Laguerre transform

 In mathematics, Laguerre transform is an integral transform named after the mathematician Edmond Laguerre, which uses generalized Laguerre polynomials  as kernels of the transform.[1][2][3][4]

The Laguerre transform of a function  is

The inverse Laguerre transform is given by

Some Laguerre transform pairsEdit

f(x)\, 
{\displaystyle x^{a-1},\ a>0\,}{\displaystyle {\frac {\Gamma (a+\alpha )\Gamma (n-a+1)}{n!\Gamma (1-a)}}}
{\displaystyle e^{-ax},\ a>-1\,}{\displaystyle {\frac {\Gamma (n+\alpha +1)a^{n}}{n!(a+1)^{n+\alpha +1}}}}
{\displaystyle \sin ax,\ a>0,\ \alpha =0\,}{\displaystyle {\frac {a^{n}}{(1+a^{2})^{\frac {n+1}{2}}}}\sin \left[n\tan ^{-1}{\frac {1}{a}}+\tan ^{-1}(-a)\right]}
{\displaystyle \cos ax,\ a>0,\ \alpha =0\,}{\displaystyle {\frac {a^{n}}{(1+a^{2})^{\frac {n+1}{2}}}}\cos \left[n\tan ^{-1}{\frac {1}{a}}+\tan ^{-1}(-a)\right]}
{\displaystyle L_{m}^{\alpha }(x)\,}{\displaystyle {\binom {n+\alpha }{n}}\Gamma (\alpha +1)\delta _{mn}}
{\displaystyle e^{-ax}L_{m}^{\alpha }(x)\,}{\displaystyle {\frac {\Gamma (n+\alpha +1)\Gamma (m+\alpha +1)}{n!m!\Gamma (\alpha +1)}}{\frac {(a-1)^{n-m+\alpha +1}}{a^{n+m+2\alpha +2}}}{}_{2}F_{1}\left(n+\alpha +1;{\frac {m+\alpha +1}{\alpha +1}};{\frac {1}{a^{2}}}\right)}[5]
{\displaystyle f(x)x^{\beta -\alpha }\,}{\displaystyle \sum _{m=0}^{n}(m!)^{-1}(\alpha -\beta )_{m}L_{n-m}^{\beta }(x)}
{\displaystyle e^{x}x^{-\alpha }\Gamma (\alpha ,x)\,}{\displaystyle \sum _{n=0}^{\infty }{\binom {n+\alpha }{n}}{\frac {\Gamma (\alpha +1)}{n+1}}}
{\displaystyle x^{\beta },\ \beta >0\,}{\displaystyle \Gamma (\alpha +\beta +1)\sum _{n=0}^{\infty }{\binom {n+\alpha }{n}}(-\beta )_{n}{\frac {\Gamma (\alpha +1)}{\Gamma (n+\alpha +1)}}}
{\displaystyle (1-z)^{-(\alpha +1)}\exp \left({\frac {xz}{z-1}}\right),\ |z|<1,\ \alpha \geq 0\,}{\displaystyle \sum _{n=0}^{\infty }{\binom {n+\alpha }{n}}\Gamma (\alpha +1)z^{n}}
{\displaystyle (xz)^{-\alpha /2}e^{z}J_{\alpha }\left[2(xz)^{1/2}\right],\ |z|<1,\ \alpha \geq 0\,}{\displaystyle \sum _{n=0}^{\infty }{\binom {n+\alpha }{n}}{\frac {\Gamma (\alpha +1)}{\Gamma (n+\alpha +1)}}z^{n}}
{\displaystyle {\frac {d}{dx}}f(x)\,}{\displaystyle {\tilde {f}}_{\alpha }(n)-\alpha \sum _{k=0}^{n}{\tilde {f}}_{\alpha -1}(k)+\sum _{k=0}^{n-1}{\tilde {f}}_{\alpha }(k)}
{\displaystyle x{\frac {d}{dx}}f(x),\alpha =0\,}{\displaystyle -(n+1){\tilde {f}}_{0}(n+1)+n{\tilde {f}}_{0}(n)}
{\displaystyle \int _{0}^{x}f(t)dt,\ \alpha =0\,}{\displaystyle {\tilde {f}}_{0}(n)-{\tilde {f}}_{0}(n-1)}
{\displaystyle e^{x}x^{-\alpha }{\frac {d}{dx}}\left[e^{-x}x^{\alpha +1}{\frac {d}{dx}}\right]f(x)\,}{\displaystyle -n{\tilde {f}}_{\alpha }(n)}
{\displaystyle \left\{e^{x}x^{-\alpha }{\frac {d}{dx}}\left[e^{-x}x^{\alpha +1}{\frac {d}{dx}}\right]\right\}^{k}f(x)\,}{\displaystyle (-1)^{k}n^{k}{\tilde {f}}_{\alpha }(n)}
{\displaystyle L_{n}^{\alpha }(x),\alpha >-1\,}{\displaystyle {\frac {\Gamma (n+\alpha +1)}{n!}}}
{\displaystyle xL_{n}^{\alpha }(x),\alpha >-1\,}{\displaystyle {\frac {\Gamma (n+\alpha +1)}{n!}}(2n+1+\alpha )}
{\displaystyle {\frac {1}{\pi }}\int _{0}^{\infty }e^{-t}f(t)dt\int _{0}^{\pi }e^{{\sqrt {xt}}\cos \theta }\cos({\sqrt {xt}}\sin \theta )g(x+t-2{\sqrt {xt}}\cos \theta )d\theta ,\alpha =0\,}{\displaystyle {\tilde {f}}_{0}(n){\tilde {g}}_{0}(n)}
{\displaystyle {\frac {\Gamma (n+\alpha +1)}{{\sqrt {\pi }}\Gamma (n+1)}}\int _{0}^{\infty }e^{-t}t^{\alpha }f(t)dt\int _{0}^{\pi }e^{-{\sqrt {xt}}\cos \theta }\sin ^{2\alpha }\theta g(x+t+2{\sqrt {xt}}\cos \theta ){\frac {J_{\alpha -1/2}({\sqrt {xt}}\sin \theta )}{[({\sqrt {xt}}\sin \theta )/2]^{\alpha -1/2}}}d\theta \,}{\displaystyle {\tilde {f}}_{\alpha }(n){\tilde {g}}_{\alpha }(n)}[6]


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 Metasyntactic variable, which is released under the 
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