Understanding the QCD Sum Rule: What is it and How Does it Work?

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i just wonder why we call it "sum rule"?

waht do we sum, and what sum for?
 
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Although 'sum rule' was originally a sum over discrete eigenstates, the term is also used to describe integrals over continuous spectra.
 
In deep inelastic scattering one derives sum rules from structure Functions F(x,Q²) integrating over x where x is the fraction of the nucleon momentum carried by the scattering quark. So sum rules give us e.g. the fraction of energy, spin, etc. of the nucleon carried e.g. by a specific quark flavour.
 
thanks, all guys
 
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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