What happens to the gluon linking Quarks at time of formation of quark

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what happens to the gluon linking Quarks at time of formation of quark star? whether the quark star consists of only quarks or quark gluon plasma?
 
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There are not "some number of gluons linking quarks" in a baryon. It is more like a mess of short-living gluons and virtual quarks (and even that model can be problematic). So you just have merging messes of gluons, virtual and real quarks.
 
I must say I do not really understand the original formulation. My two cents nevertheless.

If you collide an electron with a positron at very high energies, and produce a quark-antiquark pair flying off back-to-back, some non-singlet (or "non-zero" if you will) color is flying with each member of the pair. That implies such two jets are not independent from the onset. One can be sure that there will be some amount of color neutralization via a lower energy, non-perturbative "messy" exchange, as mfb mentions.
 
Toponium is a hadron which is the bound state of a valance top quark and a valance antitop quark. Oversimplified presentations often state that top quarks don't form hadrons, because they decay to bottom quarks extremely rapidly after they are created, leaving no time to form a hadron. And, the vast majority of the time, this is true. But, the lifetime of a top quark is only an average lifetime. Sometimes it decays faster and sometimes it decays slower. In the highly improbable case that...
I'm following this paper by Kitaev on SL(2,R) representations and I'm having a problem in the normalization of the continuous eigenfunctions (eqs. (67)-(70)), which satisfy \langle f_s | f_{s'} \rangle = \int_{0}^{1} \frac{2}{(1-u)^2} f_s(u)^* f_{s'}(u) \, du. \tag{67} The singular contribution of the integral arises at the endpoint u=1 of the integral, and in the limit u \to 1, the function f_s(u) takes on the form f_s(u) \approx a_s (1-u)^{1/2 + i s} + a_s^* (1-u)^{1/2 - i s}. \tag{70}...
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