Difference between revisions of "Marks-Gravagne-Davis Fourier transform"

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=See also=
 
=See also=
[Cuchta-Georgiev Fourier transform]
+
[[Cuchta-Georgiev Fourier transform]]
  
 
=References=
 
=References=
 
*{{PaperReference|A generalized Fourier transform and convolution on time scales|2008|Robert J. Marks II|author2=Ian A. Gravagne|author3=John M. Davis|prev=|next=}}: Section 3
 
*{{PaperReference|A generalized Fourier transform and convolution on time scales|2008|Robert J. Marks II|author2=Ian A. Gravagne|author3=John M. Davis|prev=|next=}}: Section 3
 
[http://web.ecs.baylor.edu/faculty/gravagnei/archived/Fourier.pdf]
 
[http://web.ecs.baylor.edu/faculty/gravagnei/archived/Fourier.pdf]

Revision as of 15:52, 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 a function. Define the Fourier transform of $f$ centered at $s$ by $$\mathscr{F}\{f\}(z;s)=\displaystyle\int_{\mathbb{T}} f(\tau)e_{\ominus \mathring{\iota} 2 \pi z}(\tau,s) \Delta \tau,$$ where $\ominus$ denotes the circle minus operation, $e_{\ominus \mathring{\iota}2 \pi z}$ denotes the delta exponential, and $\mathring{\iota}$ denotes the Hilger pure imaginary.

See also

Cuchta-Georgiev Fourier transform

References

[1]