The special relativity principle and superluminal velocities

dc.authorid Yarman, Tolga/0000-0003-3209-2264
dc.authorscopusid 7004016669
dc.authorscopusid 55893162300
dc.authorscopusid 6602529732
dc.authorscopusid 6602787345
dc.authorwosid Yarman, Tolga/Q-9753-2019
dc.contributor.author Kholmetskii, A. L.
dc.contributor.author Missevitch, O. V.
dc.contributor.author Smirnov-Rueda, R.
dc.contributor.author Yarman, T.
dc.date.accessioned 2024-05-25T11:24:13Z
dc.date.available 2024-05-25T11:24:13Z
dc.date.issued 2012
dc.department Okan University en_US
dc.department-temp [Kholmetskii, A. L.; Missevitch, O. V.] Belarusian State Univ, Inst Nucl Problems, Minsk 220030, BELARUS; [Smirnov-Rueda, R.] Univ Complutense, Fac Math, E-28040 Madrid, Spain; [Yarman, T.] Okan Univ, Istanbul, Turkey; [Yarman, T.] Savronik, Eskisehir, Turkey en_US
dc.description Yarman, Tolga/0000-0003-3209-2264 en_US
dc.description.abstract In view of numerous experimental results reported in the past decades on the observation of faster-than-light electromagnetic signals, we analyze the structure of relativistic kinematics, where such superluminal signals are allowed. As the first step, we suggest replacing the Einstein postulates with the general relativity principle (the possibility of describing any phenomenon in any frame of reference achievable in nature) applied to an inertial motion in an empty space. Then, as in common relativistic kinematics, we also arrive at the Lorentz transformations between inertial reference frames, where a superluminal motion of massless entities is not prohibited (in particular, for perturbations of bound electromagnetic field). However, for any objects with a finite rest mass, the limited velocity remains always less than the light velocity c, and in such a way we avoid the tachyonic-type theories in their common meaning. We show that the application of superluminal electromagnetic signals to synchronization of distant clocks yields the common expressions for the relativity of the simultaneity of events for different inertial observers. This result confirms the validity of the Lorentz transformations in generalized relativistic kinematics, though along with superluminal signals. Hence we arrive at the invariance of the space-time interval, as in common relativistic kinematics, where, however, the superluminal motion of massless entities is allowed. Even so, no further changes emerge in relativistic dynamics and other common relativistic implications. Finally, we consider causal paradoxes related to the propagation and exchange of superluminal signals between inertial observers and provide their resolution. (C) 2012 Physics Essays Publication. [DOI: 10.4006/0836-1398-25.4.621] en_US
dc.identifier.citationcount 2
dc.identifier.doi 10.4006/0836-1398-25.4.621
dc.identifier.endpage 626 en_US
dc.identifier.issn 0836-1398
dc.identifier.issn 2371-2236
dc.identifier.issue 4 en_US
dc.identifier.scopus 2-s2.0-84874028592
dc.identifier.startpage 621 en_US
dc.identifier.uri https://doi.org/10.4006/0836-1398-25.4.621
dc.identifier.uri https://hdl.handle.net/20.500.14517/787
dc.identifier.volume 25 en_US
dc.identifier.wos WOS:000313924300018
dc.institutionauthor Yarman, Nuh Tolga
dc.language.iso en
dc.publisher Physics Essays Publication en_US
dc.relation.publicationcategory Makale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı en_US
dc.rights info:eu-repo/semantics/closedAccess en_US
dc.scopus.citedbyCount 3
dc.subject Superluminal Velocities en_US
dc.subject Bound Electromagnetic Field en_US
dc.subject Special Relativity en_US
dc.title The special relativity principle and superluminal velocities en_US
dc.type Article en_US
dc.wos.citedbyCount 2

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