The Dirac delta function, also known as the unit impulse, is a generalized function on the real numbers whose value is zero everywhere except at zero, where it is infinite, with the property that its integral over the whole real line equals one. Because no ordinary function actually has this property, the delta function is modeled rigorously using limits or, more commonly in mathematics, measure theory and the theory of distributions developed by Laurent Schwartz. It is named after the physicist Paul Dirac and is applied routinely in physics and engineering to model point masses and concentrated loads; its name reflects its role as a continuous analogue of the discrete Kronecker delta.
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Source Wikipedia: Dirac delta function
Source Wikipedia: Dirac delta function
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Source Wikipedia: Dirac delta function
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Paul Dirac introduced the delta-function in a 1927 paper, subsequently popularized in his 1930 book The Principles of Quantum Mechanics.
Introduction, opening sentence
is a generalized function on the real numbers, whose value is zero everywhere except at zero, where it is infinite.
- In Branch: Analysis, Lead sentence
Attributed To: Paul Dirac, Lead
The delta function is named after physicist Paul Dirac, and has been applied routinely in physics and engineering to model point masses and concentrated loads
Attributed To: Laurent Schwartz, Lead
The mathematical rigor of the delta function was disputed until Laurent Schwartz developed the theory of distributions, where it is defined as a linear form acting on functions.
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