Can You Show Me How to Find the Integral of a Smooth Function Using Limits?

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SUMMARY

The discussion focuses on demonstrating the integral of a smooth function using limits, specifically the expression involving the limit as epsilon approaches zero. The key formula discussed is: lim_{epsilon→0+}epsilon∫_{−∞}^{∞}f(τ)e^{−epsilon/τ}dτ=f(+∞)+f(−∞). Participants emphasize the importance of selecting appropriate functions for integration, particularly those with known values at infinity. The discussion also highlights the relevance of these concepts in scattering theory, particularly in the context of adiabatic switching of interactions.

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  • Familiarity with smooth functions and their properties
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ndung200790
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Please demonstrate this expression for me:
For any smooth function f(τ):
f(+[itex]\infty[/itex])+f(-[itex]\infty[/itex])=lim[itex]_{\epsilon\rightarrow0+}[/itex][itex]\epsilon[/itex][itex]\int[/itex][itex]^{+\infty}_{-\infty}[/itex]dτf(τ)exp(-ε/τ/).
 
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You mean:
$$\lim_{x\rightarrow\infty}\big(f(x)+f(-x)\big)
= \lim_{\epsilon\rightarrow 0^+}\epsilon \int_{-\infty}^\infty f(\tau)e^{-\epsilon/\tau}d\tau$$
... but you can demonstrate it to yourself by picking a function and doing the integration.
Hint: pick one where you know the value at ##\pm\infty##.
 
No, what he means is
[tex]\lim_{\epsilon \rightarrow 0^+}\epsilon \int_{-\infty}^{\infty} \mathrm{d} t \; f(t) \exp(-\epsilon |t|)=f(\infty)+f(-\infty).[/tex]
We start with one half of the integral
[tex]I_1=\epsilon \int_0^{\infty} \mathrm{d} t f(t) \exp(-\epsilon t).[/tex]
Substitution of [itex]t=\epsilon \eta[/itex] leads to
[tex]I_1=\int_0^{\infty} \mathrm{d} \eta f \left (\frac{\eta}{\epsilon} \right ) \exp(-\eta).[/tex]
Now according to the mean-value theorem for integration, there exists some [itex]\tilde{\eta} > 0[/itex] such that
[tex]I_1=f \left (\frac{\tilde{\eta}}{\epsilon} \right ) \int_0^{\infty} \mathrm{d} \eta \exp(-\eta) =f \left (\frac{\tilde{\eta}}{\epsilon} \right ).[/tex]
Now for [itex]\epsilon \rightarrow 0^+[/itex] this gives [itex]f(\infty)[/itex], supposed this limit exists.

The other half of the integral can be treated analogously. Such considerations play an important role in scattering theory ("adiabatic switching of the interaction").
 

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