Wigner and Racah coefficients for SU3
dc.contributor.author | Draayer, J. P. | en_US |
dc.contributor.author | Akiyama, Yoshimi | en_US |
dc.date.accessioned | 2010-05-06T21:42:44Z | |
dc.date.available | 2010-05-06T21:42:44Z | |
dc.date.issued | 1973-12 | en_US |
dc.identifier.citation | Draayer, J. P.; Akiyama, Yoshimi (1973). "Wigner and Racah coefficients for SU3." Journal of Mathematical Physics 14(12): 1904-1912. <http://hdl.handle.net/2027.42/70151> | en_US |
dc.identifier.uri | https://hdl.handle.net/2027.42/70151 | |
dc.description.abstract | A general yet simple and hence practical algorithm for calculating SU3⊃SU2×U1SU3⊃SU2×U1 Wigner coefficients is formulated. The resolution of the outer multiplicity follows the prescription given by Biedenharn and Louck. It is shown that SU3 Racah coefficients can be obtained as a solution to a set of simultaneous equations with unknown coefficients given as a by‐product of the initial steps in the SU3⊃SU2×U1SU3⊃SU2×U1 Wigner coefficient construction algorithm. A general expression for evaluating SU3⊃R3SU3⊃R3 Wigner coefficients as a sum over a simple subset of the corresponding SU3⊃SU2×U1SU3⊃SU2×U1 Wigner coefficients is also presented. State conjugation properties are discussed and symmetry relations for both the SU3⊃SU2×U1SU3⊃SU2×U1 and SU3⊃R3SU3⊃R3 Wigner coefficients are given. Machine codes based on the results are available. | en_US |
dc.format.extent | 3102 bytes | |
dc.format.extent | 793267 bytes | |
dc.format.mimetype | text/plain | |
dc.format.mimetype | application/pdf | |
dc.publisher | The American Institute of Physics | en_US |
dc.rights | © The American Institute of Physics | en_US |
dc.title | Wigner and Racah coefficients for SU3 | en_US |
dc.type | Article | en_US |
dc.subject.hlbsecondlevel | Physics | en_US |
dc.subject.hlbtoplevel | Science | en_US |
dc.description.peerreviewed | Peer Reviewed | en_US |
dc.contributor.affiliationum | Department of Physics, The University of Michigan, Ann Arbor, Michigan 48105 | en_US |
dc.description.bitstreamurl | http://deepblue.lib.umich.edu/bitstream/2027.42/70151/2/JMAPAQ-14-12-1904-1.pdf | |
dc.identifier.doi | 10.1063/1.1666267 | en_US |
dc.identifier.source | Journal of Mathematical Physics | en_US |
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dc.identifier.citedreference | For a coupled system (λ1μ1)×(λ2μ2)→(λ3μ3),(λ1μ1)×(λ2μ2)→(λ3μ3), Eq. (32) cannot simultaneously be applied to all three representations (λ1μ1),(λ2μ2),(λ1μ1),(λ2μ2), and (λ3μ3),(λ3μ3), in a consistent fashion. An additional dependence upon the multiplicity label is required. See, for example, J. J. deSwart, Rev. Mod. Phys. 35, 916 (1963), Sec. 14 and Sec. 4B of the current article. | en_US |
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dc.identifier.citedreference | J. P. Draayer and Yoshimi Akiyama, Comput. Phys. Commun. 5, 405 (1973). | en_US |
dc.owningcollname | Physics, Department of |
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