Polyakov's spin factor for a classical spinning particle via the BRST invariant path integral

Jin Ho Cho, Seungjoon Hyun, Hyuk jae Lee

Research output: Contribution to journalArticle

1 Citation (Scopus)

Abstract

For the 'classical' formulation of a massive spinning particle, the propagator is obtained along with the spin factor. We treat the system with two kinds of constraints that were recently shown to be concerned with the reparametrization invariance and 'quasi-supersymmetry'. In the path integral, the BRST invariant Lagrangian is used and the same spin factor is obtained as in the pseudo-classical formulation.

Original languageEnglish
Pages (from-to)274-278
Number of pages5
JournalPhysics Letters B
Volume327
Issue number3-4
DOIs
Publication statusPublished - 1994 May 19

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metal spinning
formulations
supersymmetry
invariance
propagation

All Science Journal Classification (ASJC) codes

  • Nuclear and High Energy Physics

Cite this

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abstract = "For the 'classical' formulation of a massive spinning particle, the propagator is obtained along with the spin factor. We treat the system with two kinds of constraints that were recently shown to be concerned with the reparametrization invariance and 'quasi-supersymmetry'. In the path integral, the BRST invariant Lagrangian is used and the same spin factor is obtained as in the pseudo-classical formulation.",
author = "Cho, {Jin Ho} and Seungjoon Hyun and Lee, {Hyuk jae}",
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Polyakov's spin factor for a classical spinning particle via the BRST invariant path integral. / Cho, Jin Ho; Hyun, Seungjoon; Lee, Hyuk jae.

In: Physics Letters B, Vol. 327, No. 3-4, 19.05.1994, p. 274-278.

Research output: Contribution to journalArticle

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AU - Hyun, Seungjoon

AU - Lee, Hyuk jae

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N2 - For the 'classical' formulation of a massive spinning particle, the propagator is obtained along with the spin factor. We treat the system with two kinds of constraints that were recently shown to be concerned with the reparametrization invariance and 'quasi-supersymmetry'. In the path integral, the BRST invariant Lagrangian is used and the same spin factor is obtained as in the pseudo-classical formulation.

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