In the physicists' Hermite polynomial convention, begin by differentiating the Gaussian function:
The defining prefactor then gives
The derivative-based definition uses nonnegative integers; negative orders are not part of this polynomial definition.
Let , so . Differentiate this identity times, for . By the Leibniz rule, only the first two derivatives of the linear factor can contribute:
Rearranging proves
The case is the starting identity , treated separately without introducing a negative derivative order.
Differentiate the product in the definition of . Using the identity in (b),
The last expression is , so
Also separately. This is the Hermite polynomial derivative recurrence in the physicists' normalization.

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