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In [[mathematical analysis]], a '''Hermitian function''' is a [[complex number|complex]] [[function (mathematics)|function]] with the property that its [[complex conjugate]] is equal to the original function with the variable changed in [[sign (mathematics)|sign]]: | |||
:<math>f(-x) = \overline{f(x)}</math> | |||
for all <math>x</math> in the domain of <math>f</math>. | |||
This definition extends also to functions of two or more variables, e.g., in the case that <math>f</math> is a function of two variables it is Hermitian if | |||
:<math>f(-x_1, -x_2) = \overline{f(x_1, x_2)}</math> | |||
for all pairs <math>(x_1, x_2)</math> in the domain of <math>f</math>. | |||
From this definition it follows immediately that, if <math>f</math> is a Hermitian function, then | |||
* the real part of <math>f</math> is an [[even function]] | |||
* the imaginary part of <math>f</math> is an [[odd function]] | |||
== Motivation == | |||
Hermitian functions appear frequently in mathematics, physics, and signal processing. For example, the following two statements follow from basic properties of the Fourier transform: | |||
* The function <math>f</math> is real-valued if and only if the [[Fourier transform]] of <math>f</math> is Hermitian. | |||
* The function <math>f</math> is Hermitian if and only if the [[Fourier transform]] of <math>f</math> is real-valued. | |||
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. | |||
* If ''f'' is Hermitian, then <math>f \star g = f*g</math> | |||
Where the <math> \star </math> is [[cross-correlation]], and <math> * </math> is [[convolution]]. | |||
* If both ''f'' and ''g'' are Hermitian, then <math>f \star g = g \star f</math>, which in general is not true. | |||
<!--------An example wanted for these two statements above! -------> | |||
== See also == | |||
* [[Even and odd functions]] | |||
[[Category:Types of functions]] | |||
[[Category:Calculus]] | |||
{{mathanalysis-stub}} |
Revision as of 12:19, 7 April 2013
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:
This definition extends also to functions of two or more variables, e.g., in the case that is a function of two variables it is Hermitian if
for all pairs in the domain of .
From this definition it follows immediately that, if is a Hermitian function, then
- the real part of is an even function
- the imaginary part of is an odd function
Motivation
Hermitian functions appear frequently in mathematics, physics, and signal processing. For example, the following two statements follow from basic properties of the Fourier transform:
- The function is real-valued if and only if the Fourier transform of is Hermitian.
- The function is Hermitian if and only if the Fourier transform of is real-valued.
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.
Where the is cross-correlation, and is convolution.