M. and Thomas, J. A. (2006). Elements of Information Theory . John Wiley & Sons, 2nd edition

  5. [5]

    Darmois, G. (1935). Sur les lois de probabilit\' e \` a estimation exhaustive. C. R. Acad. Sci. Paris , 200:1265--1266

  6. [6]

    Dawid, A. (2007). The geometry of proper scoring rules. Ann. Inst. Statist. Math. , 59:77--93

  7. [7]

    Efron, B. (2022). Exponential Families in Theory and Practise . Cambridge University Press

  8. [8]

    Esscher, F. (1932). On the probability function in the collective theory of risk. Scand. Actuar. J. , 15:175--195

  9. [9]

    Fisher, R. A. (1934). Two new properties of mathematical likelihood. Proc. R. Soc. Lond. A , 144:285--307

  10. [10]

    Golan, A. (2018). Foundations of Info-Metrics: Modeling, Inference, and Imperfect Information . Oxford University Press

  11. [11]

    Jaynes, E. T. (1957). Information theory and statistical mechanics. Phys. Rev. , 106:620--630

  12. [12]

    Jaynes, E. T. (1968). Prior probabilities. IEEE Trans. Syst. Sci. Cybern. , 4:227--241

  13. [13]

    Khan, M. E. and Rue, H. (2023). The bayesian learning rule. J. Mach. Learn. Res. , 24(281):1--46

  14. [14]

    Knoblauch, J., Jewson, J., and Damoulas, T. (2022). An optimization-centric view on bayes' rule: Reviewing and generalizing variational inference. J. Mach. Learn. Res. , 23(132):1--109

  15. [15]

    and Kitagawa, G

    Konishi, S. and Kitagawa, G. (2008). Information Criteria and Statistical Modeling . Springer

  16. [16]

    Koopman, B. O. (1936). On distributions admitting a sufficient statistic. Trans. Amer. Math. Soc. , 39:399--409

  17. [17]

    and Leibler, R

    Kullback, S. and Leibler, R. A. (1951). On information and sufficiency. Ann. Math. Statist. , 22:79--86

  18. [18]

    Leff, H. S. (1996). Thermodynamic entropy: The spreading and sharing of energy. Am. J. Phys. , 64:1261--1271

  19. [19]

    Leff, H. S. (2007). Entropy, its language, and interpretation. Bell Syst. Tech. J. , 77:1744--1766

  20. [20]

    Levine, R. D. and Tribus, M., editors (1979). The Maximum Entropy Formalism . MIT Press

  21. [21]

    Little, M. A. (2019). Machine Learning for Signal Processing: Data Science, Algorithms, and Computational Statistics . Oxford University Press

  22. [22]

    Mandelbrot, B. (1962). The role of sufficiency and of estimation in thermodynamics. Ann. Math. Statist , 33:1021--1038

  23. [23]

    Mandl, F. (1988). Statistical Physics . Wiley, 2nd edition

  24. [24]

    McElreath, R. (2020). Statistical Rethinking . Chapman and Hall/CRC, 2nd edition

  25. [25]

    Morris, C. N. and Lock, K. F. (2009). Unifying the named natural exponential families and their relatives. Am. Stat. , 63:247--253

  26. [26]

    Murphy, K. P. (2012). Machine Learning: A Probabilistic Perspective . MIT Press

  27. [27]

    Murphy, K. P. (2023). Probabilistic Machine Learning: Advanced Topics . MIT Press

  28. [28]

    A., Yang, Y.-J., and Dill, K

    Pachter, J. A., Yang, Y.-J., and Dill, K. A. (2024). Entropy, irreversibility and inference at the foundations of statistical physics. Nat. Rev. Physics , 6:382--393

  29. [29]

    Pitman, E. J. G. (1936). Sufficient statistics and intrinsic accuracy. Math. Proc. Camb. Philos. Soc. , 32:567--579

  30. [30]

    Reif, F. (1965). Fundamentals of Statistical and Thermal Physics . McGraw-Hill

  31. [31]

    D., editor (1983)

    Rosenkrantz, R. D., editor (1983). E. T. Jaynes: Papers on Probability, Statistics and Statistical Physics . D. Reidel Publishing Company

  32. [32]

    and Johnson, R

    Shore, J. and Johnson, R. (1981). Properties of cross-entropy minimization. IEEE Trans. Inform. Theory , 27:472--482

  33. [33]

    Sundberg, R. (2019). Statistical Modelling by Exponential Families . Cambridge University Press

  34. [34]

    Wainwright, M. J. and Jordan, M. I. (2008). Graphical models, exponential families, and variational inference. Found. Trends Mach. Learn. , 1:1--305

  35. [35]

    Wehrl, A. (1978). General properties of entropy. Rev. Mod. Phys. , 50:221--260