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arXiv 0907.5313quant-phhep-thmath-phmath.MP
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自旋、统计和第一原理

Spin and Statistics and First Principles

Sergio Doplicher

摘要:

70年代初,在局域量子理论中,(这是量子场论的最一般的表述,如果我们只忽略量子引力的未知场景)统计学的概念可以仅仅基于局部的可观测量(不假设对易关系,甚至不假设不可观测带电场算符的存在);人们发现,只有众所周知的玻色/费米型(para)统计是允许的关键原则的局部可交换性的观察。在这个框架中,可以纯粹根据第一原理来制定和证明自旋和统计定理。在随后的阶段,它已经有可能证明存在一个独特的,规范代数的局部场运营商服从普通玻色/费米交换关系在类空分离。在这个一般的幌子自旋统计定理适用于理论(在四维闵可夫斯基空间),其中只有有限质量简并的大质量粒子可以发生。在这里,我们描述了基本的简单的基本思想,并简要地提到随后的概括;最后,我们评论的可能有效性的自旋统计定理的存在下,无质量的粒子,或违反局域性的预期在量子引力。

英文摘要:

It was shown in the early Seventies that, in Local Quantum Theory (that is the most general formulation of Quantum Field Theory, if we leave out only the unknown scenario of Quantum Gravity) the notion of Statistics can be grounded solely on the local observable quantities (without assuming neither the commutation relations nor even the existence of unobservable charged field operators); one finds that only the well known (para)statistics of Bose/Fermi type are allowed by the key principle of local commutativity of observables. In this frame it was possible to formulate and prove the Spin and Statistics Theorem purely on the basis of First Principles. In a subsequent stage it has been possible to prove the existence of a unique, canonical algebra of local field operators obeying ordinary Bose/Fermi commutation relations at spacelike separations. In this general guise the Spin - Statistics Theorem applies to Theories (on the four dimensional Minkowski space) where only massive particles with finite mass degeneracy can occur. Here we describe the underlying simple basic ideas, and briefly mention the subsequent generalisations; eventually we comment on the possible validity of the Spin - Statistics Theorem in presence of massless particles, or of violations of locality as expected in Quantum Gravity.

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