This leads to a fixed point where the top mass is smaller, 170 200 GeV . The uncertainty in this prediction arises because the bottom quark Yukawa coupling can be amplified in the MSSM . Some theorists believe this is supporting evidence for the MSSM.
42.
A particle made up of one top and two bottom quarks & ndash; while still being of neutral charge & ndash; would be a very different beast . ( Much more massive, and very short-lived . ) talk ) 20 : 31, 8 January 2006 ( UTC)
43.
Depending on the specific details of the SUSY model and the mass hierarchy of the sparticles, the stop might decay into a bottom quark and a chargino, with a subsequent decay of the chargino into the lightest neutralino ( which is often the lightest supersymmetric particle ).
44.
The Yukawa couplings of the up, down, charm, strange and bottom quarks, are small at the extremely high energy scale of grand unification, \ mu \ approx 10 ^ { 15 } GeV . Therefore, the y ^ 2 term can be neglected in the above equation.
45.
The Yukawa couplings of the up, down, charm, strange and bottom quarks, are hypothesized to have small values at the extremely high energy scale of grand unification, 10 15 GeV . They increase in value at lower energy scales, at which the quark masses are generated by the Higgs.
46.
Two types of quarkonia have been extensively studied : charmonia, which consist of a charm quark and an anti-charm, and bottomonia made of a bottom and an anti-bottom quark . Charm and anticharm quarks in the presence of the Quark Gluon Plasma, in which there are many free colour charges, are not able to see each other any more and therefore they cannot form bound states.
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