Special Relativity and Quantum Theory 1988
DOI: 10.1007/978-94-009-3051-3_19
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Covariant Harmonic Oscillators and the Quark Model

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Cited by 9 publications
(19 citation statements)
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“…What is new in this paper? In our first paper on this subject [44], we started with a Lorentz-covariant Gaussian form proposed by Yukawa's in his 1953 paper [8], and its applications to high-energy physics [45,46,47,48,49]. We were particularly interested in how the Gaussian form becomes deformed under Lorentz boosts.…”
Section: Discussionmentioning
confidence: 99%
“…What is new in this paper? In our first paper on this subject [44], we started with a Lorentz-covariant Gaussian form proposed by Yukawa's in his 1953 paper [8], and its applications to high-energy physics [45,46,47,48,49]. We were particularly interested in how the Gaussian form becomes deformed under Lorentz boosts.…”
Section: Discussionmentioning
confidence: 99%
“…The series of the form of Eq. (1) was developed earlier for studying harmonic oscillators in moving frames [24,20,25,26,27,28]. Here z and t are the space-like and time-like separations between the two constituent particles bound together by a harmonic oscillator potential.…”
Section: Space-time Entanglementmentioning
confidence: 99%
“…where the x and y variables are replaced by z and t respectively. If Lorentz-boosted, this Gaussian function becomes squeezed to [24,20,25]…”
Section: Space-time Entanglementmentioning
confidence: 99%
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“…The relativistic harmonic oscillator appeared in the first works of Born on reciprocity [2,3] and in the context of the study of relativistic bound states [4,5] (see [6,7] for recent analysis and more references). In our context is that the coordinate x subject to the harmonic oscillator potential is not a relative position between two constituents, but the actual coordinate of the particle.…”
Section: Introductionmentioning
confidence: 99%