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Volumn 56, Issue 2, 1997, Pages 689-701

[Formula Presented]-[Formula Presented] problem: Connectedness, transition amplitudes, and quasiparticle approximation

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EID: 0031497663     PISSN: 05562813     EISSN: 1089490X     Source Type: Journal    
DOI: 10.1103/PhysRevC.56.689     Document Type: Article
Times cited : (5)

References (31)
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    • L. D. Faddeev, Mathematical Aspects of the Three-Body Problem in the Quantum Scattering Theory (Israel Program for Scientific Translations, Jerusalem, 1965).
    • Faddeev, L.D.1
  • 23
    • 85035269371 scopus 로고    scopus 로고
    • To be rigorous, one ought to introduce integrations over the momenta of the spectator particles in Eq. (2.2). Since these integrations are removed when considering the momentum-space matrix elements of the relevant transition operators, to save on notation here and in the following we shall leave such integrations implicit
    • To be rigorous, one ought to introduce integrations over the momenta of the spectator particles in Eq. (2.2). Since these integrations are removed when considering the momentum-space matrix elements of the relevant transition operators, to save on notation here and in the following we shall leave such integrations implicit.
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    • Phys. Rev. 150, 1321 (1966)
    • (1966) Phys. Rev. , vol.150 , pp. 1321
  • 27
    • 85035297014 scopus 로고    scopus 로고
    • Strictly speaking, because of the identity of the nucleons, one has a unique transition amplitude for the process (Formula presented). As usual in scattering theory, for the moment we assume the nucleons as distinguishable, so that the configurations (Formula presented) and (Formula presented) are regarded as different from each other. The prescriptions due to particle identity can be taken into account at the end, through suitable linear combinations of the transition amplitudes. However, to save on notation, we shall simply write (Formula presented) in place of (Formula presented) in the transition amplitudes
    • Strictly speaking, because of the identity of the nucleons, one has a unique transition amplitude for the process (Formula presented). As usual in scattering theory, for the moment we assume the nucleons as distinguishable, so that the configurations (Formula presented) and (Formula presented) are regarded as different from each other. The prescriptions due to particle identity can be taken into account at the end, through suitable linear combinations of the transition amplitudes. However, to save on notation, we shall simply write (Formula presented) in place of (Formula presented) in the transition amplitudes.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.