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arXiv math/0102031math.GM
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黎曼假设与超共形不变性

Riemann hypothesis and super-conformal invariance

Matti Pitkanen

摘要:

一个战略证明(不是证明,因为是第一个过于乐观的信念)的黎曼假设的建议。黎曼Zeta的消失归结为一个以黎曼Zeta的零点为特征值的非厄米特算子D^+的特征函数的正交条件。构造D^+的灵感来自于这样一种信念:黎曼泽塔与一个物理系统相关联,该系统允许超共形变换作为其对称性,并允许根据超共形代数的表示进行二次量子化。D^+的本征函数类似于所谓的相干态,并且一般彼此不正交。与真空态正交的态(具有负范数平方)对应于黎曼ζ的零点。具有正范数平方的物理状态对应于临界线处的黎曼Zeta零点。黎曼假设由以下假设推导出:普通超共形代数作为所有与真空态正交的相干态的规范对称性,也包括可能存在于临界线之外的非物理相干态。

英文摘要:

A strategy for proving (not a proof of, as was the first over-optimistic belief) the Riemann hypothesis is suggested. The vanishing of Riemann Zeta reduces to an orthogonality condition for the eigenfunctions of a non-Hermitian operator D^+ having the zeros of Riemann Zeta as its eigenvalues. The construction of D^+ is inspired by the conviction that Riemann Zeta is associated with a physical system allowing superconformal transformations as its symmetries and second quantization in terms of the representations of superconformal algebra. The eigenfunctions of D^+ are analogous to the so called coherent states and in general not orthogonal to each other. The states orthogonal to a vacuum state (having a negative norm squared) correspond to the zeros of Riemann Zeta. The physical states having a positive norm squared correspond to the zeros of Riemann Zeta at the critical line. Riemann hypothesis follows by reductio ad absurdum from the hypothesis that ordinary superconformal algebra acts as gauge symmetries for all coherent states orthogonal to the vacuum state, including also the non-physical coherent states that might exist off from the critical line.

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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