What are the next steps in constructing \phi_{3}^{4} in Field Theory?

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SUMMARY

The discussion centers on the construction of the \phi_{3}^{4} field theory, building upon the previously established \phi_{2}^{4} model. The participant has successfully created a Hilbert Space where the Hamiltonian operates without producing infinities and without an ultraviolet cut-off. The next critical steps involve demonstrating that the Hamiltonian is self-adjoint and semi-bounded, followed by the removal of the volume cut-off to advance the construction of \phi_{3}^{4}.

PREREQUISITES
  • Understanding of Hilbert Spaces in quantum mechanics
  • Knowledge of Hamiltonian operators and their properties
  • Familiarity with the concepts of self-adjointness and semi-boundedness
  • Basic principles of quantum field theory, particularly \phi^{4} theories
NEXT STEPS
  • Research the criteria for self-adjointness in quantum mechanics
  • Study semi-bounded operators and their implications in field theory
  • Explore techniques for removing volume cut-offs in quantum field theories
  • Examine the construction and properties of \phi_{2}^{4} as a foundational model
USEFUL FOR

This discussion is beneficial for theoretical physicists, particularly those specializing in quantum field theory, as well as graduate students and researchers looking to deepen their understanding of advanced field theory constructions.

DarMM
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I previously took part in two separate threads where I slowly went through various field theories from a rigorous perspective. I would like to restart the discussion. Here are the two previous threads for anybody who would like to take part this time:

Thread 1
The pages from 12 on (and especially 15 and 16) are the most relevant.

Also:
Thread 2

So far [tex]\phi_{2}^{4}[/tex] has been constructed. For [tex]\phi_{3}^{4}[/tex] I have built the appropriate Hilbert Space on which the Hamiltonian is a well defined operator (it doesn't produce infinities in loose language) with no ultraviolet cut-off. However I must next show that it is self-adjoint and semi-bounded. After that I will need to remove the volume cut-off.
 
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DarMM said:
For [tex]\phi_{3}^{4}[/tex] I have built the appropriate Hilbert Space on which the Hamiltonian is a well defined operator (it doesn't produce infinities in loose language) with no ultraviolet cut-off. However I must next show that it is self-adjoint and semi-bounded. After that I will need to remove the volume cut-off.

Welcome back! I am looking forward to learn about the next step of the ladder!
 

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