Abstract:Ever since the work of von Ignatowsky circa 1910 it has been known (if not
always widely appreciated) that the relativity principle, combined with the
basic and fundamental physical assumptions of locality, linearity, and
isotropy, leads almost uniquely to either the Lorentz transformations of
special relativity or to Galileo's transformations of classical Newtonian
mechanics. Thus, if one wishes to entertain the possibility of Lorentz symmetry
breaking within the context of the class of local physical theorie… Show more
“…This line element also was found in [11]. Some works about Lorentz violation can be seen in [12,13,14,15,16,44,18,19,20,21,22,23,24,25,26,27,28] and works about VSR can be found in [29,30,31,32,33,34,35,36].…”
The action for a (3+1)-dimensional particle in very special relativity is studied. It is proved that massless particles only travel in effective (2 + 1)-dimensional space-time. It is remarkable that this action can be written as an action for a relativistic particle in a background gauge field and it is shown that this field causes the dimensional reduction. A new symmetry for this system is found. Furthermore, a general action with restored Lorentz symmetry is proposed for this system. It is shown that this new action contains very special relativity and two-time physics.
“…This line element also was found in [11]. Some works about Lorentz violation can be seen in [12,13,14,15,16,44,18,19,20,21,22,23,24,25,26,27,28] and works about VSR can be found in [29,30,31,32,33,34,35,36].…”
The action for a (3+1)-dimensional particle in very special relativity is studied. It is proved that massless particles only travel in effective (2 + 1)-dimensional space-time. It is remarkable that this action can be written as an action for a relativistic particle in a background gauge field and it is shown that this field causes the dimensional reduction. A new symmetry for this system is found. Furthermore, a general action with restored Lorentz symmetry is proposed for this system. It is shown that this new action contains very special relativity and two-time physics.
“…Berzi and Gorini (1969) consider that taking the transformation functions to be real and continuous is a mathematical assumption. Baccetti, Tate, and Visser (2012) consider the description of space and time using real numbers as an assumption. Levy-Leblond (1976) also calls the attention to a causality assumption related to the notion of flow of time, differentiating clearly time from space.…”
In Einstein's physical geometry, the geometry of space and the uniformity of time are taken to be non-conventional. However, due to the stipulation of the isotropy of the one-way speed of light in the synchronization of clocks (or definition of simultaneity), as it stands, Einstein's views do not seem to apply to the whole of the Minkowski spacetime. In this work we will see how Einstein's views can be applied to the Minkowski space-time. In this way, when adopting Einstein's views, chronogeometry is a physical chronogeometry.
“…The first was by Ignatowsky [1] in 1910. Many other derivations followed; see [2] for a full list of references. Nevertheless, the approach here, based on symmetry, is new.…”
We explore the role of symmetry in the theory of Special Relativity. Using the symmetry of the principle of relativity and eliminating the Galilean transformations, we obtain a universally preserved speed and an invariant metric, without assuming the constancy of the speed of light. We also obtain the spacetime transformations between inertial frames depending on this speed. From experimental evidence, this universally preserved speed is c, the speed of light, and the transformations are the usual Lorentz transformations. The ball of relativistically admissible velocities is a bounded symmetric domain with respect to the group of affine automorphisms. The generators of velocity addition lead to a relativistic dynamics equation. To obtain explicit solutions for the important case of the motion of a charged particle in constant, uniform, and perpendicular electric and magnetic fields, one can take advantage of an additional symmetry—the symmetric velocities. The corresponding bounded domain is symmetric with respect to the conformal maps. This leads to explicit analytic solutions for the motion of the charged particle.
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