Differential Operator
The operator representing the computation of a derivative,
|
(1)
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sometimes also called the Newton-Leibniz operator. The second derivative is then denoted ,
the third
,
etc. The integral is denoted
.
The differential operator satisfies the identity
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(2)
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where
is a Hermite polynomial (Arfken 1985, p. 718),
where the first few cases are given explicitly by
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(3)
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(4)
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(5)
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(6)
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(7)
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(8)
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The symbol
can be used to denote the operator
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(9)
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(Bailey 1935, p. 8). A fundamental identity for this operator is given by
|
(10)
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where
is a Stirling number of the second
kind (Roman 1984, p. 144), giving
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(11)
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(12)
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(13)
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(14)
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and so on (OEIS A008277). Special cases include
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(15)
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(16)
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(17)
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A shifted version of the identity is given by
|
(18)
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(Roman 1984, p. 146).
See also
Convective Derivative, Derivative, Fractional Derivative, GradientExplore with Wolfram|Alpha
References
Arfken, G. Mathematical Methods for Physicists, 3rd ed. Orlando, FL: Academic Press, 1985.Bailey, W. N. Generalised Hypergeometric Series. Cambridge, England: University Press, 1935.Roman, S. The Umbral Calculus. New York: Academic Press, pp. 59-63, 1984.Sloane, N. J. A. Sequence A008277 in "The On-Line Encyclopedia of Integer Sequences."Referenced on Wolfram|Alpha
Differential OperatorCite this as:
Weisstein, Eric W. "Differential Operator." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/DifferentialOperator.html