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Mathematical integral From Wikipedia, the free encyclopedia
In mathematics, the complete Fermi–Dirac integral, named after Enrico Fermi and Paul Dirac, for an index j is defined by
This equals
where is the polylogarithm.
Its derivative is
and this derivative relationship is used to define the Fermi-Dirac integral for nonpositive indices j. Differing notation for appears in the literature, for instance some authors omit the factor . The definition used here matches that in the NIST DLMF.
The closed form of the function exists for j = 0:
For x = 0, the result reduces to
where is the Dirichlet eta function.
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