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  "body": "\n## Summary\n\nThe Whittaker functions $M_{\\kappa, \\mu}(z)$ and $W_{\\kappa, \\mu}(z)$ are solutions of Whittaker's equation $w'' + \\left( -\\frac14 + \\frac{\\kappa}{z} + \\frac{\\frac14 - \\mu^2}{z^2} \\right) w = 0$.\nThey are the [[confluent hypergeometric functions|6AZ4ZBN1M8]] rewritten so that the equation has no first derivative term.\nThis normal form is convenient in physics and in asymptotic analysis, and it makes the symmetry $\\mu \\mapsto -\\mu$ visible.\n\n## Explanations\n\n### L1 human\n\nKummer's equation has a first derivative term; multiplying the unknown by $e^{-z/2} z^{b/2}$ removes it.\nThe result is Whittaker's equation, which looks like a Schrödinger equation with a constant, a Coulomb-type term $\\kappa / z$ and a centrifugal-type term $(\\frac14 - \\mu^2)/z^2$.\nThe function $M_{\\kappa, \\mu}$ is the solution that behaves like $z^{\\mu + 1/2}$ near $0$, and $W_{\\kappa, \\mu}$ is the solution that decays like $e^{-z/2} z^{\\kappa}$ at $+\\infty$.\nA simple case is $W_{0, 1/2}(z) = e^{-z/2}$, which indeed satisfies $w'' - \\frac14 w = 0$.\n",
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