Principle of relative locality

We propose a deepening of the relativity principle according to which the invariant arena for nonquantum physics is a phase space rather than spacetime. Descriptions of particles propagating and interacting in spacetimes are constructed by observers, but different observers, separated from each other by translations, construct different spacetime projections from the invariant phase space. Nonetheless, all observers agree that interactions are local in the spacetime coordinates constructed by observers local to them. This framework, in which absolute locality is replaced by relative locality, results from deforming energy-momentum space, just as the passage from absolute to relative simultaneity results from deforming the linear addition of velocities. Different aspects of energy-momentum space geometry, such as its curvature, torsion and nonmetricity, are reflected in different kinds of deformations of the energy-momentum conservation laws. These are in principle all measurable by appropriate experiments. We also discuss a natural set of physical hypotheses which singles out the cases of energy-momentum space with a metric compatible connection and constant curvature.

[1]  Topological field theory and the quantum double of SU(2) , 1998, hep-th/9804130.

[2]  S. Majid,et al.  Twisting of Quantum Differentials and¶the Planck Scale Hopf Algebra , 1998, math/9811054.

[3]  Quantum symmetry, the cosmological constant and Planck scale phenomenology , 2003, hep-th/0306134.

[4]  Edward Witten,et al.  (2+1)-Dimensional Gravity as an Exactly Soluble System , 1988 .

[5]  S. Hossenfelder Bounds on an energy-dependent and observer-independent speed of light from violations of locality. , 2010, Physical review letters.

[6]  T. Piran,et al.  Modifications to Lorentz invariant dispersion in relatively boosted frames , 2010, 1004.0575.

[7]  L. H. Thomas The Motion of the Spinning Electron , 1926, Nature.

[8]  M. Arzano Anatomy of a deformed symmetry: field quantization on curved momentum space , 2010, 1009.1097.

[9]  J. Mitchell,et al.  Observations on helical dislocations in crystals of silver chloride , 1958 .

[10]  G. Amelino-Camelia Relativity in space-times with short distance structure governed by an observer independent (Planckian) length scale , 2000, gr-qc/0012051.

[11]  J. Lukierski,et al.  Q deformation of Poincare algebra , 1991 .

[12]  N. Mavromatos,et al.  Probing a possible vacuum refractive index with γ-ray telescopes☆ , 2009, 0901.4052.

[13]  G. A. Camelia Testable scenario for relativity with minimum - length , 2001 .

[14]  G. Amelino-Camelia,et al.  Taming nonlocality in theories with Planck-scale deformed Lorentz symmetry. , 2010, Physical review letters.

[15]  Eugene P. Wigner,et al.  80 Years of Professor Wigner's Seminal Work "On Unitary Representations of the Inhomogeneous Lorentz Group" , 2021 .

[16]  D. Minic,et al.  QUANTUM GRAVITY, DYNAMICAL ENERGY–MOMENTUM SPACE AND VACUUM ENERGY , 2010, 1004.4220.

[17]  Lee Smolin,et al.  Prospects for constraining quantum gravity dispersion with near term observations , 2009, 0906.3731.

[18]  E. Álvarez,et al.  Quantum Gravity , 2004, gr-qc/0405107.

[19]  Quantum group symmetry and particle scattering in (2+1)-dimensional quantum gravity , 2002, hep-th/0205021.

[20]  E. Livine,et al.  Effective 3d Quantum Gravity and Non-Commutative Quantum Field Theory , 2005 .

[21]  E. Livine,et al.  Ponzano–Regge model revisited: III. Feynman diagrams and effective field theory , 2005, hep-th/0502106.

[22]  Quantum Mechanics of a Point Particle in 2+1 Dimensional Gravity , 1997, gr-qc/9708054.

[23]  Carlo Rovelli Quantum gravity , 2008, Scholarpedia.

[24]  Poisson structure and symmetry in the Chern?Simons formulation of (2 + 1)-dimensional gravity , 2003, gr-qc/0301108.

[25]  Reinhard Haring Quantum Symmetry , 1993, hep-th/9307164.

[26]  H. Snyder,et al.  Quantized Space-Time , 1947 .

[27]  G. Amelino-Camelia DOUBLY-SPECIAL RELATIVITY: FIRST RESULTS AND KEY OPEN PROBLEMS , 2002, gr-qc/0210063.

[28]  L. H. Thomas The Kinematics of an electron with an axis , 1927 .

[29]  A. Ashtekar Lessons from (2+1)-dimensional quantum gravity , 1990 .

[30]  Generalized Lorentz invariance with an invariant energy scale , 2002, gr-qc/0207085.

[31]  M. Arzano,et al.  Kinematics of a relativistic particle with de Sitter momentum space , 2010, 1008.2962.

[32]  S. Matsuura,et al.  Momentum space metric, nonlocal operator, and topological insulators , 2010, 1007.2200.

[33]  S. Majid Meaning of Noncommutative Geometry and the Planck-Scale Quantum Group , 2000, hep-th/0006166.

[34]  Alain Connes,et al.  Noncommutative geometry , 1988 .

[35]  F. Girelli Snyder Space-Time: K-Loop and Lie Triple System ? , 2010, 1009.4762.

[36]  M. Kikkawa Geometry of homogeneous Lie loops , 1975 .

[37]  Group Field Theory: An Overview , 2005, hep-th/0505016.

[38]  A. Einstein Zur Elektrodynamik bewegter Körper , 1905 .

[39]  R. E. Hughes,et al.  A limit on the variation of the speed of light arising from quantum gravity effects , 2009, Nature.

[40]  Bicrossproduct structure of κ-Poincare group and non-commutative geometry , 1994, hep-th/9405107.

[41]  J. Kowalski-Glikman,et al.  Effective particle kinematics from Quantum Gravity , 2008, 0808.2613.