fourier transform of e^-2x
Answers
Step-by-step explanation:
Caveat: I'm using the normalization f^(ω)=∫∞−∞f(t)e−itωdt.
A cute way to to derive the Fourier transform of f(t)=e−t2 is the following trick: Since
f′(t)=−2te−t2=−2tf(t),
taking the Fourier transfom of both sides will give us
iωf^(ω)=−2if^′(ω).
Solving this differential equation for f^ yields
f^(ω)=Ce−ω2/4
and plugging in ω=0 finally gives
C=f^(0)=∫∞−∞e−t2dt=π−−√.
I.e.
f^(ω)=π−−√e−ω2/4.
Thanks yes that seems familiar could you explain how you get to the step ................ taking the Fourier transfom of both sides will give us
iωf^(ω)=−2if^′(ω).
– S F
Those should be familiar "rules" for Fourier transforms: The Fourier transform of f′(t) is iωf^(ω) and the FT of tf(t) is −if^′(ω). If they are not familiar, they follow fairly easily from the definition of the Fourier transform. – mrf
Furthermore why does e^-infinity - e^ infinity = square root(pi)