The special relativity principle and superluminal velocities

dc.authoridYarman, Tolga/0000-0003-3209-2264
dc.authorscopusid7004016669
dc.authorscopusid55893162300
dc.authorscopusid6602529732
dc.authorscopusid6602787345
dc.authorwosidYarman, Tolga/Q-9753-2019
dc.contributor.authorYarman, Nuh Tolga
dc.contributor.authorMissevitch, O. V.
dc.contributor.authorSmirnov-Rueda, R.
dc.contributor.authorYarman, T.
dc.contributor.otherEnerji Sistemleri Mühendisliği / Energy Systems Engineering
dc.date.accessioned2024-05-25T11:24:13Z
dc.date.available2024-05-25T11:24:13Z
dc.date.issued2012
dc.departmentOkan Universityen_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, Turkeyen_US
dc.descriptionYarman, Tolga/0000-0003-3209-2264en_US
dc.description.abstractIn 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.citation2
dc.identifier.doi10.4006/0836-1398-25.4.621
dc.identifier.endpage626en_US
dc.identifier.issn0836-1398
dc.identifier.issn2371-2236
dc.identifier.issue4en_US
dc.identifier.scopus2-s2.0-84874028592
dc.identifier.startpage621en_US
dc.identifier.urihttps://doi.org/10.4006/0836-1398-25.4.621
dc.identifier.urihttps://hdl.handle.net/20.500.14517/787
dc.identifier.volume25en_US
dc.identifier.wosWOS:000313924300018
dc.institutionauthorYarman, Nuh Tolga
dc.language.isoen
dc.publisherPhysics Essays Publicationen_US
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanıen_US
dc.rightsinfo:eu-repo/semantics/closedAccessen_US
dc.subjectSuperluminal Velocitiesen_US
dc.subjectBound Electromagnetic Fielden_US
dc.subjectSpecial Relativityen_US
dc.titleThe special relativity principle and superluminal velocitiesen_US
dc.typeArticleen_US
dspace.entity.typePublication
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relation.isAuthorOfPublication.latestForDiscoverye8750528-f58f-486e-9a0a-eb4ab45fb468
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