What is the connection between pQCD, NRQCD, and Heavy Quark Effective Theory?

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SUMMARY

The discussion clarifies the relationship between perturbative Quantum Chromodynamics (pQCD), Non-Relativistic Quantum Chromodynamics (NRQCD), and Heavy Quark Effective Theory (HQET). pQCD is applicable in high energy and short-distance regimes, such as quark-gluon plasma, where the strong coupling constant (\alpha_s) is small. In contrast, NRQCD serves as an effective field theory for low energy and long-distance scenarios, particularly in quarkonium states. The heavy quark effective theory connects with both pQCD and NRQCD, focusing on scenarios where heavy quarks are produced near threshold, characterized by low velocities.

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What is the relationship between pQCD and NRQCD?

Is it that pQCD is for high energy/short-distance regime, e.g. quark gluon plasma? And NRQCD is for low energy/long-distance regime, e.g. quarkonium ?

And what is relation between heavy quark effective theory and pQCD and that between heavy quark effective theory and NRQCD ?

Thanks in advance.
 
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pQCD works in the perturbitive region where \alpha_s the strong coupling constant is small, Matrix elements for physical processes are obtained from expansion in this parameter. NRQCD works as an effective field theory for quarks with velocities much less than the speed of light and the results obtained are expansions in the parameter (\alpha/v)^n. pNRQCD is obtained from the low velocity limit of the QCD Lagrangian. The NRQCD effective theory is useful when heavy quarks are produced near threshold and hence have small velocites, whereas in the high energy regieme pQCD is used.
 
NRQCD expends in powers of (\alpha/v)^n but not \beta ? \beta = v/c where
v is the relative velocity of the two heavy quark constituents for quarkonium. \beta ~ 0.3 for charmonium and \beta ~0.1 for bottomonium, right?
 

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