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dc.contributor.authorYarman, T.
dc.contributor.authorYarman, Ozan Uğraş
dc.contributor.authorArik, M.
dc.contributor.authorKholmetskii, A. L.
dc.date.accessioned2021-12-10T10:18:23Z
dc.date.available2021-12-10T10:18:23Z
dc.identifier.citationKholmetskii A. L. , Yarman T., Yarman O. U. , Arik M., "Doppler effect in rotating systems and Mossbauer rotor experiments", ANNALS OF PHYSICS, cilt.432, 2021
dc.identifier.issn0003-4916
dc.identifier.othervv_1032021
dc.identifier.otherav_37a00609-1061-4673-a729-240c6308dc97
dc.identifier.urihttp://hdl.handle.net/20.500.12627/169628
dc.identifier.urihttps://doi.org/10.1016/j.aop.2021.168568
dc.description.abstractWe address once more the problem of the physical interpretation of the Mossbauer effect in a rotating system in the view of the recently discovered extra energy shift (EES) between emitted and absorbed resonant radiation, which emerges in addition to the usual second order Doppler shift for an orbiting absorber. We highlight that both fractional components of the total energy shift have the same sign and correspond to the blueshift of the resonant radiation propagating from the rotational axis to the rotor rim. We indicate a possible way of understanding the origin of the EES in terms of combining metric effects in rotating systems with the quantum mechanical description of resonant nuclei confined in crystal cells by taking into account the recoil-free essence of the Mossbauer effect, where no energy is transmitted to the source (absorber) during the emission (absorption) of resonant radiation. (C) 2021 Elsevier Inc. All rights reserved.
dc.language.isoeng
dc.subjectTemel Bilimler (SCI)
dc.subjectTemel Bilimler
dc.subjectDisiplinlerarası Fizik ve İlgili Bilim ve Teknoloji Alanları
dc.subjectFizik
dc.subjectFİZİK, MULTİDİSİPLİNER
dc.titleDoppler effect in rotating systems and Mossbauer rotor experiments
dc.typeMakale
dc.relation.journalANNALS OF PHYSICS
dc.contributor.departmentBelarusian State University , ,
dc.identifier.volume432
dc.contributor.firstauthorID2725232


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