Difference between revisions of "Cuchta-Georgiev Fourier transform"
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=Properties= | =Properties= | ||
[[Cuchta-Georgiev Fourier transform of delta derivatives]] | [[Cuchta-Georgiev Fourier transform of delta derivatives]] | ||
+ | |||
+ | =Examples= | ||
+ | <center> | ||
+ | {| class="wikitable" | ||
+ | |+Marks-Gravagne-Davis Fourier transform on various time scales | ||
+ | |- | ||
+ | |$\mathbb{T}$ | ||
+ | | | ||
+ | |- | ||
+ | |[[Real_numbers | $\mathbb{R}$]] | ||
+ | |$\mathcal{F}\{f\}(z;s)= \displaystyle\int_{-\infty}^{\infty} f(t)e^{2\pi izt} \mathrm{d}t$ | ||
+ | |- | ||
+ | |[[Integers | $\mathbb{Z}$]] | ||
+ | |$\mathcal{F}\{f\}(z;s) = \displaystyle\sum_{k=-\infty}^{\infty} f(k)e^{2\pi izk} $ | ||
+ | |- | ||
+ | |[[Multiples_of_integers | $h\mathbb{Z}$]] | ||
+ | | $\mathcal{F}\{f\}(z;s) = h\displaystyle\sum_{k=-\infty}^{\infty} f(hk) e^{2\pi i zhk}$ | ||
+ | |- | ||
+ | | [[Square_integers | $\mathbb{Z}^2$]] | ||
+ | | $\mathcal{F}\{f\}(z;s) = $ | ||
+ | |- | ||
+ | |[[Quantum_q_greater_than_1 | $\overline{q^{\mathbb{Z}}}, q > 1$]] | ||
+ | | $\mathcal{F}\{f\}(z;s) = $ | ||
+ | |- | ||
+ | |[[Quantum_q_less_than_1 | $\overline{q^{\mathbb{Z}}}, q < 1$]] | ||
+ | | $\mathcal{F}\{f\}(z;s) =$ | ||
+ | |- | ||
+ | |[[Harmonic_numbers | $\mathbb{H}$]] | ||
+ | |$\mathcal{F}\{f\}(z;s) = $ | ||
+ | |} | ||
+ | </center> | ||
+ | |||
=See also= | =See also= |
Revision as of 16:44, 15 January 2023
Let $\mathbb{T}$ be a time scale and let $s \in \mathbb{T}$. Let $f \colon \mathbb{T} \rightarrow \mathbb{C}$ be regulated. Define the Cuchta-Georgiev Fourier transform of $f$ centered at $s$ by $$\mathcal{F}_{\mathbb{T}}\{f\}(z;s)=\displaystyle\int_{\mathbb{T}} f(\tau)e_{\ominus iz}(\sigma(t),\tau) \Delta \tau,$$ where $\ominus$ denotes the forward circle minus operation and $e_{\ominus iz}$ denotes the delta exponential.
Contents
Properties
Cuchta-Georgiev Fourier transform of delta derivatives
Examples
$\mathbb{T}$ | |
$\mathbb{R}$ | $\mathcal{F}\{f\}(z;s)= \displaystyle\int_{-\infty}^{\infty} f(t)e^{2\pi izt} \mathrm{d}t$ |
$\mathbb{Z}$ | $\mathcal{F}\{f\}(z;s) = \displaystyle\sum_{k=-\infty}^{\infty} f(k)e^{2\pi izk} $ |
$h\mathbb{Z}$ | $\mathcal{F}\{f\}(z;s) = h\displaystyle\sum_{k=-\infty}^{\infty} f(hk) e^{2\pi i zhk}$ |
$\mathbb{Z}^2$ | $\mathcal{F}\{f\}(z;s) = $ |
$\overline{q^{\mathbb{Z}}}, q > 1$ | $\mathcal{F}\{f\}(z;s) = $ |
$\overline{q^{\mathbb{Z}}}, q < 1$ | $\mathcal{F}\{f\}(z;s) =$ |
$\mathbb{H}$ | $\mathcal{F}\{f\}(z;s) = $ |
See also
Marks-Gravagne-Davis Fourier transform
References
- Tom Cuchta and Svetlin Georgiev: Analysis of the bilateral Laplace transform on time scales with applications (2021): Definition 4.1 (15)