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MATH
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Definitions from Eigenvalues and eigenvectors

All definitions from Eigenvalues and eigenvectors.

Eigenvalue

Let T:V→VT:V\to V be a linear map over a field FF. A scalar λ∈F\lambda\in F is an eigenvalue of TT if there is a non-zero vector v∈Vv\in V such that

T(v)=λv.T(v)=\lambda v.

The equation says that the line through vv is mapped into itself, with every vector on that line scaled by λ\lambda. A negative real λ\lambda reverses direction and λ=0\lambda=0 collapses the line to the origin. For a matrix AA, the same condition is

Av=λv.Av=\lambda v.

Eigenvector

If T(v)=λvT(v)=\lambda v for a non-zero vector vv, then vv is an eigenvector of TT corresponding to the eigenvalue λ\lambda.

The zero vector is excluded because T(0)=λ0T(0)=\lambda 0 holds for every scalar, so it says nothing about a direction. Any non-zero scalar multiple of an eigenvector is another eigenvector for the same eigenvalue.

Eigenspace

For A∈Mn(F)A\in M_n(F) and an eigenvalue λ∈F\lambda\in F, the eigenspace corresponding to λ\lambda is

Eλ=ker⁡F(A−λI).E_\lambda=\ker_F(A-\lambda I).

Its non-zero vectors are precisely the eigenvectors of AA corresponding to λ\lambda.

To find the eigenspace, solve the homogeneous system

(A−λI)v=0.(A-\lambda I)v=0.

The kernel description makes the eigenspace a subspace, so it contains the zero vector even though the zero vector is not an eigenvector.

Characteristic polynomial

For an n×nn\times n matrix AA over FF, the characteristic polynomial is

pA(λ)=det⁡(A−λI).p_A(\lambda)=\det(A-\lambda I).

The equation pA(λ)=0p_A(\lambda)=0 is the associated characteristic equation.

The characteristic polynomial turns the search for a non-zero solution of (A−λI)v=0(A-\lambda I)v=0 into root-finding over the chosen field. A polynomial with no roots in FF may gain roots when the scalars are extended, for example from R\mathbb R to C\mathbb C.

Some texts define the polynomial as det⁡(λI−A)\det(\lambda I-A) instead. For an n×nn\times n matrix this is (−1)npA(λ)(-1)^n p_A(\lambda), so both conventions give the same eigenvalues.

Two names clash with Calculus. The characteristic equation of a scalar ODE is a different object with the same name. In constrained extrema, the letter λ\lambda denotes a Lagrange multiplier rather than an eigenvalue.

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