User:IssaRice/Linear algebra/Classification of operators: Difference between revisions
No edit summary |
No edit summary |
||
| Line 3: | Line 3: | ||
{| class="sortable wikitable" | {| class="sortable wikitable" | ||
|- | |- | ||
! Operator kind !! Description in terms of eigenvectors !! Description in terms of diagonalizability !! Notes !! Examples | ! Operator kind !! Description in terms of eigenvectors !! Description in terms of diagonalizability !! Geometric interpretation !! Notes !! Examples | ||
|- | |- | ||
| <math>T</math> is diagonalizable || There exists a basis of <math>V</math> consisting of eigenvectors of <math>T</math> || <math>T</math> is diagonalizable (there exists a basis <math>\beta</math> of <math>V</math> with respect to which <math>[T]_\beta^\beta</math> is a diagonal matrix) || This basis is not unique because we can reorder the vectors and also scale eigenvectors by a non-zero number to obtain an eigenvector. But there are at most <math>\dim V</math> distinct eigenvalues so the diagonal matrix should be unique up to order? || If <math>T</math> is the identity map, then every non-zero vector <math>v \in V</math> is an eigenvector of <math>T</math> with eigenvalue <math>1</math> because <math>Tv = 1v</math>. Thus every basis <math>\beta = (v_1,\ldots,v_n)</math> diagonalizes <math>T</math>. The matrix of <math>T</math> with respect to <math>\beta</math> is the identity matrix. | | <math>T</math> is diagonalizable || There exists a basis of <math>V</math> consisting of eigenvectors of <math>T</math> || <math>T</math> is diagonalizable (there exists a basis <math>\beta</math> of <math>V</math> with respect to which <math>[T]_\beta^\beta</math> is a diagonal matrix) || || This basis is not unique because we can reorder the vectors and also scale eigenvectors by a non-zero number to obtain an eigenvector. But there are at most <math>\dim V</math> distinct eigenvalues so the diagonal matrix should be unique up to order? || If <math>T</math> is the identity map, then every non-zero vector <math>v \in V</math> is an eigenvector of <math>T</math> with eigenvalue <math>1</math> because <math>Tv = 1v</math>. Thus every basis <math>\beta = (v_1,\ldots,v_n)</math> diagonalizes <math>T</math>. The matrix of <math>T</math> with respect to <math>\beta</math> is the identity matrix. | ||
|- | |- | ||
| <math>T</math> is normal || There exists an orthonormal basis of <math>V</math> consisting of eigenvectors of <math>T</math> || <math>T</math> is diagonalizable using an orthonormal basis | | <math>T</math> is normal || There exists an orthonormal basis of <math>V</math> consisting of eigenvectors of <math>T</math> || <math>T</math> is diagonalizable using an orthonormal basis || | ||
|- | |- | ||
| <math>T</math> self-adjoint (<math>T</math> is Hermitian) || There exists an orthonormal basis of <math>V</math> consisting of eigenvectors of <math>T</math> with real eigenvalues || <math>T</math> is diagonalizable using an orthonormal basis and the diagonal entries are all real | | <math>T</math> self-adjoint (<math>T</math> is Hermitian) || There exists an orthonormal basis of <math>V</math> consisting of eigenvectors of <math>T</math> with real eigenvalues || <math>T</math> is diagonalizable using an orthonormal basis and the diagonal entries are all real || | ||
|- | |- | ||
| <math>T</math> is an isometry || There exists an orthonormal basis of <math>V</math> consisting of eigenvectors of <math>T</math> whose eigenvalues all have absolute value 1 || <math>T</math> is diagonalizable using an orthonormal basis and the diagonal entries all have absolute values 1 || This only works when the field of scalars is the complex numbers | | <math>T</math> is an isometry || There exists an orthonormal basis of <math>V</math> consisting of eigenvectors of <math>T</math> whose eigenvalues all have absolute value 1 || <math>T</math> is diagonalizable using an orthonormal basis and the diagonal entries all have absolute values 1 || || This only works when the field of scalars is the complex numbers | ||
|- | |- | ||
| <math>T</math> is positive (positive semidefinite) || There exists an orthonormal basis of <math>V</math> consisting of eigenvectors of <math>T</math> with nonnegative real eigenvalues || <math>T</math> is diagonalizable using an orthonormal basis and the diagonal entries are all nonnegative real numbers | | <math>T</math> is positive (positive semidefinite) || There exists an orthonormal basis of <math>V</math> consisting of eigenvectors of <math>T</math> with nonnegative real eigenvalues || <math>T</math> is diagonalizable using an orthonormal basis and the diagonal entries are all nonnegative real numbers || | ||
|} | |} | ||
Revision as of 05:27, 17 January 2020
Let be a finite-dimensional inner product space, and let be a linear transformation. Then in the table below, the statements within the same row are equivalent.
| Operator kind | Description in terms of eigenvectors | Description in terms of diagonalizability | Geometric interpretation | Notes | Examples |
|---|---|---|---|---|---|
| is diagonalizable | There exists a basis of consisting of eigenvectors of | is diagonalizable (there exists a basis of with respect to which is a diagonal matrix) | This basis is not unique because we can reorder the vectors and also scale eigenvectors by a non-zero number to obtain an eigenvector. But there are at most distinct eigenvalues so the diagonal matrix should be unique up to order? | If is the identity map, then every non-zero vector is an eigenvector of with eigenvalue because . Thus every basis diagonalizes . The matrix of with respect to is the identity matrix. | |
| is normal | There exists an orthonormal basis of consisting of eigenvectors of | is diagonalizable using an orthonormal basis | |||
| self-adjoint ( is Hermitian) | There exists an orthonormal basis of consisting of eigenvectors of with real eigenvalues | is diagonalizable using an orthonormal basis and the diagonal entries are all real | |||
| is an isometry | There exists an orthonormal basis of consisting of eigenvectors of whose eigenvalues all have absolute value 1 | is diagonalizable using an orthonormal basis and the diagonal entries all have absolute values 1 | This only works when the field of scalars is the complex numbers | ||
| is positive (positive semidefinite) | There exists an orthonormal basis of consisting of eigenvectors of with nonnegative real eigenvalues | is diagonalizable using an orthonormal basis and the diagonal entries are all nonnegative real numbers |