Graduate How to take non-relativistic limit of the following Lagrangian

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SUMMARY

The discussion focuses on deriving the non-relativistic limit of the Lagrangian given by $$L=g \partial_{\mu} a \bar{\psi} \gamma^{\mu}\gamma^5\psi$$, which results in the Hamiltonian $$H=-g\vec{\nabla} a \cdot \vec{\sigma_{\psi}}$$. The variables involved include the axion field (a), the fermion field ($\psi$), the interaction strength (g), and the spin operator ($\sigma_{\psi}$). Participants seek guidance on transitioning from the Lagrangian to the non-relativistic Hamiltonian and inquire about the non-relativistic limit of Dirac spinors, referencing relevant literature for Yukawa interactions.

PREREQUISITES
  • Understanding of Lagrangian mechanics in quantum field theory
  • Familiarity with non-relativistic quantum mechanics
  • Knowledge of Dirac spinors and their properties
  • Basic grasp of axion physics and its implications
NEXT STEPS
  • Study the derivation of the non-relativistic limit of Dirac spinors
  • Examine the process of obtaining Hamiltonians from Lagrangians in quantum field theory
  • Review the papers on Yukawa interactions for comparative analysis
  • Explore the implications of axion fields in particle physics
USEFUL FOR

Physicists, particularly those specializing in quantum field theory, particle physics researchers, and students exploring the non-relativistic limits of complex fields.

Tan Tixuan
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TL;DR
I want to take the non-relativistic limit of the following Lagrangian.
In https://arxiv.org/pdf/1709.07852.pdf, it is claimed in equation (1) and (2) that when we take non-relativistic limit, the following Lagrangian (the interaction part)
$$L=g \partial_{\mu} a \bar{\psi} \gamma^{\mu}\gamma^5\psi$$

will yield the following Hamiltonian
$$H=-g\vec{\nabla} a \cdot \vec{\sigma_{\psi}}$$

Where ##a## is the axion field (scalar field), and ##\psi## is a fermion field. g is the interaction strength. ##\sigma_{\psi}## is the spin operator of the fermion field.

Can anyone teach me how to take this limit? How to start from the Lagrangian and obtain the non-relativistic Hamiltonian?
 
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