Difference between revisions of "Hilger alternating axis"
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$$\mathbb{A}_h = \left\{z \in \mathbb{C}_h \colon z \in \mathbb{R}, z < -\dfrac{1}{h} \right\},$$ | $$\mathbb{A}_h = \left\{z \in \mathbb{C}_h \colon z \in \mathbb{R}, z < -\dfrac{1}{h} \right\},$$ | ||
where $\mathbb{C}_h$ is the [[Hilger complex plane]]. | where $\mathbb{C}_h$ is the [[Hilger complex plane]]. | ||
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| + | =Properties= | ||
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| + | =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=Hilger real axis|next=Hilger circle}}: Definition $2.2$ | ||
Revision as of 00:38, 30 May 2017
The Hilger alternating axis is defined by $$\mathbb{A}_h = \left\{z \in \mathbb{C}_h \colon z \in \mathbb{R}, z < -\dfrac{1}{h} \right\},$$ where $\mathbb{C}_h$ is the Hilger complex plane.
Properties
References
- Robert J. Marks II, Ian A. Gravagne and John M. Davis: A generalized Fourier transform and convolution on time scales (2008)... (previous)... (next): Definition $2.2$
