Fourier Transform
#Math
$\displaystyle f(x)=\frac{1}{\sqrt{ 2\pi }}\int_{-\infty}^{\infty} \tilde{f}(k)e^{ikx} , \mathrm{d}k$
- The Fourier transform of a reciprocal Space function
$\displaystyle \mathcal{F}[f(x)]=\tilde{f}(k)=\frac{1}{\sqrt{ 2\pi }}\int_{-\infty}^{\infty} f(x)e^{-ikx} , \mathrm{d}x$
- This is the Fourier transform of $\displaystyle f(x)$ that takes inputs from $\displaystyle k$ space
$\displaystyle \int_{-\infty}^{\infty} f(t) , \mathrm{d}t=\tilde{f}(0)$
$\displaystyle \mathcal{F}[f(t)\cdot g(t)]=\mathcal{F}[f(t)]*\mathcal{F}[g(t)]$
Quantum Physics
Topics
- Momentum Basis
- Borwein Integrals
$\displaystyle \Psi(x)=\frac{1}{\sqrt{ 2\pi }}\int_{-\infty}^{\infty} \tilde{\Psi}(k)e^{ikx} , \mathrm{d}k$
$\displaystyle \tilde{\Psi}(k)=\frac{1}{\sqrt{ 2\pi }}\int_{-\infty}^{\infty} \Psi(x)e^{-ikx} , \mathrm{d}x$
Signal Processing
$\displaystyle F(j\omega)=\int_{-\infty}^{\infty} f(t)e^{-j\omega t} , \mathrm{d}t$
- The $\displaystyle F(j\omega)$ is effectively the same as $\displaystyle F(\omega)$