- #1
sufive
- 23
- 0
Dear Colleagues,
How to prove Fourier transformation rules of the following function
\int k^a * exp[i*k*x] * dk = x^{-1-a} * Gamma[1+a] * sin[a*pi/2] ------------(1)
I need this equation to prove some conclusions in translating propagators
in momentum space to position-space. I wish those know solutions to this
question give me hints or references urgently.
The following is the information I know, but I cannot get to the final goal.
By variable changes, k*x -> z, it's easy to get the factor k^{-1-a}, i.e.
l.h.s -> (\int z^a * exp[i*z] * dz) / x^{1+a} -------------------------------------(2)
but the remaining integration seems very difficult.
We know,
\int z^a * exp[-z] * dz \propto Gamma[1+a] --------------------------------------(3)
So, my key question is, how to do integrations in eq(2) whose exponential
argument is imaginary instead negative?
Thanks to everyone!
How to prove Fourier transformation rules of the following function
\int k^a * exp[i*k*x] * dk = x^{-1-a} * Gamma[1+a] * sin[a*pi/2] ------------(1)
I need this equation to prove some conclusions in translating propagators
in momentum space to position-space. I wish those know solutions to this
question give me hints or references urgently.
The following is the information I know, but I cannot get to the final goal.
By variable changes, k*x -> z, it's easy to get the factor k^{-1-a}, i.e.
l.h.s -> (\int z^a * exp[i*z] * dz) / x^{1+a} -------------------------------------(2)
but the remaining integration seems very difficult.
We know,
\int z^a * exp[-z] * dz \propto Gamma[1+a] --------------------------------------(3)
So, my key question is, how to do integrations in eq(2) whose exponential
argument is imaginary instead negative?
Thanks to everyone!