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Type of complex function
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In mathematical analysis, a Hermitian function is a complex function with the property that its complex conjugate is equal to the original function with the variable changed in sign:

πŸ‘ {\displaystyle f^{*}(x)=f(-x)}

(where the πŸ‘ {\displaystyle ^{*}}
indicates the complex conjugate) for all πŸ‘ {\displaystyle x}
in the domain of πŸ‘ {\displaystyle f}
. In physics, this property is referred to as PT symmetry.

This definition extends also to functions of two or more variables, e.g., in the case that πŸ‘ {\displaystyle f}
is a function of two variables it is Hermitian if

πŸ‘ {\displaystyle f^{*}(x_{1},x_{2})=f(-x_{1},-x_{2})}

for all pairs πŸ‘ {\displaystyle (x_{1},x_{2})}
in the domain of πŸ‘ {\displaystyle f}
.

From this definition it follows immediately that: πŸ‘ {\displaystyle f}
is a Hermitian function if and only if

Motivation

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Hermitian functions appear frequently in mathematics, physics, and signal processing. For example, the following two statements follow from basic properties of the Fourier transform:[citation needed]

Since the Fourier transform of a real signal is guaranteed to be Hermitian, it can be compressed using the Hermitian even/odd symmetry. This, for example, allows the discrete Fourier transform of a signal (which is in general complex) to be stored in the same space as the original real signal. Informally, only half of the fourier transform of a real signal is needed to lossessly represent it in frequency domain.

For the magnitude spectra (obtained from DFT), the axis of symmetry is around the Nyquist point; one half is the mirror image of the other.

Where the πŸ‘ {\displaystyle \star }
is cross-correlation, and πŸ‘ {\displaystyle *}
is convolution.

See also

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