The Hardy-Littlewood theorem on fractional integration for Laguerre series
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- by Yūichi Kanjin and Enji Sato
- Proc. Amer. Math. Soc. 123 (1995), 2165-2171
- DOI: https://doi.org/10.1090/S0002-9939-1995-1257113-2
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Abstract:
The Hardy-Littlewood theorem on fractional integration for Fourier series says that if ${I_\sigma }g \sim \sum \nolimits _{n \ne 0} {|n{|^{ - \sigma }}\hat g} (n){e^{\operatorname {int} }}$, then ${I_\sigma }$ is bounded from ${L^p}$ to ${L^q}$, where $1 < p < q < \infty ,\frac {1}{q} = \frac {1}{p} - \sigma$. We shall establish an analogue of this theorem for the Laguerre function system $\left \{ {{{\left ( {\frac {{n!}}{{\Gamma (n + \alpha + 1)}}} \right )}^{\frac {1}{2}}}L_n^\alpha (x){e^{ - \frac {x}{2}}}{x^{\frac {\alpha }{2}}}} \right \}_{n = 0}^\infty$.References
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Bibliographic Information
- © Copyright 1995 American Mathematical Society
- Journal: Proc. Amer. Math. Soc. 123 (1995), 2165-2171
- MSC: Primary 42C10; Secondary 42A45
- DOI: https://doi.org/10.1090/S0002-9939-1995-1257113-2
- MathSciNet review: 1257113