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eigenvector

   Also found in: Dictionary/thesaurus, Acronyms, Wikipedia 0.04 sec.
eigenvector [′ī·gən‚vek·tər]
(mathematics)
A nonzero vectorvwhose direction is not changed by a given linear transformationT; that is,T(v) = λvfor some scalar λ. Also known as characteristic vector.

(mathematics)eigenvector - A vector which, when acted on by a particular linear transformation, produces a scalar multiple of the original vector. The scalar in question is called the eigenvalue corresponding to this eigenvector.

It should be noted that "vector" here means "element of a vector space" which can include many mathematical entities. Ordinary vectors are elements of a vector space, and multiplication by a matrix is a linear transformation on them; smooth functions "are vectors", and many partial differential operators are linear transformations on the space of such functions; quantum-mechanical states "are vectors", and observables are linear transformations on the state space.

An important theorem says, roughly, that certain linear transformations have enough eigenvectors that they form a basis of the whole vector states. This is why Fourier analysis works, and why in quantum mechanics every state is a superposition of eigenstates of observables.

An eigenvector is a (representative member of a) fixed point of the map on the projective plane induced by a linear map.


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The book provides guidance not only on systems of linear equations and matrix algebra but also on the often-harder-to-grasp topics of vector spaces, linear transformations, determinants, and eigenvector problems.
Property 4 If the sum of the entries of each row in A is equal to the same number k, then k itself is an eigenvalue that corresponds to the eigenvector [1; 1; .
First, introduce the Green's tensor and take its Fourier transform in time and space; then, expand the transformed Green's tensor according to the eigenvector of the Christoffel matrix, and decompose the fields into downgoing waves and upgoing waves; third, use boundary conditions to interatively get the solution in the transform domain in a form of "generalized ray" series; finally, use the Willis inversion technique to get the solution.
 
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