Abstract:We construct a Dirac equation that is consistent with one of the recently-proposed schemes for a "doubly-special relativity", a relativity with both an observer-independent velocity scale (still naturally identified with the speed-of-light constant) and an observer-independent length/momentum scale (possibly given by the Planck length/momentum). We find that the introduction of the second observer-independent scale only induces a mild deformation of the structure of Dirac spinors. We also show that our modifie… Show more
“…by Agostini, Amelino-Camelia, and Arzano in [39] but my interpretation differs dramatically. In what follows, I also incorporate an important phase factor, not appreciated in [39].…”
Section: A MIX Of Deformations In Algebra and Transformation Parameterscontrasting
confidence: 57%
“…In what follows, I also incorporate an important phase factor, not appreciated in [39]. The neglect of that phase amounts to projecting out antiparticles from NSR-2s as I have already noted in [42].…”
Section: A MIX Of Deformations In Algebra and Transformation Parametersmentioning
confidence: 99%
“…For this reason, the O(ℓ P ) departures given in [39] are artifacts of the used variables. The same holds true for the O(ℓ P ) corrections at the level of vector potential given in [40].…”
Section: Judes-visser Variables: Challenging Some Of the Nsr-2's Claimsmentioning
Abstract.I briefly argue for logical necessity to incorporate, besides c,h, two fundamental length scales in the symmetries associated with the interface of gravitational and quantum realms. Next, in order to clear the proverbial bush, I discuss the CPT and indistinguishability issue related to recent non-linear deformations of special relativity and suggest why algebraically well-defined extensions of special relativity do not require non-linear deformations. That done, I suggest why the stable Snyder-Yang-Mendes Lie algebra should be considered as a serious candidate for the symmetries underlying freely falling frames at the interface of gravitational and quantum realms; thus echoing, and complementing, arguments recently put forward by Chryssomalakos and Okon. In the process I obtain concrete form of uncertainty relations which involve above-indicated length scales and a new dimensionless constant. I draw attention to the fact that because superconducting quantum interference devices can carry roughly 10 23 Cooper pairs in a single quantum state, Planck-mass quantum systems already exist in the laboratory. These may be used for possible exploration of the interface of the gravitational and quantum realms.
“…by Agostini, Amelino-Camelia, and Arzano in [39] but my interpretation differs dramatically. In what follows, I also incorporate an important phase factor, not appreciated in [39].…”
Section: A MIX Of Deformations In Algebra and Transformation Parameterscontrasting
confidence: 57%
“…In what follows, I also incorporate an important phase factor, not appreciated in [39]. The neglect of that phase amounts to projecting out antiparticles from NSR-2s as I have already noted in [42].…”
Section: A MIX Of Deformations In Algebra and Transformation Parametersmentioning
confidence: 99%
“…For this reason, the O(ℓ P ) departures given in [39] are artifacts of the used variables. The same holds true for the O(ℓ P ) corrections at the level of vector potential given in [40].…”
Section: Judes-visser Variables: Challenging Some Of the Nsr-2's Claimsmentioning
Abstract.I briefly argue for logical necessity to incorporate, besides c,h, two fundamental length scales in the symmetries associated with the interface of gravitational and quantum realms. Next, in order to clear the proverbial bush, I discuss the CPT and indistinguishability issue related to recent non-linear deformations of special relativity and suggest why algebraically well-defined extensions of special relativity do not require non-linear deformations. That done, I suggest why the stable Snyder-Yang-Mendes Lie algebra should be considered as a serious candidate for the symmetries underlying freely falling frames at the interface of gravitational and quantum realms; thus echoing, and complementing, arguments recently put forward by Chryssomalakos and Okon. In the process I obtain concrete form of uncertainty relations which involve above-indicated length scales and a new dimensionless constant. I draw attention to the fact that because superconducting quantum interference devices can carry roughly 10 23 Cooper pairs in a single quantum state, Planck-mass quantum systems already exist in the laboratory. These may be used for possible exploration of the interface of the gravitational and quantum realms.
“…Furthermore the NC quantum theories are qualitatively different with an inherent nonlocality that obviously can not be captured in the canonical set up which, however, provides a very convenient framework to construct the quantum theory. An explicit example is given [177] where we construct the DSR generalization of Dirac fermions in a very simple way as compared to the original derivation [178].…”
In this review article we discuss some of the applications of noncommutative
geometry in physics that are of recent interest, such as noncommutative
many-body systems, noncommutative extension of Special Theory of Relativity
kinematics, twisted gauge theories and noncommutative gravity.Comment: New references added, Published online in Foundations of Physic
“…For example in the description of fields in κ-Minkowski one must of course introduce a differential calculus, for which various alternatives have been proposed in the κ-Minkowski literature. In particular there has been interest in a four-dimensional [22] and in a fivedimensional [23] differential calculus, and both of these differential calculi deserve equal consideration at the mathematics level, but if one insists on compatibility with the DSR principles only the five-dimensional differential calculus turns out [24] to be acceptable.…”
Section: Hopf-algebra Description Of Poincaré Symmetries Not Sufficiementioning
The idea of a role for DSR (doubly-special relativity) in quantum gravity finds some encouragement in a few scenarios, but in order to explore some key conceptual issues it is necessary to find a well-understood toy-quantum-gravity model that is fully compatible with the DSR principles. Perhaps the most significant source of encouragement comes from the recent proposal of a path for the emergence of DSR in Loop Quantum Gravity, which however relies on a few assumptions on the results of some computations that we are still unable to perform. Indications in favor of the possibility of using some elements of κ-Poincaré Hopf algebras (and of the related κ-Minkowski noncommutative spacetime) for the construction of a DSR theory have been discussed extensively, but a few stubborn open issues must still be resolved, especially in the two-particle sector. It has been recently observed that certain structures encountered in a formulation of 2+1-dimensional classical-gravity models would fit naturally in a DSR framework, but some key elements of these 2+1-dimensional models, including the description of observers, might be incompatible with the DSR principles.
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