Concept of Field: Canonical Formalism in QFT

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Discussion Overview

The discussion revolves around the canonical formalism in quantum field theory (QFT) and its relation to the concept of fields. Participants explore the transition from classical field theory to QFT, addressing the replacement of generalized coordinates with field functions.

Discussion Character

  • Exploratory, Technical explanation, Conceptual clarification, Homework-related

Main Points Raised

  • One participant seeks clarification on the canonical formalism and the replacement of generalized coordinates with field functions in QFT.
  • Another participant emphasizes the importance of understanding classical field theory before tackling QFT, noting that classical field theory generalizes systems with finite degrees of freedom to those with infinite degrees of freedom.
  • A participant mentions the complexity of transitioning to QFT and suggests reading 't Hooft's work for a conceptual basis.
  • One participant expresses their current focus on mastering classical field theory and outlines their academic constraints, indicating a lack of time to delve into QFT at the moment.
  • Another participant recommends checking field theory textbooks, specifically mentioning Mandl and Shaw as a good reference for canonical formalism.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the understanding of canonical formalism in QFT, with some expressing uncertainty and others focusing on foundational topics. Multiple viewpoints regarding the prerequisites for studying QFT are present.

Contextual Notes

Some participants highlight limitations in their current understanding of classical field theory and the prerequisites for studying QFT, indicating that their knowledge may not be comprehensive.

Who May Find This Useful

Individuals interested in the foundational aspects of quantum field theory, classical field theory, and those seeking references for further study in these areas may find this discussion useful.

preet0283
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can ne 1 explain 2 me the canonical formalism of generalising the concept of field in QFT...i m not 2 sure abt the replacement of generalised coordinates q(i) i=1,2,... n with phi(x)
 
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I'm not sure if this view is popular, but I for one would personally appreciate if you wrote your posts in correct English as it makes it a lot easier for me to read.

I would recommend that you first gain an understanding of the classical field before you attempt to learn about a quantum system which reduces to a classical field theory in a certain limit (which is what QFT is; see 't Hooft's piece on the "conceptual basis for QFT" for further details).

Classical field theory is the generalisation of a system with finite degrees to one with infinite degrees of freedom. This is why we replace co-ordinates with a (usually) function; we have a Lagrangian density {\cal L} (which is a scalar) and we try and extremize the action given by this Lagrangian so that:

\delta \frac{1}{c}\int{\cal L} d^4\vec{x} = 0

and this procedure generates field equations.

Getting to QFT is a lot more complicated, and I would recommend firstly 't Hooft's work as a brief introduction and then to dive into one of the several texts on the topic.
 
thanks for the help ...and i apologise for not writing in the correct english ... could u please tell me more about the references for QFT
 
I'm sorry, but at this stage I'm only just about mastering Classical Field Theory -- EM was relatively simple (no pun intended), and GR took a bit of work. Term has started again, and I have little free time to continue my dalliances in advanced physics. QFT is my next topic of interest, but I have to learn thermodynamics, quantum mechanics and electromagnetism + optics according to the syllabus for my exams this year.

Essentially what I'm trying to say (and doing so badly) is that you'll have to ask someone else.
 
f u want a gd xplanation of th canonical frmlsm then prob just check any field thry bk.

I find Mandl and Shaw and good reference.

chrs.
 

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