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Moreover, if the entire vector space V can be spanned by the eigenvectors of T, or equivalently if the direct sum of the eigenspaces associated with all the eigenvalues of T is the entire vector space V, then a basis of V called an eigenbasis can be formed from linearly independent eigenvectors of T.
Given an n × n square matrix A of real or complex numbers, an eigenvalue λ and its associated generalized eigenvector v are a pair obeying the relation [1] =,where v is a nonzero n × 1 column vector, I is the n × n identity matrix, k is a positive integer, and both λ and v are allowed to be complex even when A is real.l When k = 1, the vector is called simply an eigenvector, and the pair ...
Once the eigenvalues are computed, the eigenvectors could be calculated by solving the equation (), = using Gaussian elimination or any other method for solving matrix equations. However, in practical large-scale eigenvalue methods, the eigenvectors are usually computed in other ways, as a byproduct of the eigenvalue computation.
For example, if has real-valued elements, then it may be necessary for the eigenvalues and the components of the eigenvectors to have complex values. [ 35 ] [ 36 ] [ 37 ] The set spanned by all generalized eigenvectors for a given λ {\displaystyle \lambda } forms the generalized eigenspace for λ {\displaystyle \lambda } .
Let be the vector space spanned by the eigenvectors of which correspond to a negative eigenvalue and analogously for the positive eigenvalues. If a ∈ W s {\displaystyle a\in W^{s}} then lim t → ∞ x ( t ) = 0 {\displaystyle {\mbox{lim}}_{t\rightarrow \infty }x(t)=0} ; that is, the equilibrium point 0 is attractive to x ( t ) {\displaystyle ...
In numerical linear algebra, the Arnoldi iteration is an eigenvalue algorithm and an important example of an iterative method.Arnoldi finds an approximation to the eigenvalues and eigenvectors of general (possibly non-Hermitian) matrices by constructing an orthonormal basis of the Krylov subspace, which makes it particularly useful when dealing with large sparse matrices.
In mathematics, power iteration (also known as the power method) is an eigenvalue algorithm: given a diagonalizable matrix, the algorithm will produce a number , which is the greatest (in absolute value) eigenvalue of , and a nonzero vector , which is a corresponding eigenvector of , that is, =.
In the easiest case =, the matrix turns into a unit column-vector , the matrix is a scalar that is equal to the Rayleigh quotient = /, the only = solution to the eigenvalue problem is = and = (), and the only one Ritz vector is itself.