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Thermodynamic Stability and the Arithmetic Phase Transition of the Riemann Hypothesis

This article explores the connection between quantum statistical mechanics and the Riemann Hypothesis by analyzing the stability of KMS states in the Bost-Connes system and their relation to primorial inequalities.


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Introduction

The intersection of quantum statistical mechanics and analytic number theory represents a profound frontier in mathematical physics. At the heart of this convergence lies the Bost-Connes system, a C*-dynamical system that exhibits a phase transition with spontaneous symmetry breaking, where the partition function is the Riemann zeta function. The research paper arXiv:hal-00549030v3, authored by Michel Planat, Patrick Sole, and Sami Omar, extends this framework by establishing a direct link between the stability of Kubo-Martin-Schwinger (KMS) states and the Riemann Hypothesis.

The fundamental challenge in Riemann Hypothesis research is proving that all non-trivial zeros of the zeta function, zeta(s), lie on the critical line where the real part of s is 1/2. While traditional approaches rely on complex analysis, the approach in arXiv:hal-00549030v3 utilizes the thermodynamic properties of an arithmetic system. By defining a specific Hamiltonian based on the logarithms of integers and examining the behavior of the system at low temperatures, the authors derive inequalities that are equivalent to the truth of the Riemann Hypothesis.

Mathematical Background

The primary object of study is the C*-algebra C*(Q/Z) of additive or phase operators. These operators act on a Hilbert space spanned by qudits |n>, where n is a positive integer. The dynamics of the system are governed by a Hamiltonian H_0, defined such that the energy of the state |n> is log n. This leads to the evolution operator:

exp(-beta H_0)|n> = n^-beta

The partition function of the system is given by the trace of the evolution operator, which yields zeta(beta) for the real part of beta > 1. This identity identifies the inverse temperature of the physical system with the argument of the Riemann zeta function. For beta > 1, the system possesses a unique KMS_beta state, which describes the equilibrium of the system. A critical component of the argument is the evaluation of this state on primorial numbers N_q, which are the products of the first q primes.

Main Technical Analysis

Spectral Properties and Zero Distribution

The core of the technical argument rests on the behavior of the KMS state when evaluated at primorial numbers. The authors define a ratio epsilon_beta(q) that measures the deviation of the state magnitude from a theoretical threshold derived from Mertens' theorem. This threshold involves the Euler constant gamma and the zeta function evaluated at beta - 1.

For a square-free integer like a primorial N_q, the state simplifies to a product over the prime factors. The authors analyze this in the low-temperature regime, specifically where beta > 2. The significance of this range arises from the convergence properties of the Dirichlet series and the relationship to Robin's inequality, which states that the sum-of-divisors function satisfies a specific bound if and only if the Riemann Hypothesis is true.

The Role of Primorials in KMS States

The positivity of epsilon_beta(q) for all q serves as a generalized criterion for the Riemann Hypothesis. As q increases, the primorial N_q grows extremely rapidly, and log log N_q grows as log p_q (where p_q is the q-th prime). The term e^gamma / zeta(beta - 1) acts as the asymptotic limit of the ratio. The Riemann Hypothesis essentially constrains the fluctuations of the prime distribution such that this limit is approached from above.

If the Riemann Hypothesis were false, the oscillations in the prime density caused by zeros off the critical line would eventually force epsilon_beta(q) to become negative for infinitely many values of q. Thus, the thermodynamic stability of the KMS state is a physical manifestation of the Riemann Hypothesis.

Novel Research Pathways

Pathway 1: Explicit-Formula Expansion for Epsilon Deviations

One compelling research direction involves deriving a rigorous explicit-formula representation for the error function of epsilon_beta(q). This would involve converting the logarithmic derivative of the prime products into a sum over the non-trivial zeros of the zeta function. By identifying the leading oscillatory terms, researchers could quantify exactly how zero distributions force sign changes in the KMS inequality.

Pathway 2: Galois Group Actions and L-function Generalizations

The symmetry group of the Bost-Connes system is the Galois group Gal(Q_cycl/Q). This group acts on the space of KMS states. Future research could investigate "twisted" KMS states that correspond to Dirichlet L-functions. This would connect the stability of the Bost-Connes system to the Generalized Riemann Hypothesis, potentially providing a unified framework for all Dirichlet L-functions through quantum statistical mechanics.

Computational Implementation

The following Wolfram Language implementation calculates the epsilon_beta(q) values for a range of primorials and inverse temperatures. This allows for the numerical verification of the inequalities proposed in arXiv:hal-00549030v3.

Wolfram Language
(* Section: KMS State and Riemann Hypothesis Verification *)
(* Purpose: To compute the epsilon_beta(q) function for primorials *)

Module[{maxQ = 40, beta = 3.0, gamma = EulerGamma},
  (* Define the primorial N_q *)
  primorial[q_] := Product[Prime[i], {i, 1, q}];
  
  (* Define the KMS state magnitude |phi_beta(N_q)| *)
  kmsMagnitude[q_, b_] := Module[{nq = primorial[q], primes},
    primes = Table[Prime[i], {i, 1, q}];
    (nq^-b) * Product[(1 - Prime[i]^(b - 1))/(1 - 1/Prime[i]), {i, 1, q}]
  ];

  (* Define the epsilon_beta(q) function *)
  epsilon[q_, b_] := Module[{nq = primorial[q], phiMag},
    phiMag = Abs[kmsMagnitude[q, b]];
    (nq * phiMag / Log[Log[nq]]) - (Exp[gamma] / Zeta[b - 1])
  ];

  (* Generate data for analysis *)
  data = Table[{q, epsilon[q, beta]}, {q, 2, maxQ}];
  
  (* Visualize the results *)
  Print[ListLinePlot[data, 
    PlotRange -> All, 
    AxesLabel -> {"q (Primorial Index)", "epsilon_beta(q)"}, 
    PlotLabel -> "Positivity of epsilon for beta = " <> ToString[beta],
    Filling -> Bottom]];
    
  (* Check for violations *)
  negValues = Select[data, #[[2]] < 0 &];
  If[Length[negValues] == 0, 
    Print["No violations found. Consistent with RH."],
    Print["Potential violations at: ", negValues]
  ];
]

The investigation into arXiv:hal-00549030v3 reveals that the Riemann Hypothesis is not merely a statement about the distribution of primes, but a fundamental constraint on the thermodynamic equilibrium of arithmetic quantum systems. By mapping the zeta function to the partition function of the Bost-Connes system, the problem of complex analysis is transformed into one of spectral stability. The most promising avenue for further research lies in the refinement of the epsilon_beta(q) bound. While current evidence establishes positivity for beta > 2, a tighter analysis of the region closer to the critical temperature could bridge the gap to a definitive proof.

References

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