Modulation space
Modulation spaces[1] are a family of Banach spaces defined by the behavior of the short-time Fourier transform with respect to a test function from the Schwartz space. They were originally proposed by Hans Georg Feichtinger and are recognized to be the right kind of function spaces for time-frequency analysis. Feichtinger's algebra, while originally introduced as a new Segal algebra,[2] is identical to a certain modulation space and has become a widely used space of test functions for time-frequency analysis.
Modulation spaces are defined as follows. For , a non-negative function on and a test function , the modulation space is defined by
In the above equation, denotes the short-time Fourier transform of with respect to evaluated at , namely
- Failed to parse (unknown function "\mathscr"): {\displaystyle V_gf(x,\omega)=\int_{\mathbb{R}^d}f(t)\overline{g(t-x)}e^{-2\pi it\cdot \omega}dt=\mathscr{F}^{-1}_{\xi}(\overline{\hat{g}(\xi)}\hat{f}(\xi))).}
In other words, is equivalent to . The space is the same, independent of the test function chosen. The canonical choice is a Gaussian.
Feichtinger's algebra
For and , the modulation space is known by the name Feichtinger's algebra and often denoted by for being the minimal Segal algebra invariant under time-frequency shifts, i.e. combined translation and modulation operators. is a Banach space embedded in , and is invariant under the Fourier transform. It is for these and more properties that is a natural choice of test function space for time-frequency analysis.
References