Gaussian Function - Multi-dimensional Gaussian Function

Multi-dimensional Gaussian Function

In an -dimensional space a Gaussian function can be defined as


f(x) = \exp(-x^TAx) \;,

where is a column of coordinates, is a positive-definite matrix, and denotes transposition.

The integral of a Gaussian function over the whole -dimensional space is given as


\int_{\mathbb{R}^n}\exp(-x^TBx)dx = \sqrt{\frac{\pi^n}{\det{B}}} \;.

It can be easily calculated by diagonalizing the matrix and changing the integration variables to the eigenvectors of .

More generally a shifted Gaussian function is defined as


f(x) = \exp(-x^TAx+s^Tx) \;,

where is the shift vector and the matrix can be assumed to be symmetric, . The following integrals with this function can be calculated with the same technique,


\int d^nx e^{-x^TBx+v^Tx} = \sqrt{\frac{\pi^n}{\det{B}}} \exp(\frac{1}{4}v^TB^{-1}v)\equiv \mathcal{M}\;.

\int d^n x e^{- x^T B x + v^T x} \left( a^T x \right) = (a^T u) \cdot
\mathcal{M}\;,\; {\rm where}\;
u = \frac{1}{2} B^{- 1} v \;.

\int d^n x e^{- x^T B x + v^T x} \left( x^T D x \right) = \left( u^T D u +
\frac{1}{2} {\rm tr} (D B^{- 1}) \right) \cdot \mathcal{M}\;.

\begin{align}
& \int d^n x e^{- x^T A' x + s'^T x} \left( -
\frac{\partial}{\partial x} \Lambda \frac{\partial}{\partial x} \right) e^{-
x^T A x + s^T x} = \\
& = \left( 2 {\rm tr} (A' \Lambda A B^{- 1}) + 4 u^T A' \Lambda A u - 2 u^T
(A' \Lambda s + A \Lambda s') + s'^T \Lambda s \right) \cdot \mathcal{M}\;,
\\ & {\rm where} \;
u = \frac{1}{2} B^{- 1} v, v = s + s', B = A + A' \;.
\end{align}

Read more about this topic:  Gaussian Function

Famous quotes containing the word function:

    Philosophical questions are not by their nature insoluble. They are, indeed, radically different from scientific questions, because they concern the implications and other interrelations of ideas, not the order of physical events; their answers are interpretations instead of factual reports, and their function is to increase not our knowledge of nature, but our understanding of what we know.
    Susanne K. Langer (1895–1985)