Quenched & Unquenched Quark Model

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SUMMARY

The discussion centers on the differences between the quenched and unquenched quark models in the context of Exotic Hadrons, particularly involving Charmonium states and tetraquarks. The quenched approximation in lattice QCD simplifies calculations by ignoring the determinant of fermions, treating them as nondynamical, while the unquenched model incorporates fully dynamic fermions. Key literature references include lecture notes on the qualitative aspects of the quenched approximation and methods for incorporating dynamic fermions.

PREREQUISITES
  • Understanding of Exotic Hadrons and their properties
  • Familiarity with lattice Quantum Chromodynamics (QCD)
  • Knowledge of path integral formulation in quantum field theory
  • Basic concepts of perturbation theory in quantum mechanics
NEXT STEPS
  • Study the path integral formulation of QCD in detail
  • Explore the implications of the quenched approximation in lattice QCD
  • Research methods for incorporating dynamic fermions in lattice calculations
  • Review the lecture notes on the qualitative aspects of the quenched approximation
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Researchers and students in theoretical physics, particularly those focusing on Quantum Chromodynamics, lattice QCD, and the study of Exotic Hadrons.

Naeem Anwar
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Just started the study Exotic Hadrons (like mixing of Charmonium states with tetraquarks etc.) and got confused with quenched & unquenched quark model.

What are the major differences between these two models? What key factors I should keep in mind doing calculations with these models invidiously?

I will highly acknowledge literature recommendations.
 
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In terms of the path integral (PI) for QCD , since the fermions appear only quadratically, one can symbolically do the functional integral over them to find a highly nonlocal determinant
$$ \int D\psi D\bar{\psi} \exp \left[ \bar{\psi} ( { \not{ \! \! D}} + m ) \psi \right] = \det (\not{\! \! D} + m ) .$$
Since the gauge bosons and consequently the gauge coupling appears in the covariant derivative, if we were doing perturbation theory, we could treat this beast order by order. In the quenched approximation to lattice QCD, this determinant is simply ignored for computational simplicity (its value is set equal to 1 in the PI). We could analogously call this an approximation with nondynamical fermions, i.e. fermions that we don't promote to fields that we have to integrate over in the PI.

I haven't really studied lattice QCD, so I am not up on references. The lecture notes http://arxiv.org/abs/hep-ph/0205181 discusses the qualitative aspects of the quenched approximation in one or two places. The notes http://www.itp.uni-hannover.de/saalburg/Lectures/wiese.pdf (hat-tip: atyy) are a discussion of ways to incorporate fully dynamically fermions, but I don't think he discusses the quenched approximation in any detail.
 
Although my background is not LQCD but still this material is at least giving me the spirit of my query. Thanks & looking forward some exact explanations in detail.
 

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