The Mass Gap of the Space-time and its Shape

Check out our latest exploration into Snyder’s quantum space-time! We dive into how quanta of space-time have a positive mass, explore the intriguing 24-cell geometry, and discuss its potential links to the standard model of particles. Plus, we connect these findings to major concepts like mass generation and the flatness of the observable universe.

TL;DR
We’re investigating Snyder’s quantum space-time, focusing on its Lorentz invariance and the intriguing positive mass gap. The study highlights the 24-cell geometry, its symmetry group, and potential connections to the standard model of particles. This research touches on mass generation, Avogadro’s number, and the observable universe’s flatness.


This content originally appeared on HackerNoon and was authored by Phenomenology

:::info Author:

(1) Ahmed Farag Ali, Essex County College and Department of Physics, Faculty of Science, Benha University.

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Abstract and Introduction

Space-time quanta and Becken Universal bound

Shape of space-time quanta

Symmetry of space-time quanta

Space-time quanta and Spectral mass gap

Phenomenological implications

Conclusion, Acknowledgments, and References

Abstract

Snyder’s quantum space-time which is Lorentz invariant is investigated. It is found that the quanta of space-time have a positive mass that is interpreted as a positive real mass gap of space-time. This mass gap is related to the minimal length of measurement which is provided by Snyder’s algebra. Several reasons to consider the space-time quanta as a 24-cell are discussed. Geometric reasons include its self-duality property and its 24 vertices that may represent the standard model of elementary particles. The 24-cell symmetry group is the Weyl/Coxeter group of the F4 group which was found recently to generate the gauge group of the standard model. It is found that 24-cell may provide a geometric interpretation of the mass generation, Avogadro number, color confinement, and the flatness of the observable universe. The phenomenology and consistency with measurements is discussed.

\ “The knowledge at which geometry aims is knowledge of the eternal”— Plato.

I. INTRODUCTION

In 1947, Snyder established a remarkable step that reconciles the minimal length of measurement with Lorentz symmetry by constructing quantum Lorentzian space-time [1]. The price was introducing non-commutative geometry and the generalized uncertainty principle (GUP) in Snyder’s algebra. For Non-commutative geometry part, it is found to emerge naturally at limits of M/string theory [2] as higher dimensional corrections of ordinary Yang-Mills theory [3]. Several implications of non-commutative geometry were investigated in quantum field theory and condensed matter systems [4, 5]. For the GUP part, it emerged in several approaches to quantum gravity such as string theory, loop quantum gravity, and quantum geometry [6–12]. Phenomenological and experimental implications of the GUP have been investigated in low and high-energy systems [13–25]. Useful reviews on quantum space-time and GUP can be found in [26–28]. Snyder’s algebra is generated by three main generators which are position xµ, momentum pµ and Lorentz generators Jµν = xµpν − xνpµ. They satisfy the Poincar´e commutation relations and suggest new commutation relations that provide a quantum/minimal length as follows:

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\ where ℓP l is a Planck length, κ is a dimensionless parameter that identifies the minimal measurable length, and ηµν = (−1, 1, 1, 1). Eq. (1) introduces the non-commutative geometry and Eq. (2) introduces a GUP. Both equations are invariant under Lorentz symmetry [1].

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:::info This paper is available on arxiv under CC BY 4.0 DEED license.

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This content originally appeared on HackerNoon and was authored by Phenomenology


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