What Are the 8 Gluons and Their Role in Subatomic Physics?

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what are they?
 
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There are three quarks (with three color indices i=1,2,3); this can be written as qi. Now we want to introduce an algebra of matrices A acting on this object qi, that means Aik qk (with a sum over k). These matrices A live in a 3*3 matrix algebra. For complex qi there are two possibilities u(3) and su(3). u(3) is something like u(1) + su(3) which means that there would be a structure like u(1) which corresponds to a long-range force w/o self-interaction which is something like electromagnetism. b/c we do not observe this force we have to chose su(3) instead. Writing down basis vectors for this su(3) algebra one finds that there are eight, not nine, b/c due to the 's' in 'su(3)' one must use only traceless matrices; a matrix with trace ≠ 0 would correspond to the u(1). This reduces the nine possible basis vectors to eight.
 
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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