
%0 Journal Article
%A Genz, Henning 
%T Two Remarks Concerning the Signs of the Light Quark Masses
%J Australian Journal of Physics
%D 1997/10/06
%V 50
%N 5
%P 913-920
%K 
%R https://doi.org/10.1071/P97018
%U https://www.publish.csiro.au/paper/P97018 
%X Partial conservation of the nine axial currents Ab&#181; for &#946; = 0, 1,..., 8 applied to the vacuum expectation values of the equal-time commutators of the nine axial charges Q&#945;A (x0) for &#945; = 0, 1,..., 8 and the corresponding axial current divergences &part;&#181;A&#946;&#181; implies that the non-vanishing current quark masses m&ugr;, md, ms of the light quarks u, d, shave the same sign. Under the more realistic assumption of partial conservation of only the eight axial currents of SU(3) &otimes; SU(3), i.e. a = 1,..., 8 and &#946; = 1,..., 8 in the above, inequalities for the quark masses follow. They are trivially fulfilled if the three light quark masses have the same sign and imply, for non-vanishing quark masses mu, md, ms that at least two of these masses have the same sign as their sum mu + md + ms. If one of the three quark masses vanishes, one of the other two might also. If both do not, they have the same sign (the same, of course, as their sum). Our assumptions include the standard vector SU(3) symmetry of the vacuum. 
