Why Do Theorists Use Series Expansion in Lagrangian Models?

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SUMMARY

The discussion centers on the use of series expansion in Lagrangian models, specifically within the context of chiral effective theories like the Skyrme model. It highlights how the pion field is represented as an SU(2) matrix and how nucleons are modeled as classical solitons. The conversation details the process of introducing fluctuations in the pion field and expanding the Lagrangian up to second order, which allows for the calculation of quantum corrections to nucleon masses and form factors. A key reference provided is the paper by Frank Meier and Hans Walliser, which discusses quantum corrections in chiral soliton models.

PREREQUISITES
  • Understanding of Lagrangian mechanics
  • Familiarity with chiral effective theories
  • Knowledge of SU(2) symmetry in particle physics
  • Basic concepts of quantum field theory
NEXT STEPS
  • Study the Skyrme model and its implications in particle physics
  • Learn about quantum corrections in effective field theories
  • Explore the mathematical framework of SU(2) matrices in quantum mechanics
  • Read the paper "Quantum Corrections to Baryon Properties in Chiral Soliton Models" for in-depth analysis
USEFUL FOR

Physicists, particularly those specializing in theoretical physics, quantum field theory, and particle physics, will benefit from this discussion. It is also relevant for researchers interested in effective field theories and their applications in modeling baryonic properties.

Neitrino
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Hi,
I have a following question...

Can it be that there is given some Lagrangian and instead of considering whole Lagrangian one makes its series expansion and considers only some orders of expansion? Can you bring some examples or why and when does this happen... ?

Thank you
 
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One example are chiral effective theories like the skyrme model. The pion field appears as an SU(2) matrix

U(x)=e^{i\tau^a \phi^a(x)}

Nucleons are described by classical solitons

U_0(x)=e^{i\tau^a \phi_0^a(x)}

Now you can introduce fluctuations i.e. pions in a nucleon (soliton) background

U(x)=e^{i\tau^a (\phi_0^a + \pi^a)}

and expand the resulting Lagrangian in \pi(x) up to second order; you can couple this Lagrangian to el.-mag. fields and calculate photo-pion production; you can quantize the \pi(x) fluctuations and calculate quantum corrections to nucleon masses and form factors; ...

Have a look at (e.g.)

http://arxiv.org/abs/hep-ph/9602359
Quantum Corrections to Baryon Properties in Chiral Soliton ModelsAuthors: Frank Meier, Hans Walliser
(Fachbereich Physik, U-GH Siegen, Germany)
(Submitted on 21 Feb 1996 (v1), last revised 14 Aug 1996 (this version, v2))
Abstract: We present a procedure to calculate 1-loop graphs in the soliton sector of chiral Lagrangians and use it to calculate quantum corrections to certain baryon observables in Skyrme-type models. Results generally show an improvement over the values obtained in tree approximation except for the case of the axial coupling g_A.
 

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