Prerequisites for Learning Lagrangian Formalism in Quantum Field Theory

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SUMMARY

The prerequisites for learning Lagrangian formalism in Quantum Field Theory (QFT) include a solid understanding of calculus, specifically integration and differentiation with several variables, as well as functionals. Familiarity with basic Newtonian mechanics is also essential. Key physics concepts outlined by Mark Srdnecki in his QFT draft include differential scattering cross-section, creation and annihilation operators, angular momentum ladder operators, and the evolution of operators in the Heisenberg picture. Mastery of these topics is crucial for a comprehensive understanding of the Lagrangian approach in QFT.

PREREQUISITES
  • Integration and differentiation with several variables
  • Functionals
  • Basic Newtonian mechanics
  • Familiarity with quantum mechanics and electromagnetism
NEXT STEPS
  • Study differential scattering cross-section in quantum mechanics
  • Learn about creation and annihilation operators in quantum field theory
  • Understand angular momentum ladder operators and their applications
  • Explore the evolution of operators in the Heisenberg picture
USEFUL FOR

Students and researchers in theoretical physics, particularly those focusing on Quantum Field Theory, as well as anyone seeking to deepen their understanding of Lagrangian mechanics and its applications in modern physics.

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Hi,

May anybody tell the pre-reqs (on calculus) for learn the lagrangian formalism used on quantum field theory ? :confused:

Thanks.
 
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well integration and differentiation with several variables, functionals
 
In addition, a knowledge of basic Newtonian mechanics is helpful.

However, you mention its use in QFT. If that's your goal, you'll need a lot more physics. In the introduction to his QFT book, Mark Srdnecki gives a set of equations, mostly from QM, that one should be familiar with as prerequisites. See page 8 of

http://www.physics.ucsb.edu/~mark/ms-qft-DRAFT.pdf

Expressed in English, you should be comfortable with:

  1. Differential scattering cross-section.
  2. Creation and annihilation operators.
  3. Angular momentum ladder operators.
  4. Evolution of operators in the Heisenberg picture.
  5. Obtaining the Hamiltonian from the Lagrangian.
  6. Lorentz transformations.
  7. Relativistic energy-momentum.
  8. Electromagnetic vector potential.

Topics that are covered in good QM, E&M, and mechanics texts.
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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