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arXiv 1012.4665math-phmath.MPmath.NTmath.QAquant-ph
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黎曼假设与量子力学

Riemann hypothesis and Quantum Mechanics

Michel Planat, Patrick Solé, Sami Omar

摘要:

在他们1995年的论文中,Jean-Benovitt Bost和Alain Connes(BC)构建了一个量子动力学系统,其配分函数是黎曼zeta函数$ζ(β)$,其中$β$是逆温度。我们将Riemann假设(RH)作为该理论的低温Kubo-Martin-Schwinger(KMS)态的一个性质。更准确地说,BC相位算子的期望值可以写为$$ϕ_β(q)=N_{q-1}^{β-1} ψ_{β-1}(N_q), $$其中$N_q=\prod_{k=1}^qp_k$是阶数$q$的素数,$ ψ_b $是依赖于一个实参数$b$的广义Dedekind $ψ$函数,为$$ ψ_b (q)=q \prod_{p \in \mathcal{P,}p \vert q}\frac{1-1/p^b}{1-1/p}.$$固定一个大的逆温度$β>2.$黎曼假设然后被证明是等价于$q$足够大的不等式$$ N_q |ϕ_β(N_q)|ζ(β-1) >e^γ\log \log N_q, $$。在相对湿度下,导出了高温KMS态($1.5< β<2$)的计算公式.

英文摘要:

In their 1995 paper, Jean-Benoît Bost and Alain Connes (BC) constructed a quantum dynamical system whose partition function is the Riemann zeta function $ζ(β)$, where $β$ is an inverse temperature. We formulate Riemann hypothesis (RH) as a property of the low temperature Kubo-Martin-Schwinger (KMS) states of this theory. More precisely, the expectation value of the BC phase operator can be written as $$ϕ_β(q)=N_{q-1}^{β-1} ψ_{β-1}(N_q), $$ where $N_q=\prod_{k=1}^qp_k$ is the primorial number of order $q$ and $ ψ_b $ a generalized Dedekind $ψ$ function depending on one real parameter $b$ as $$ ψ_b (q)=q \prod_{p \in \mathcal{P,}p \vert q}\frac{1-1/p^b}{1-1/p}.$$ Fix a large inverse temperature $β>2.$ The Riemann hypothesis is then shown to be equivalent to the inequality $$ N_q |ϕ_β(N_q)|ζ(β-1) >e^γ\log \log N_q, $$ for $q$ large enough. Under RH, extra formulas for high temperatures KMS states ($1.5< β<2$) are derived.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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