FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2022148931> ?p ?o ?g. }

• W2022148931 endingPage "3031" @default.
• W2022148931 startingPage "3020" @default.
• W2022148931 abstract "The model of the quantum relativistic rotator is defined by three correspondences: (1) the correspondence to a classical relativistic rotator when the quantum description goes over into the classical description (classical limit), (2) the correspondence to an elementary particle when the structure is ignored (elementary limit), and (3) the correspondence to a nonrelativistic quantum rotator (a rigid rotating string) in the nonrelativistic limit. The dynamics is given by a Hamiltonian which is obtained from a constraint relation that leads to a phenomenologically acceptable mass-spin trajectory relation. From the equation of motion it follows that the expectation value of the particle position spirals with approximately the velocity of light about the direction of the momentum, which is also the direction in which the center of mass propagates. The radius of this helical motion (i.e., the size of the rotator), as obtained from the phenomenological mass spectrum, is of the order of ${10}^{ensuremath{-}13}$ cm." @default.
• W2022148931 created "2016-06-24" @default.
• W2022148931 creator A5001739378 @default.
• W2022148931 creator A5014154161 @default.
• W2022148931 creator A5014433969 @default.
• W2022148931 creator A5039391552 @default.
• W2022148931 creator A5043520159 @default.
• W2022148931 creator A5056807494 @default.
• W2022148931 creator A5073464088 @default.
• W2022148931 creator A5078528770 @default.
• W2022148931 date "1983-12-15" @default.
• W2022148931 modified "2023-10-18" @default.
• W2022148931 title "Relativistic rotator. I. Quantum observables and constrained Hamiltonian mechanics" @default.
• W2022148931 cites W130762564 @default.
• W2022148931 cites W1601914152 @default.
• W2022148931 cites W1978135745 @default.
• W2022148931 cites W1978652497 @default.
• W2022148931 cites W1982511538 @default.
• W2022148931 cites W1985069850 @default.
• W2022148931 cites W1989349842 @default.
• W2022148931 cites W1993396933 @default.
• W2022148931 cites W1999224695 @default.
• W2022148931 cites W1999252655 @default.
• W2022148931 cites W2006983364 @default.
• W2022148931 cites W2012128119 @default.
• W2022148931 cites W2018915773 @default.
• W2022148931 cites W2021999674 @default.
• W2022148931 cites W2025012879 @default.
• W2022148931 cites W2025547642 @default.
• W2022148931 cites W2031882508 @default.
• W2022148931 cites W2042771312 @default.
• W2022148931 cites W2043940719 @default.
• W2022148931 cites W2045897146 @default.
• W2022148931 cites W2054664936 @default.
• W2022148931 cites W2056571964 @default.
• W2022148931 cites W2061347075 @default.
• W2022148931 cites W2083155641 @default.
• W2022148931 cites W2090903290 @default.
• W2022148931 cites W2095168843 @default.
• W2022148931 cites W2121348811 @default.
• W2022148931 cites W2162345253 @default.
• W2022148931 cites W2225001832 @default.
• W2022148931 cites W4238182962 @default.
• W2022148931 cites W4245613536 @default.
• W2022148931 doi "https://doi.org/10.1103/physrevd.28.3020" @default.
• W2022148931 hasPublicationYear "1983" @default.
• W2022148931 type Work @default.
• W2022148931 sameAs 2022148931 @default.
• W2022148931 citedByCount "33" @default.
• W2022148931 countsByYear W20221489312013 @default.
• W2022148931 countsByYear W20221489312019 @default.
• W2022148931 crossrefType "journal-article" @default.
• W2022148931 hasAuthorship W2022148931A5001739378 @default.
• W2022148931 hasAuthorship W2022148931A5014154161 @default.
• W2022148931 hasAuthorship W2022148931A5014433969 @default.
• W2022148931 hasAuthorship W2022148931A5039391552 @default.
• W2022148931 hasAuthorship W2022148931A5043520159 @default.
• W2022148931 hasAuthorship W2022148931A5056807494 @default.
• W2022148931 hasAuthorship W2022148931A5073464088 @default.
• W2022148931 hasAuthorship W2022148931A5078528770 @default.
• W2022148931 hasConcept C121332964 @default.
• W2022148931 hasConcept C126255220 @default.
• W2022148931 hasConcept C130787639 @default.
• W2022148931 hasConcept C14037181 @default.
• W2022148931 hasConcept C149324446 @default.
• W2022148931 hasConcept C15184713 @default.
• W2022148931 hasConcept C154761356 @default.
• W2022148931 hasConcept C162324750 @default.
• W2022148931 hasConcept C206611041 @default.
• W2022148931 hasConcept C2779577033 @default.
• W2022148931 hasConcept C33923547 @default.
• W2022148931 hasConcept C34447519 @default.
• W2022148931 hasConcept C36185635 @default.
• W2022148931 hasConcept C47513753 @default.
• W2022148931 hasConcept C53702628 @default.
• W2022148931 hasConcept C57476683 @default.
• W2022148931 hasConcept C62520636 @default.
• W2022148931 hasConcept C74650414 @default.
• W2022148931 hasConcept C84114770 @default.
• W2022148931 hasConceptScore W2022148931C121332964 @default.
• W2022148931 hasConceptScore W2022148931C126255220 @default.
• W2022148931 hasConceptScore W2022148931C130787639 @default.
• W2022148931 hasConceptScore W2022148931C14037181 @default.
• W2022148931 hasConceptScore W2022148931C149324446 @default.
• W2022148931 hasConceptScore W2022148931C15184713 @default.
• W2022148931 hasConceptScore W2022148931C154761356 @default.
• W2022148931 hasConceptScore W2022148931C162324750 @default.
• W2022148931 hasConceptScore W2022148931C206611041 @default.
• W2022148931 hasConceptScore W2022148931C2779577033 @default.
• W2022148931 hasConceptScore W2022148931C33923547 @default.
• W2022148931 hasConceptScore W2022148931C34447519 @default.
• W2022148931 hasConceptScore W2022148931C36185635 @default.
• W2022148931 hasConceptScore W2022148931C47513753 @default.
• W2022148931 hasConceptScore W2022148931C53702628 @default.
• W2022148931 hasConceptScore W2022148931C57476683 @default.
• W2022148931 hasConceptScore W2022148931C62520636 @default.
• W2022148931 hasConceptScore W2022148931C74650414 @default.
• W2022148931 hasConceptScore W2022148931C84114770 @default.

• next