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Quantum mechanics on a p-adic Hilbert space: Foundations and prospects
International Journal of Geometric Methods in Modern Physics ( IF 2.1 ) Pub Date : 2024-03-11 , DOI: 10.1142/s0219887824400176
Paolo Aniello 1, 2 , Stefano Mancini 3, 4 , Vincenzo Parisi 3, 4
Affiliation  

We review some recent results on the mathematical foundations of a quantum theory over a scalar field that is a quadratic extension of the non-Archimedean field of p-adic numbers. In our approach, we are inspired by the idea — first postulated in [I. V. Volovich, p-adic string, Class. Quantum Grav.4 (1987) L83–L87] — that space, below a suitably small scale, does not behave as a continuum and, accordingly, should be modeled as a totally disconnected metrizable topological space, ruled by a metric satisfying the strong triangle inequality. The first step of our construction is a suitable definition of a p-adic Hilbert space. Next, after introducing all necessary mathematical tools — in particular, various classes of linear operators in a p-adic Hilbert space — we consider an algebraic definition of physical states in p-adic quantum mechanics. The corresponding observables, whose definition completes the statistical interpretation of the theory, are introduced as SOVMs, a p-adic counterpart of the POVMs associated with a standard quantum system over the complex numbers. Interestingly, it turns out that the typical convex geometry of the space of states of a standard quantum system is replaced, in the p-adic setting, with an affine geometry; therefore, a symmetry transformation of a p-adic quantum system may be defined as a map preserving this affine geometry. We argue that, as a consequence, the group of all symmetry transformations of a p-adic quantum system has a richer structure with respect to the case of standard quantum mechanics over the complex numbers.



中文翻译:

p 进希尔伯特空间上的量子力学:基础和前景

我们回顾了关于标量场量子理论数学基础的一些最新结果,标量场是非阿基米德场的二次扩展p-进数。在我们的方法中,我们受到这个想法的启发——首先在[IV Volovich,p-adic 字符串,类。量子重力 4 (1987) L83–L87]——在适当的小尺度以下,该空间不会表现为连续体,因此,应该建模为完全断开的可度量拓扑空间,由满足强三角不等式的度量来统治。我们构建的第一步是对 a 进行适当的定义p-adic 希尔伯特空间。接下来,在介绍了所有必要的数学工具之后——特别是线性算子中的各种类别p-adic Hilbert 空间——我们考虑物理状态的代数定义p- 超量子力学。相应的可观察量,其定义完成了理论的统计解释,被引入为 SOVM,p-与复数上的标准量子系统相关联的 POVM 的 adic 对应项。有趣的是,事实证明,标准量子系统状态空间的典型凸几何被替换了,p-adic 设置,具有仿射几何形状;因此,a 的对称变换p-adic量子系统可以被定义为保留这种仿射几何的映射。因此,我们认为,a 的所有对称变换组成的群p-相对于复数标准量子力学的情况,adic 量子系统具有更丰富的结构。

更新日期:2024-03-14
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