Fetching the paper…
Reading the bibliography…
We report on a calculation of higher electromagnetic multipole moments of baryons in a non-covariant quark model approach.
E.M. Henley and W. Thirring, Elementary Quantum Field Theory
1962
Earlier work this paper cites.
F. Gürsey and L.A. Radicati, Phys. Rev. Lett. 13
1964
Earlier work this paper cites.
T.W. Donnelly, I. Sick, Rev. Mod. Phys. 56
1984
Earlier work this paper cites.
G. Morpurgo, Phys. Rev. D 40
1989
Earlier work this paper cites.
M.N. Butler, M.J. Savage, R.P. Springer, Phys. Rev. D 49
1995
Earlier work this paper cites.
A.J. Buchmann, E. Hernández, A. Faessler, Phys. Rev. C 55
1997
Cited alongside, same era.
G. Dillon, G. Morpurgo, Phys. Lett. B 448
1999
Cited alongside, same era.
G. Blanpied et al., Phys. Rev. C 64
2001
Cited alongside, same era.
A.J. Buchmann, E.M. Henley, Phys. Rev. C 63
2001
Cited alongside, same era.
M. Kotulla et al., Phys. Rev. Lett. 89
2002
Cited alongside, same era.
If two of these had the same particle index, spin commutation relations would reduce them to a single Pauli matrix
Cited in the paper.
For ground state baryons an allowed operator Ω \Omega must transform according to one of the irreducible representations found in the product 𝟓𝟔 ¯ × 𝟓𝟔 = 𝟏 + 𝟑𝟓 + 𝟒𝟎𝟓 + 𝟐𝟔𝟗𝟓 . \bar{{\bf 56}}\times{\bf 56}={\bf 1}+{\bf 35}+{\bf 405}+{\bf 2695}. Here, the 1
Cited in the paper.
A.J. Buchmann and R.F. Lebed, Phys. Rev. D 62
2002
Later among the works it cites.
A.J. Buchmann and E.M. Henley, Phys. Rev. D 65
2002
Later among the works it cites.
L. Tiator, D. Drechsel, S.S. Kamalov, and S.N. Yang, Eur. Phys. J. A 17
2003
Later among the works it cites.
A.M. Bernstein and C.N. Papanicolas, AIP Conference Proceedings 904
2007
Later among the works it cites.
V. Pascalutsa and M. Vanderhaeghen, S. N. Yang, Phys. Rep. 437
2007
Later among the works it cites.
alphaXiv searches the wider corpus for related work and actual follow-ups.
alphaXiv is searching for related work…