Some inequalities for entire functions

Let $\mathcal{L}_p$ be the subspace of the space $L_p(\bR)$ consisting of the restriction to the real axis of all entire functions of exponential type $\le \pi$. In this paper, for any function $f\in \mathcal{L}_p \,\,(1\le p\le \infty)$, we obtain estimates for the norm of $f$ in terms of the sequence $(f(n/2))_{n\in\bZ},$ namely$$\frac12 \|f\|_{p,1}\le \|f\|_{\mathcal{L}_p}\le 2 \|f\|_{p,1},$$where $\|f\|_{p,1}:=\frac12(\|Jf\|_{\ell_p(\bZ)} +\|JT_{1/2}f\|_{\ell_p(\bZ)})$. Here $J:\mathcal{L}_p\to\ell_p(\bZ)$ is the linear operator given by the formula $$ (Jf)(n):=(-1)^nf(n), \quad n\in\bZ,$$ and $T_\tau$ is the shift by $\tau\in\bR$ of the function $f$,$$ (T_\tau f)(z):=f(z+\tau), \quad z\in\bC.$$

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Publication Details

Journal
Matematychni Studii
Published
2024-09-15
DOI
https://doi.org/10.30970/ms.62.1.109-112
Citations
1
Primary Topic
Meromorphic and Entire Functions
Type
article
Field-Weighted Citation Impact
0.97
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article

Some inequalities for entire functions

D. Lukivska, N. Sushchyk
1 citations
Matematychni Studii
Meromorphic and Entire Functions
0.97
article

Some inequalities for entire functions

D. Lukivska, N. Sushchyk
article en
1 citations

Abstract

Let $\mathcal{L}_p$ be the subspace of the space $L_p(\bR)$ consisting of the restriction to the real axis of all entire functions of exponential type $\le \pi$. In this paper, for any function $f\in \mathcal{L}_p \,\,(1\le p\le \infty)$, we obtain estimates for the norm of $f$ in terms of the sequence $(f(n/2))_{n\in\bZ},$ namely$$\frac12 \|f\|_{p,1}\le \|f\|_{\mathcal{L}_p}\le 2 \|f\|_{p,1},$$where $\|f\|_{p,1}:=\frac12(\|Jf\|_{\ell_p(\bZ)} +\|JT_{1/2}f\|_{\ell_p(\bZ)})$. Here $J:\mathcal{L}_p\to\ell_p(\bZ)$ is the linear operator given by the formula $$ (Jf)(n):=(-1)^nf(n), \quad n\in\bZ,$$ and $T_\tau$ is the shift by $\tau\in\bR$ of the function $f$,$$ (T_\tau f)(z):=f(z+\tau), \quad z\in\bC.$$

Matematychni StudiiVol. 62(1)
Lviv University (UA)
Openalex Percentile: Top 26%
Meromorphic and Entire Functions
0.97
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