Functional diffential-integral equations

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Discussion Overview

The discussion revolves around the topic of functional differential-integral equations, particularly in the context of quantum field theory and functional calculus. Participants explore the notation used for functional derivatives and the potential for solving functionals similarly to differential equations, while also considering the implications of boundary conditions and Taylor expansions of functionals.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant expresses intrigue with the notation for functional derivatives used in quantum field theory, questioning whether functionals can be solved like differential equations.
  • Another participant asserts that functionals cannot be solved in the same way as differential equations, suggesting a lack of boundary conditions for functionals.
  • A subsequent reply questions the reasoning behind the inability to solve functionals, proposing that uniqueness might be addressed through variations of the functional.
  • Participants discuss the relevance of various resources, including a specific introduction to functionals and mathematical methods for physics that cover functional analysis.
  • There is mention of the high cost of a referenced book, prompting inquiries about its value and content related to the topic.
  • Some participants express interest in Taylor expansions of functionals and draw parallels between functional calculus and operator theory in Hilbert spaces, speculating on the relationship between the two.
  • One participant notes the use of functional Taylor expressions in field theory, highlighting a desire for more rigorous explanations of these concepts.

Areas of Agreement / Disagreement

Participants do not reach a consensus on whether functionals can be solved like differential equations. There are competing views regarding the nature of functionals, boundary conditions, and the applicability of Taylor expansions.

Contextual Notes

The discussion reveals limitations in understanding functional calculus, particularly regarding boundary conditions and the specific notation used. There is also a noted absence of rigorous justification for certain techniques in functional analysis.

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I'm reading Quantum Field Theory Of Point Particles And Strings, by Brian Hatfield, chapter 9 called Functional Calculus. But he seems to assume some famiality with the subject. I'm intriqued by his notation. He uses notation for functional derivatives almost as if it were ordinary derivatives; he uses the notation:

[tex]\[<br /> \frac{{\delta F[a]}}{{\delta a(x)}}<br /> \][/tex], [tex]\[<br /> \frac{{\delta ^2 G[a]}}{{\delta a(y)^2 }}<br /> \][/tex], and [tex]\[<br /> \int {\Delta a\,\,e^{ - F[a]} } <br /> \][/tex].

I'm looking for a more complete development of these ideas using this kind of notation. I wonder if it is developed enough to solve for Functionals F[a], like differential equations solve for functions. It makes me wonder if, say, the functional Lagrangian of physics can be derived on first principles using these methods. Any guidance would be appreciated. Thanks.
 
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Yeah, no, you can't really 'solve' functionals the same way you would a differential equation.
(Oh the elusive Exact Density Functional! Hear the lament of the quantum chemist! 45 years since we http://www-theor.ch.cam.ac.uk/people/ross/thesis/node32.html" you existed and no one yet knows what you are! :cry:)

Anyway, http://julian.tau.ac.il/~bqs/functionals.pdf" seems like an okay introduction - or you could check out some Mathematical Methods for Physics books (e.g. Arfken) that have chapters on functional analysis, or one of the many dedicated books on the topic.
 
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alxm said:
Yeah, no, you can't really 'solve' functionals the same way you would a differential equation.
I wonder if there is any proof of this statement. Or are you speaking from your own experience? Could it be because there is no way to specify boundary conditions for functionals as there is for functions? Maybe not in general, but perhaps in special circumstances. Or maybe it is sufficient to show that some functional does obey the Functional differential equation. Could uniqueness be addressed by showing that a slight variation of the functional is not a solution?

alxm said:
Anyway, http://julian.tau.ac.il/~bqs/functionals.pdf" seems like an okay introduction - or you could check out some Mathematical Methods for Physics books (e.g. Arfken) that have chapters on functional analysis, or one of the many dedicated books on the topic.

In the bibliography, Brian Hatfield references F. A. Berezine, The Method of Second Quantization, 1966. I looked this up on Amazon.com; they want $530 a copy for this book. Does it really have this special information in it?

What exactly would be the topic that I would look up for this subject? I looked in some of my variational calculus books. They don't seem to use this notation and don't get into functional integration (path integrals) very much.
 
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I was also looking for this kind of stuff. For instance whenever it comes to obtain Taylor-expansions of functionals. :)
 
haushofer said:
I was also looking for this kind of stuff. For instance whenever it comes to obtain Taylor-expansions of functionals. :)

It seems there is some similarity between functional differential-integral calculus and that of operators on a Hilbert space. You can have infinite dimensional vectors in Hilbert space used to describe functions. And the operators that act on these vectors are derivatives and integrals, much like functionals that act on functions. I wonder how close the relationship is. Perhaps operator math on Hilbert space simply uses a different notation, where, perhaps, the operators are limited to being linear. There are operators defined in terms of other operators. And if I remember correctly, there are taylor expansions and power series of operators. Perhaps these techniques transfers to functional math.
 
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I guess they do, because in field theory people are quite used to use these functional Taylor expressions. For instance, when you perform a coordinate transformation and look at the functional and coordinate change of the action. I tried to find a rigorous justification for this, but somehow few people take the effort to explain this in detail. Maybe I should try it for myself :)
 

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