Quantization of hamiltonian with complex form

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SUMMARY

The discussion focuses on the canonical quantization of Hamiltonians with complex forms, specifically those including interaction terms, as outlined in Bjorken and Drell Vol II. It highlights the shift from four-dimensional Fourier transforms to three-dimensional Fourier expansions at t = 0 due to the absence of plane wave solutions in interacting fields. The operator expansion coefficients maintain the same commutation relations as free fields, yet their physical interpretations as creation and destruction operators for single quanta become more complex and less straightforward.

PREREQUISITES
  • Understanding of canonical quantization procedures
  • Familiarity with Hamiltonian mechanics
  • Knowledge of quantum field theory, particularly spinor electrodynamics
  • Proficiency in Fourier analysis, specifically in three-dimensional contexts
NEXT STEPS
  • Study the canonical quantization of interacting fields in quantum field theory
  • Explore the implications of three-dimensional Fourier expansions in quantum mechanics
  • Investigate the physical interpretations of operator expansion coefficients in quantum systems
  • Review Bjorken and Drell Vol II for detailed examples of quantization in spinor electrodynamics
USEFUL FOR

Physicists, quantum field theorists, and advanced students seeking to deepen their understanding of Hamiltonian quantization methods, particularly in the context of interacting fields.

Nixom
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In most of textbooks, the canonical quantization procedure is used to quantize the hamiltonian with a simple form, the quadratic form. I just wonder how should we deal with more complex form hamiltonian, such like the ones including interaction terms?
 
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Bjorken and Drell Vol II discusses canonical quantization of spinor electrodynamics in the chapter "Interacting Fields". Since the fields are no longer free fields, they don't have plane wave solutions, so instead of four-dimensional Fourier transforms they do a three-dimensional Fourier expansion at t = 0. The operator expansion coefficients are assigned the same commutation relations as for free fields, and then show the relations continue to hold for all t.

"The operator expansion coefficients, however, no longer retain their simple physical interpretations as creation and destruction operators for single quanta of given definite masses".
 

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