Understanding the Equivalence of Dirac Delta Functions in Quantum Mechanics

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SUMMARY

The Dirac delta function, developed by Paul Dirac in the context of quantum mechanics, is a distribution that can be defined through its interaction with Schwartz functions. In the theory of tempered distributions, two distributions are considered equivalent if they yield the same result when convolved with Schwartz functions. Specifically, if a distribution g satisfies the integral relation ∫ g(x) f(x) dx = f(0) for all Schwartz functions f, then g is equivalent to the Dirac delta distribution. This equivalence is transitive, meaning if another distribution h also satisfies this condition, then g equals h.

PREREQUISITES
  • Understanding of Dirac delta functions in quantum mechanics
  • Familiarity with tempered distributions
  • Knowledge of Schwartz functions
  • Basic calculus, particularly integral calculus
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  • Study the properties of tempered distributions in detail
  • Learn about the convolution of distributions and its applications
  • Explore the role of Schwartz functions in mathematical physics
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Physicists, mathematicians, and students of quantum mechanics who seek a deeper understanding of the Dirac delta function and its equivalences in the framework of tempered distributions.

Mike2
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Dirac developed his delta function in the context of QM. But there are various functions under the integral that give the delta function. My question is does one Dirac delta function equal any other? Are all ways of getting the Dirac delta function equivalent? Thanks.
 
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In the theory of tempered distributions (which is one way to formalize the Dirac delta function), the identity of a distribution is entirely determined by the results you get by convolving it with Schwartz functions.

Therefore, if you compute a distribution g that satisfies the relation2
[tex]\int_{-\infty}^{+\infty} g(x) f(x) \, dx = f(0)[/tex]
for every Schwartz function f, then g is equal to the Dirac delta distribution1. And equality is transitive: if you compute another distribution h that also satisfies that relation, then g = h.


1: I will use this name, since the Dirac delta isn't a function
2: Note that this integral is a generalization of what you learned in calculus. In particular, it's not defined as a limit of Riemann sums.
 
Last edited:
DDFs can be defined in terms of a restricted class of functions f in Herky's integral. If the f's are different, the DDFs could be dlfferent.
 

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