零点长度的热性和引力自对偶性

IF 2.1 3区 物理与天体物理 Q2 PHYSICS, MATHEMATICAL
P. Fernandez de Cordoba, J. M. Isidro, Rudranil Roy
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引用次数: 1

摘要

有人认为零点长度的存在是量子引力的标志。在本文中,我们提出了一种热机制,即这种长度量子在平坦的欧几里得时空中产生[公式:见文本]。为此,我们考虑所有平坦欧几里得时空的无限序列[公式:见文]和[公式:见文],并假设每个[公式:见文]发生的概率分布。所考虑的分布是一个正则系综在温度下的分布[公式:见文本],能级是一维谐振子的能级。由于谐振能级和时空维度都是均匀间隔的,我们可以用维度的特征值来识别谐振子的正则分布[公式:见文]。描述这个统计集合的状态在位置算子中有一个均方差,这可以解释为长度的量子。因此,将振荡器与浴槽置于热平衡状态提供了一种热机制,从而产生零点长度。然后讨论了这种结构的量子引力含义。特别地,我们提出了一个模型来实现弱引力强量子系统和弱量子强引力系统之间的猜想二象性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Thermality of the zero-point length and gravitational selfduality
It has been argued that the existence of a zero-point length is the hallmark of quantum gravity. In this paper, we suggest a thermal mechanism whereby this quantum of length arises in flat, Euclidean spacetime [Formula: see text]. For this, we consider the infinite sequence of all flat, Euclidean spacetimes [Formula: see text] with [Formula: see text], and postulate a probability distribution for each [Formula: see text] to occur. The distribution considered is that of a canonical ensemble at temperature [Formula: see text], the energy levels those of a 1-dimensional harmonic oscillator. Since both the harmonic energy levels and the spacetime dimensions are evenly spaced, one can identify the canonical distribution of harmonic-oscillator eigenvalues with that of dimensions [Formula: see text]. The state describing this statistical ensemble has a mean square deviation in the position operator, that can be interpreted as a quantum of length. Thus, placing an oscillator in thermal equilibrium with a bath provides a thermal mechanism whereby a zero-point length is generated. The quantum-gravitational implications of this construction are then discussed. In particular, a model is presented that realizes a conjectured duality between a weakly gravitational, strongly quantum system and a weakly quantum, strongly gravitational system.
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来源期刊
CiteScore
3.40
自引率
22.20%
发文量
274
审稿时长
6 months
期刊介绍: This journal publishes short communications, research and review articles devoted to all applications of geometric methods (including commutative and non-commutative Differential Geometry, Riemannian Geometry, Finsler Geometry, Complex Geometry, Lie Groups and Lie Algebras, Bundle Theory, Homology an Cohomology, Algebraic Geometry, Global Analysis, Category Theory, Operator Algebra and Topology) in all fields of Mathematical and Theoretical Physics, including in particular: Classical Mechanics (Lagrangian, Hamiltonian, Poisson formulations); Quantum Mechanics (also semi-classical approximations); Hamiltonian Systems of ODE''s and PDE''s and Integrability; Variational Structures of Physics and Conservation Laws; Thermodynamics of Systems and Continua (also Quantum Thermodynamics and Statistical Physics); General Relativity and other Geometric Theories of Gravitation; geometric models for Particle Physics; Supergravity and Supersymmetric Field Theories; Classical and Quantum Field Theory (also quantization over curved backgrounds); Gauge Theories; Topological Field Theories; Strings, Branes and Extended Objects Theory; Holography; Quantum Gravity, Loop Quantum Gravity and Quantum Cosmology; applications of Quantum Groups; Quantum Computation; Control Theory; Geometry of Chaos.
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