DLMF:33.17.E2 (Q9652)

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DLMF:33.17.E2
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    ( + 1 ) ( 1 + 2 ϵ ) r h ( ϵ , - 1 ; r ) - ( 2 + 1 ) ( ( + 1 ) - r ) h ( ϵ , ; r ) + r h ( ϵ , + 1 ; r ) = 0 , 1 1 superscript 2 italic-ϵ 𝑟 Coulomb-h italic-ϵ 1 𝑟 2 1 1 𝑟 Coulomb-h italic-ϵ 𝑟 𝑟 Coulomb-h italic-ϵ 1 𝑟 0 {\displaystyle{\displaystyle(\ell+1)\left(1+\ell^{2}\epsilon\right)rh\left(% \epsilon,\ell-1;r\right)-(2\ell+1)\left(\ell(\ell+1)-r\right)h\left(\epsilon,% \ell;r\right)+\ell rh\left(\epsilon,\ell+1;r\right)=0,}}
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    DLMF:33.17.E2
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    h ( ϵ , ; r ) Coulomb-h italic-ϵ 𝑟 {\displaystyle{\displaystyle h\left(\NVar{\epsilon},\NVar{\ell};\NVar{r}\right% )}}
    C33.S14.E7.m2adec
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