How Do I Prove Symmetry and Scaling Properties of the Dirac Delta Function?

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The discussion focuses on proving the symmetry and scaling properties of the Dirac delta function, specifically that δ(x) = δ(-x) and δ(kx) = (1/|k|)δ(x). The first proof involves integrating the delta function and considering the transformation u = -x, but the original poster struggles with the assumption f(u) = -f(-u). For the second proof, the integration with respect to kx is analyzed, where the sign of k affects the bounds of the integral. Participants emphasize the importance of switching the bounds when k is negative for both proofs. Overall, the conversation highlights the need for careful consideration of integral properties in these proofs.
yungman
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I want to proof (1)##\delta(x)=\delta(-x)## and (2) ## \delta(kx)=\frac{1}{|k|}\delta(x)##

(1) let ##u=-x\Rightarrow\;du=-dx##
\int_{-\infty}^{\infty}f(x)\delta(x)dx=(0)
but
\int_{-\infty}^{\infty}f(x)\delta(-x)dx=-\int_{-\infty}^{\infty}f(-u)\delta(u)du=-f(0)

I cannot proof (1) is equal as I don't know if ##f(u)=-f(-u)##. Please help.

(2)Let ##u=kx\Rightarrow\;\frac{du}{k}=dx##. The sign of the limit reverse depends on the polarity of k.
\int_{-\infty}^{\infty}f(x)\delta(kx)dx=\frac{1}{k}\int_{-\infty}^{\infty}f(\frac{u}{k})\delta(u)du=^+_-\frac{1}{k}f(0)
Since sign is +ve if k is positive. Sign is -ve if k is -ve. This means the result is always ##\frac{1}{|k|}f(0)##. Am I correct?

Thanks
 
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yungman said:
I want to proof (1)##\delta(x)=\delta(-x)## and (2) ## \delta(kx)=\frac{1}{|k|}\delta(x)##

(1) let ##u=-x\Rightarrow\;du=-dx##
\int_{-\infty}^{\infty}f(x)\delta(x)dx=(0)
but
\int_{-\infty}^{\infty}f(x)\delta(-x)dx=-\int_{-\infty}^{\infty}f(-u)\delta(u)du=-f(0)

I cannot proof (1) is equal as I don't know if ##f(u)=-f(-u)##. Please help.


The bounds of the integral change too, so you would have

\int_{-\infty}^{\infty}f(x)\delta(-x)dx=-\int_{\infty}^{-\infty}f(-u)\delta(u)du

intead of what you had. Does that change anything?
 
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micromass said:
The bounds of the integral change too, so you would have

\int_{-\infty}^{\infty}f(x)\delta(-x)dx=-\int_{\infty}^{-\infty}f(-u)\delta(u)du

intead of what you had. Does that change anything?

Got it. How about (2)

Thanks
 
yungman said:
Got it. How about (2)

Thanks

You should switch the bounds in (2) too, if ##k## is negative. Aside from that, it's alright.
 
micromass said:
You should switch the bounds in (2) too, if ##k## is negative. Aside from that, it's alright.

Thanks
 

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