From Semiclassical to Quantum Approach

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SUMMARY

The discussion focuses on the transition from semiclassical to quantum approaches in the context of path integrals. It highlights the asymptotic series in \hbar, specifically the expression I= \int D[\phi]e^{-S[\phi]/\hbar}=I_{WKB}(1+ \sum_{n=1}^{\infty} a(n,X)\hbar ^{n}). The series converges only as h approaches zero, while diverging for h equal to one. The application of Borel resummation allows for the summation of the asymptotic series for any argument value, although it is constrained by specific axioms and is applicable only to certain well-defined series.

PREREQUISITES
  • Understanding of path integrals in quantum mechanics
  • Familiarity with asymptotic series and their convergence properties
  • Knowledge of Borel resummation techniques
  • Basic principles of quantum field theory
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  • Study the principles of semiclassical approximations in quantum mechanics
  • Explore the mathematical foundations of asymptotic series
  • Learn about Borel resummation and its applications in physics
  • Investigate specific examples of asymptotic series with physical relevance
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The discussion is beneficial for theoretical physicists, particularly those specializing in quantum mechanics and quantum field theory, as well as mathematicians interested in asymptotic analysis and resummation techniques.

lokofer
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From "Semiclassical" to Quantum Approach..

If we use the semiclassical expansion of a "path integral" to quantize a theory we have the "Asymptotic series (in [tex]\hbar[/tex] )

[tex]I= \int D[\phi]e^{-S[\phi]/\hbar}=I_{WKB}(1+ \sum_{n=1}^{\infty} a(n,X)\hbar ^{n})[/tex]

The problem is that the "series" involving [tex]\hbar[/tex] does only converges for h-->0 ( with a few terms) for example for h-->1 the series is divergent although if we apply "Borel resummation" we get:

[tex]\sum_{n=1}^{\infty}a(n,X)\hbar ^{n} \rightarrow \int_{0}^{\infty}duB(u,X)e^{-u/\hbar}(1/\hbar)[/tex]

With [tex]B(u,X)= \sum_{n=1}^{\infty} a(n,X)\frac{u^{n}}{n!}[/tex]

So, an asymptotic series can be "summed" for every value of the argument (big or small)
 
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Thats correct, but note that Borel summation is limited by its own axioms, you cannot use it for every asymptotic series, just some nice ones (and the ones where you can that have physical relevance are typically famous and rare examples)
 

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