Difference between revisions of "Hilger real axis"
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(Created page with "Let $h>0$. We define the Hilger real axis by $$\mathbb{R}_h = \left\{ z \in \mathbb{C}_h \colon z \in \mathbb{R}, z > -\dfrac{1}{h} \right\},$$ where $\mathbb{C}_h$ is the H...") |
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Let $h>0$. We define the Hilger real axis by | Let $h>0$. We define the Hilger real axis by | ||
| − | $$\mathbb{R}_h = \left\{ z \in \mathbb{ | + | $$\mathbb{R}_h = \left\{ z \in \mathbb{R} \colon z > -\dfrac{1}{h} \right\},$$ |
| − | + | and for $h=0$, we let $\mathbb{R}_0=\mathbb{R}$. | |
| + | |||
| + | =Properties= | ||
| + | |||
| + | =References= | ||
| + | *{{PaperReference|A generalized Fourier transform and convolution on time scales|2008|Robert J. Marks II|author2=Ian A. Gravagne|author3=John M. Davis|prev=Hilger complex plane|next=Hilger alternating axis}}: Definition $2.2$ | ||
Revision as of 00:41, 30 May 2017
Let $h>0$. We define the Hilger real axis by $$\mathbb{R}_h = \left\{ z \in \mathbb{R} \colon z > -\dfrac{1}{h} \right\},$$ and for $h=0$, we let $\mathbb{R}_0=\mathbb{R}$.
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 $2.2$
