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- W1926095209 abstract "The nucleon self-energy and its relation to the nucleon axial charge gA are discussed at large Nc. The energy is compared for the hedgehog, conventional, and recently proposed dichotomous nucleon wavefunctions which give different values for gA. We consider their energies at both perturbative and non-perturbative levels. In perturbative estimates, we take into account the pion exchanges among quarks up to the third orders of axial charge vertices, including the many-body forces such as the Wess-Zumino terms. It turns out that the perturbative pion exchanges among valence quarks give the same leading Nc contributions for three wavefunctions, while their mass differences are O(Lamba_qcd). The signs of splittings flip for different orders of the axial charge vertices, so it is hard to conclude which one is the most energetically favored. For non-perturbative estimates involving the modification of quark bases, we use the chiral quark soliton model as an illustration. With the hedgehog quark wavefunctions with gA of O(Nc), we investigate whether solutions with coherent pions are energetically favored. Again it is hard to give decisive conclusions, but it is likely that adding the confining effects disfavors the solution with the coherent pions, making a pion cloud around a nucleon quantum rather than coherent. The nuclear matter at large Nc is also discussed in light of the value of gA." @default.
- W1926095209 created "2016-06-24" @default.
- W1926095209 creator A5036052560 @default.
- W1926095209 date "2013-02-01" @default.
- W1926095209 modified "2023-10-03" @default.
- W1926095209 title "Can the nucleon axial charge be ?" @default.
- W1926095209 cites W145550202 @default.
- W1926095209 cites W1497250908 @default.
- W1926095209 cites W1756775360 @default.
- W1926095209 cites W1815296165 @default.
- W1926095209 cites W1869515999 @default.
- W1926095209 cites W1964683291 @default.
- W1926095209 cites W1964799454 @default.
- W1926095209 cites W1967167699 @default.
- W1926095209 cites W1971107372 @default.
- W1926095209 cites W1974366566 @default.
- W1926095209 cites W1976168478 @default.
- W1926095209 cites W1976339978 @default.
- W1926095209 cites W1978790589 @default.
- W1926095209 cites W1978810016 @default.
- W1926095209 cites W1979630741 @default.
- W1926095209 cites W1984699758 @default.
- W1926095209 cites W1989545275 @default.
- W1926095209 cites W1993508664 @default.
- W1926095209 cites W1998908695 @default.
- W1926095209 cites W1999421686 @default.
- W1926095209 cites W2000442025 @default.
- W1926095209 cites W2000757904 @default.
- W1926095209 cites W2000893655 @default.
- W1926095209 cites W2001359355 @default.
- W1926095209 cites W2001392205 @default.
- W1926095209 cites W2001966693 @default.
- W1926095209 cites W2002595530 @default.
- W1926095209 cites W2004821984 @default.
- W1926095209 cites W2007884756 @default.
- W1926095209 cites W2010968937 @default.
- W1926095209 cites W2011564386 @default.
- W1926095209 cites W2017152320 @default.
- W1926095209 cites W2017629854 @default.
- W1926095209 cites W2018603564 @default.
- W1926095209 cites W2028117837 @default.
- W1926095209 cites W2029085152 @default.
- W1926095209 cites W2033960318 @default.
- W1926095209 cites W2034430164 @default.
- W1926095209 cites W2037788066 @default.
- W1926095209 cites W2042248841 @default.
- W1926095209 cites W2042347788 @default.
- W1926095209 cites W2043866013 @default.
- W1926095209 cites W2044127898 @default.
- W1926095209 cites W2050773679 @default.
- W1926095209 cites W2053030790 @default.
- W1926095209 cites W2054555035 @default.
- W1926095209 cites W2057456532 @default.
- W1926095209 cites W2062946384 @default.
- W1926095209 cites W2069957981 @default.
- W1926095209 cites W2080259298 @default.
- W1926095209 cites W2080311006 @default.
- W1926095209 cites W2083371794 @default.
- W1926095209 cites W2084051200 @default.
- W1926095209 cites W2084619821 @default.
- W1926095209 cites W2084685833 @default.
- W1926095209 cites W2087831571 @default.
- W1926095209 cites W2088658813 @default.
- W1926095209 cites W2091714703 @default.
- W1926095209 cites W2092488504 @default.
- W1926095209 cites W2094755808 @default.
- W1926095209 cites W2097475575 @default.
- W1926095209 cites W2104017398 @default.
- W1926095209 cites W2104603839 @default.
- W1926095209 cites W2116048063 @default.
- W1926095209 cites W2127400118 @default.
- W1926095209 cites W2140530668 @default.
- W1926095209 cites W2145492370 @default.
- W1926095209 cites W2156852522 @default.
- W1926095209 cites W2161761018 @default.
- W1926095209 cites W2169002648 @default.
- W1926095209 cites W2191709252 @default.
- W1926095209 cites W2234342599 @default.
- W1926095209 cites W2530154967 @default.
- W1926095209 cites W2594560099 @default.
- W1926095209 doi "https://doi.org/10.1016/j.nuclphysa.2012.12.116" @default.
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