Recoupling Coefficients for the Group SU(3)
dc.contributor.author | Resnikoff, M. | en_US |
dc.date.accessioned | 2010-05-06T20:46:45Z | |
dc.date.available | 2010-05-06T20:46:45Z | |
dc.date.issued | 1967-01 | en_US |
dc.identifier.citation | Resnikoff, M. (1967). "Recoupling Coefficients for the Group SU(3)." Journal of Mathematical Physics 8(1): 79-83. <http://hdl.handle.net/2027.42/69553> | en_US |
dc.identifier.uri | https://hdl.handle.net/2027.42/69553 | |
dc.description.abstract | The Hilbert space method, employed in the previous article to obtain the coupling coefficients of SU(3), is used here to obtain the recoupling, or 6(λμ), coefficients of SU(3). The coefficients are formulated in terms of a generating function involving an integral, and an explicit expression is integrated out for the general nondegenerate case. The symmetries of the 6(λμ) coefficients are discussed. | en_US |
dc.format.extent | 3102 bytes | |
dc.format.extent | 273073 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 | Recoupling Coefficients for the Group SU(3) | 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 | Harrison M. Randall Laboratory of Physics, University of Michigan, Ann Arbor, Michigan | en_US |
dc.description.bitstreamurl | http://deepblue.lib.umich.edu/bitstream/2027.42/69553/2/JMAPAQ-8-1-79-1.pdf | |
dc.identifier.doi | 10.1063/1.1705104 | en_US |
dc.identifier.source | Journal of Mathematical Physics | en_US |
dc.identifier.citedreference | A form similar to this has been derived by J. J. de Swart, Nuovo Cimento 31, 420 (1964). Equation (1.1) is the recoupling coefficient multiplied by the factor (−1)k′+k13(N12N13)−1/2,(−1)k′+k13(N12N13)−1∕2, where N12N12 and N13N13 are the dimensions of the spaces Dλ12μ12, Dλ13μ13 (see Ref. 3 below). | en_US |
dc.identifier.citedreference | J. J. de Swart, Rev. Mod. Phys. 35, 916 (1963). | en_US |
dc.identifier.citedreference | M. Resnikoff, preceding paper, J. Math. Phys. 8, 63 (1967). This article is hereafter referred to as (I). | en_US |
dc.identifier.citedreference | J. R. Derome and W. T. Sharp, J. Math. Phys. 6, 1584 (1965), have discussed symmetries for the 6‐j symbols of a general group. In contrast to their paper, the phase and the method of labeling degenerate states is specified here, and this leads to simpler relations. de Swart (Ref. 1) obtains symmetry relations for octet recouplings. | en_US |
dc.identifier.citedreference | V. Bargmann, Rev. Mod. Phys. 34, 829 (1962). | en_US |
dc.identifier.citedreference | The general functional dependence is given by Eqs. (3.33), (3.34), and (3.35) of (I). | en_US |
dc.identifier.citedreference | The measure dμn(ζ)dμn(ζ) is defined in Eq. (1.1b) of (I), or see Bargmann (Ref. 5). | en_US |
dc.identifier.citedreference | K. T. Hecht, Nucl. Phys. 62, 1 (1965). | en_US |
dc.identifier.citedreference | K. T. Hecht, Selected Topics in Nuclear Spectroscopy (North‐Holland Publishing Company, Amsterdam, 1964). | en_US |
dc.owningcollname | Physics, Department of |
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