Laplace's method
Asymptotic evaluation of integrals dominated by a single interior maximizer of the exponent.
Laplace’s method
Laplace’s method approximates integrals of the form
for large , when the main contribution comes from a neighborhood of the point where is maximal. It is the real-variable analogue of the complex saddle-point-method .
One-dimensional interior-maximum theorem
Assume:
- is twice continuously differentiable on and has a unique maximizer ,
- ,
- is continuous at and .
Then as ,
More refined expansions are obtained by keeping higher-order terms of the local Taylor expansion.
Sketch of why it works
Near the maximizer , expand using a second-order Taylor approximation:
For large , the factor is sharply peaked at , and the integral is well-approximated by replacing the exponent with its quadratic part and extending the local integral to all of , yielding a Gaussian integral.
Multidimensional version (informal)
For ,
if has a unique interior maximizer with negative definite Hessian , then typically
Common variants and caveats
- If the maximum occurs at an endpoint ( or ), the leading order usually changes (often to an -type scale rather than ).
- If there are multiple maximizers, the leading term is typically the sum of contributions from each (when they are well-separated and nondegenerate).
- If (degenerate maximum), the scale becomes for some determined by the first nonzero derivative at .
Where it shows up
- Normal approximations and local limit behavior.
- Large- asymptotics of combinatorial sums via integral representations.
- As the real-variable building block for the complex steepest-descent/saddle-point techniques (see saddle-point-method ).