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Coulomb wave functions

Table of contents: Definitions - Differential equations - Connection formulas - Normalization functions - Derivatives - Hypergeometric representations

Definitions

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Symbol: CoulombF — Fℓ,η ⁣(z)F_{\ell,\eta}\!\left(z\right) — Regular Coulomb wave function
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Symbol: CoulombG — Gℓ,η ⁣(z)G_{\ell,\eta}\!\left(z\right) — Irregular Coulomb wave function
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Symbol: CoulombH — Hℓ,ηω ⁣(z)H^{\omega}_{\ell,\eta}\!\left(z\right) — Outgoing and ingoing Coulomb wave function
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Symbol: CoulombC — Cℓ ⁣(η)C_{\ell}\!\left(\eta\right) — Coulomb wave function Gamow factor
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Symbol: CoulombSigma — σℓ ⁣(η)\sigma_{\ell}\!\left(\eta\right) — Coulomb wave function phase shift

Differential equations

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y′′(z)+(1−2ηz−ℓ(ℓ+1)z2)y(z)=0   where y(z)=c1Fℓ,η ⁣(z)+c2Gℓ,η ⁣(z)y''(z) + \left(1 - \frac{2 \eta}{z} - \frac{\ell \left(\ell + 1\right)}{{z}^{2}}\right) y(z) = 0\; \text{ where } y(z) = {c}_{1} F_{\ell,\eta}\!\left(z\right) + {c}_{2} G_{\ell,\eta}\!\left(z\right)
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Gℓ,η ⁣(z)(ddz Fℓ,η ⁣(z))−(ddz Gℓ,η ⁣(z))Fℓ,η ⁣(z)=1G_{\ell,\eta}\!\left(z\right) \left(\frac{d}{d z}\, F_{\ell,\eta}\!\left(z\right)\right) - \left(\frac{d}{d z}\, G_{\ell,\eta}\!\left(z\right)\right) F_{\ell,\eta}\!\left(z\right) = 1

Connection formulas

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Fℓ,η ⁣(z)=Hℓ,η+ ⁣(z)−Hℓ,η− ⁣(z)2iF_{\ell,\eta}\!\left(z\right) = \frac{H^{+}_{\ell,\eta}\!\left(z\right) - H^{-}_{\ell,\eta}\!\left(z\right)}{2 i}
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Gℓ,η ⁣(z)=Hℓ,η+ ⁣(z)+Hℓ,η− ⁣(z)2G_{\ell,\eta}\!\left(z\right) = \frac{H^{+}_{\ell,\eta}\!\left(z\right) + H^{-}_{\ell,\eta}\!\left(z\right)}{2}
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Hℓ,ηω ⁣(z)=Gℓ,η ⁣(z)+ωiFℓ,η ⁣(z)H^{\omega}_{\ell,\eta}\!\left(z\right) = G_{\ell,\eta}\!\left(z\right) + \omega i F_{\ell,\eta}\!\left(z\right)
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Gℓ,η ⁣(z)=Fℓ,η ⁣(z)cos⁡(χ)−F−ℓ−1,η ⁣(z)sin⁡(χ)   where χ=σℓ ⁣(η)−σ−ℓ−1 ⁣(η)−(ℓ+12)πG_{\ell,\eta}\!\left(z\right) = \frac{F_{\ell,\eta}\!\left(z\right) \cos(\chi) - F_{-\ell - 1,\eta}\!\left(z\right)}{\sin(\chi)}\; \text{ where } \chi = \sigma_{\ell}\!\left(\eta\right) - \sigma_{-\ell - 1}\!\left(\eta\right) - \left(\ell + \frac{1}{2}\right) \pi
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Hℓ,ηω ⁣(z)=Fℓ,η ⁣(z)eωiχ−F−ℓ−1,η ⁣(z)sin⁡(χ)   where χ=σℓ ⁣(η)−σ−ℓ−1 ⁣(η)−(ℓ+12)πH^{\omega}_{\ell,\eta}\!\left(z\right) = \frac{F_{\ell,\eta}\!\left(z\right) {e}^{\omega i \chi} - F_{-\ell - 1,\eta}\!\left(z\right)}{\sin(\chi)}\; \text{ where } \chi = \sigma_{\ell}\!\left(\eta\right) - \sigma_{-\ell - 1}\!\left(\eta\right) - \left(\ell + \frac{1}{2}\right) \pi

Normalization functions

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Cℓ ⁣(η)=2ℓΓ ⁣(2ℓ+2)exp⁡ ⁣(log⁡Γ ⁣(1+ℓ+iη)+log⁡Γ ⁣(1+ℓ−iη)−πη2)C_{\ell}\!\left(\eta\right) = \frac{{2}^{\ell}}{\Gamma\!\left(2 \ell + 2\right)} \exp\!\left(\frac{\log \Gamma\!\left(1 + \ell + i \eta\right) + \log \Gamma\!\left(1 + \ell - i \eta\right) - \pi \eta}{2}\right)
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σℓ ⁣(η)=log⁡Γ ⁣(1+ℓ+iη)−log⁡Γ ⁣(1+ℓ−iη)2i\sigma_{\ell}\!\left(\eta\right) = \frac{\log \Gamma\!\left(1 + \ell + i \eta\right) - \log \Gamma\!\left(1 + \ell - i \eta\right)}{2 i}

Derivatives

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ddz Fℓ,η ⁣(z)=(ℓ+1z+ηℓ+1)Fℓ,η ⁣(z)−1+ℓ+iη1+ℓ−iηℓ+1Fℓ+1,η ⁣(z)\frac{d}{d z}\, F_{\ell,\eta}\!\left(z\right) = \left(\frac{\ell + 1}{z} + \frac{\eta}{\ell + 1}\right) F_{\ell,\eta}\!\left(z\right) - \frac{\sqrt{1 + \ell + i \eta} \sqrt{1 + \ell - i \eta}}{\ell + 1} F_{\ell + 1,\eta}\!\left(z\right)
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ddz Gℓ,η ⁣(z)=(ℓ+1z+ηℓ+1)Gℓ,η ⁣(z)−1+ℓ+iη1+ℓ−iηℓ+1Gℓ+1,η ⁣(z)\frac{d}{d z}\, G_{\ell,\eta}\!\left(z\right) = \left(\frac{\ell + 1}{z} + \frac{\eta}{\ell + 1}\right) G_{\ell,\eta}\!\left(z\right) - \frac{\sqrt{1 + \ell + i \eta} \sqrt{1 + \ell - i \eta}}{\ell + 1} G_{\ell + 1,\eta}\!\left(z\right)
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f′′(z)=(2ηz+ℓ(ℓ+1)z2−1)f(z)   where f(z)=c1Fℓ,η ⁣(z)+c2Gℓ,η ⁣(z)f''(z) = \left(\frac{2 \eta}{z} + \frac{\ell \left(\ell + 1\right)}{{z}^{2}} - 1\right) f(z)\; \text{ where } f(z) = {c}_{1} F_{\ell,\eta}\!\left(z\right) + {c}_{2} G_{\ell,\eta}\!\left(z\right)
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f′′′(z)=(2ηz+ℓ(ℓ+1)z2−1)f′(z)−2(ηz2+ℓ(ℓ+1)z3)f(z)   where f(z)=c1Fℓ,η ⁣(z)+c2Gℓ,η ⁣(z)f'''(z) = \left(\frac{2 \eta}{z} + \frac{\ell \left(\ell + 1\right)}{{z}^{2}} - 1\right) f'(z) - 2 \left(\frac{\eta}{{z}^{2}} + \frac{\ell \left(\ell + 1\right)}{{z}^{3}}\right) f(z)\; \text{ where } f(z) = {c}_{1} F_{\ell,\eta}\!\left(z\right) + {c}_{2} G_{\ell,\eta}\!\left(z\right)
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f(r+4)(z)(r+4)!=−1z2(r2+7r+12)(2(r2+5r+6)zf(r+3)(z)(r+3)!+(r2+3r+z2−2zη−ℓ(ℓ+1)+2)f(r+2)(z)(r+2)!+2(z−η)f(r+1)(z)(r+1)!+f(r)(z)r!)   where f(z)=c1Fℓ,η ⁣(z)+c2Gℓ,η ⁣(z)\frac{{f}^{(r + 4)}(z)}{\left(r + 4\right)!} = -\frac{1}{{z}^{2} \left({r}^{2} + 7 r + 12\right)} \left(2 \left({r}^{2} + 5 r + 6\right) z \frac{{f}^{(r + 3)}(z)}{\left(r + 3\right)!} + \left({r}^{2} + 3 r + {z}^{2} - 2 z \eta - \ell \left(\ell + 1\right) + 2\right) \frac{{f}^{(r + 2)}(z)}{\left(r + 2\right)!} + 2 \left(z - \eta\right) \frac{{f}^{(r + 1)}(z)}{\left(r + 1\right)!} + \frac{{f}^{(r)}(z)}{r !}\right)\; \text{ where } f(z) = {c}_{1} F_{\ell,\eta}\!\left(z\right) + {c}_{2} G_{\ell,\eta}\!\left(z\right)

Hypergeometric representations

Kummer function

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Fℓ,η ⁣(z)=Cℓ ⁣(η)zℓ+1eωiz 1F1 ⁣(1+ℓ+ωiη,2ℓ+2,−2ωiz)F_{\ell,\eta}\!\left(z\right) = C_{\ell}\!\left(\eta\right) {z}^{\ell + 1} {e}^{\omega i z} \,{}_1F_1\!\left(1 + \ell + \omega i \eta, 2 \ell + 2, -2 \omega i z\right)
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Fℓ,η ⁣(z)=2ℓexp⁡ ⁣(log⁡Γ ⁣(1+ℓ+iη)+log⁡Γ ⁣(1+ℓ−iη)−πη2)zℓ+1eωiz 1F1 ⁣(1+ℓ+ωiη,2ℓ+2,−2ωiz)F_{\ell,\eta}\!\left(z\right) = {2}^{\ell} \exp\!\left(\frac{\log \Gamma\!\left(1 + \ell + i \eta\right) + \log \Gamma\!\left(1 + \ell - i \eta\right) - \pi \eta}{2}\right) {z}^{\ell + 1} {e}^{\omega i z} \,{}_1{\textbf F}_1\!\left(1 + \ell + \omega i \eta, 2 \ell + 2, -2 \omega i z\right)

Tricomi function

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Fℓ,η ⁣(z)=2ℓzℓ+1exp⁡ ⁣(log⁡Γ(u)+log⁡Γ(v)−πη2)(eizU∗ ⁣(u,2ℓ+2,−2iz)(2iz)uΓ(v)+e−izU∗ ⁣(v,2ℓ+2,2iz)(−2iz)vΓ(u))   where u=1+ℓ+iη,  v=1+ℓ−iηF_{\ell,\eta}\!\left(z\right) = {2}^{\ell} {z}^{\ell + 1} \exp\!\left(\frac{\log \Gamma(u) + \log \Gamma(v) - \pi \eta}{2}\right) \left(\frac{{e}^{i z} U^{*}\!\left(u, 2 \ell + 2, -2 i z\right)}{{\left(2 i z\right)}^{u} \Gamma(v)} + \frac{{e}^{-i z} U^{*}\!\left(v, 2 \ell + 2, 2 i z\right)}{{\left(-2 i z\right)}^{v} \Gamma(u)}\right)\; \text{ where } u = 1 + \ell + i \eta,\;v = 1 + \ell - i \eta
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Gℓ,η ⁣(z)=12((2z)−iηexp⁡ ⁣(i(z−ℓπ2+σℓ ⁣(η)))U∗ ⁣(1+ℓ+iη,2ℓ+2,−2iz)+(2z)iηexp⁡ ⁣(−i(z−ℓπ2+σℓ ⁣(η)))U∗ ⁣(1+ℓ−iη,2ℓ+2,2iz))G_{\ell,\eta}\!\left(z\right) = \frac{1}{2} \left({\left(2 z\right)}^{-i \eta} \exp\!\left(i \left(z - \frac{\ell \pi}{2} + \sigma_{\ell}\!\left(\eta\right)\right)\right) U^{*}\!\left(1 + \ell + i \eta, 2 \ell + 2, -2 i z\right) + {\left(2 z\right)}^{i \eta} \exp\!\left(-i \left(z - \frac{\ell \pi}{2} + \sigma_{\ell}\!\left(\eta\right)\right)\right) U^{*}\!\left(1 + \ell - i \eta, 2 \ell + 2, 2 i z\right)\right)
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Gℓ,η ⁣(z)=(2z)−iηexp⁡ ⁣(i(z−ℓπ2+σℓ ⁣(η)))U∗ ⁣(1+ℓ+iη,2ℓ+2,−2iz)−iFℓ,η ⁣(z)G_{\ell,\eta}\!\left(z\right) = {\left(2 z\right)}^{-i \eta} \exp\!\left(i \left(z - \frac{\ell \pi}{2} + \sigma_{\ell}\!\left(\eta\right)\right)\right) U^{*}\!\left(1 + \ell + i \eta, 2 \ell + 2, -2 i z\right) - i F_{\ell,\eta}\!\left(z\right)
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Gℓ,η ⁣(z)=(2z)iηexp⁡ ⁣(−i(z−ℓπ2+σℓ ⁣(η)))U∗ ⁣(1+ℓ−iη,2ℓ+2,2iz)+iFℓ,η ⁣(z)G_{\ell,\eta}\!\left(z\right) = {\left(2 z\right)}^{i \eta} \exp\!\left(-i \left(z - \frac{\ell \pi}{2} + \sigma_{\ell}\!\left(\eta\right)\right)\right) U^{*}\!\left(1 + \ell - i \eta, 2 \ell + 2, 2 i z\right) + i F_{\ell,\eta}\!\left(z\right)
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Hℓ,η+ ⁣(z)=(2z)−iηexp⁡ ⁣(i(z−ℓπ2+σℓ ⁣(η)))U∗ ⁣(1+ℓ+iη,2ℓ+2,−2iz)H^{+}_{\ell,\eta}\!\left(z\right) = {\left(2 z\right)}^{-i \eta} \exp\!\left(i \left(z - \frac{\ell \pi}{2} + \sigma_{\ell}\!\left(\eta\right)\right)\right) U^{*}\!\left(1 + \ell + i \eta, 2 \ell + 2, -2 i z\right)
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Hℓ,η+ ⁣(z)=(2z)iηexp⁡ ⁣(−i(z−ℓπ2+σℓ ⁣(η)))U∗ ⁣(1+ℓ−iη,2ℓ+2,2iz)+2iFℓ,η ⁣(z)H^{+}_{\ell,\eta}\!\left(z\right) = {\left(2 z\right)}^{i \eta} \exp\!\left(-i \left(z - \frac{\ell \pi}{2} + \sigma_{\ell}\!\left(\eta\right)\right)\right) U^{*}\!\left(1 + \ell - i \eta, 2 \ell + 2, 2 i z\right) + 2 i F_{\ell,\eta}\!\left(z\right)
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Hℓ,η− ⁣(z)=(2z)iηexp⁡ ⁣(−i(z−ℓπ2+σℓ ⁣(η)))U∗ ⁣(1+ℓ−iη,2ℓ+2,2iz)H^{-}_{\ell,\eta}\!\left(z\right) = {\left(2 z\right)}^{i \eta} \exp\!\left(-i \left(z - \frac{\ell \pi}{2} + \sigma_{\ell}\!\left(\eta\right)\right)\right) U^{*}\!\left(1 + \ell - i \eta, 2 \ell + 2, 2 i z\right)
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Hℓ,η− ⁣(z)=(2z)−iηexp⁡ ⁣(i(z−ℓπ2+σℓ ⁣(η)))U∗ ⁣(1+ℓ+iη,2ℓ+2,−2iz)−2iFℓ,η ⁣(z)H^{-}_{\ell,\eta}\!\left(z\right) = {\left(2 z\right)}^{-i \eta} \exp\!\left(i \left(z - \frac{\ell \pi}{2} + \sigma_{\ell}\!\left(\eta\right)\right)\right) U^{*}\!\left(1 + \ell + i \eta, 2 \ell + 2, -2 i z\right) - 2 i F_{\ell,\eta}\!\left(z\right)

Copyright (C) Fredrik Johansson and contributors. Fungrim is provided under the MIT license. The source code is on GitHub.

2021-03-15 19:12:00.328586 UTC