Invertible matrix

An -by- square matrix is called invertible if there exists an -by- square matrix such that\mathbf{AB} = \mathbf{BA} = \mathbf{I}_n ,where denotes the -by- identity matrix and the multiplication used is ordinary matrix multiplication. If this is the case, then the matrix is uniquely determined by , and is called the inverse of , denoted by . Matrix inversion is the process of finding the matrix which when multiplied by the original matrix gives the identity matrix. == Examples ==

Consider the following 2-by-2 matrix: : \mathbf{A} = \begin{pmatrix}-1 & \tfrac{3}{2} \\ 1 & -1\end{pmatrix} The matrix \mathbf{A} is invertible, as it has inverse \mathbf{B} = \begin{pmatrix} 2 & 3 \\ 2 & 2\end{pmatrix} , which can be confirmed by computing \mathbf{A}\mathbf{B} = \begin{pmatrix}-1 & \tfrac{3}{2} \\ 1 & -1\end{pmatrix} \begin{pmatrix} 2 & 3 \\ 2 & 2\end{pmatrix} = \begin{pmatrix} (-1) \times 2 + \tfrac 3 2 \times 2 & (-1) \times 3 + \tfrac 3 2 \times 2 \\ 1 \times 2 + (-1) \times 2 & 1 \times 3 + (-1) \times 2\end{pmatrix} = \begin{pmatrix}1 & 0 \\ 0 & 1\end{pmatrix} = \mathbf{I}_2 To check that it is invertible without finding an inverse, \det \mathbf{A} = -\frac{1}{2} can be computed, which is non-zero. On the other hand, this is a non-invertible matrix: : \mathbf{C} = \begin{pmatrix} 2 & 4\\ 2 & 4 \end{pmatrix} We can see the rank of this 2-by-2 matrix is 1, which is , so it is non-invertible. Additionally, we can compute that the determinant of \mathbf{C} is 0, which is a necessary and sufficient condition for a matrix to be non-invertible. == Methods of matrix inversion ==

Gaussian elimination Gaussian elimination is a useful and easy way to compute the inverse of a matrix. To compute a matrix inverse using this method, an augmented matrix is first created with the left side being the matrix to invert and the right side being the identity matrix. Then, Gaussian elimination is used to convert the left side into the identity matrix, which causes the right side to become the inverse of the input matrix. For example, take the following matrix: \mathbf{A} = \begin{pmatrix}-1 & \tfrac{3}{2} \\ 1 & -1\end{pmatrix} The first step to compute its inverse is to create the augmented matrix \left(\!\!\begin{array}{cc|cc} -1 & \tfrac{3}{2} & 1 & 0 \\ 1 & -1 & 0 & 1 \end{array}\!\!\right) Call the first row of this matrix R_1 and the second row R_2. Then, add row 1 to row 2 (R_1 + R_2 \to R_2). This yields \left(\!\!\begin{array}{cc|cc} -1 & \tfrac{3}{2} & 1 & 0 \\ 0 & \tfrac{1}{2} & 1 & 1 \end{array}\!\!\right) Next, subtract row 2, multiplied by 3, from row 1 (R_1 - 3\, R_2 \to R_1), which yields \left(\!\!\begin{array}{cc|cc} -1 & 0 & -2 & -3 \\ 0 & \tfrac{1}{2} & 1 & 1 \end{array}\!\!\right) Finally, multiply row 1 by −1 (-R_1 \to R_1) and row 2 by 2 (2\, R_2 \to R_2). This yields the identity matrix on the left side and the inverse matrix on the right:\left(\!\!\begin{array}{cc|cc} 1 & 0 & 2 & 3 \\ 0 & 1 & 2 & 2 \end{array}\!\!\right) Thus, \mathbf{A}^{-1} = \begin{pmatrix} 2 & 3 \\ 2 & 2 \end{pmatrix} It works because the process of Gaussian elimination can be viewed as a sequence of applying left matrix multiplication using elementary row operations using elementary matrices (\mathbf E_n), such as \mathbf E_n \mathbf E_{n-1} \cdots \mathbf E_2 \mathbf E_1 \mathbf A = \mathbf I Applying right-multiplication using \mathbf A^{-1}, we get \mathbf E_n \mathbf E_{n-1} \cdots \mathbf E_2 \mathbf E_1 \mathbf I = \mathbf I \mathbf A^{-1}. And the right side \mathbf I \mathbf A^{-1} = \mathbf A^{-1}, which is the inverse we want. To obtain \mathbf E_n \mathbf E_{n-1} \cdots \mathbf E_2 \mathbf E_1 \mathbf I, we create the augmented matrix by combining with and applying Gaussian elimination. The two portions will be transformed using the same sequence of elementary row operations. When the left portion becomes , the right portion applied the same elementary row operation sequence will become . Newton's method A generalization of Newton's method as used for a multiplicative inverse algorithm may be convenient if it is convenient to find a suitable starting seed: : X_{k+1} = 2X_k - X_k A X_k Victor Pan and John Reif have done work that includes ways of generating a starting seed. Newton's method is particularly useful when dealing with families of related matrices that behave enough like the sequence manufactured for the homotopy above: sometimes a good starting point for refining an approximation for the new inverse can be the already obtained inverse of a previous matrix that nearly matches the current matrix. For example, the pair of sequences of inverse matrices used in obtaining matrix square roots by Denman–Beavers iteration. That may need more than one pass of the iteration at each new matrix, if they are not close enough together for just one to be enough. Newton's method is also useful for "touch up" corrections to the Gauss–Jordan algorithm which has been contaminated by small errors from imperfect computer arithmetic. Cayley–Hamilton method The Cayley–Hamilton theorem allows the inverse of to be expressed in terms of , traces and powers of : : \mathbf{A}^{-1} = \frac{1}{\det(\mathbf{A})} \sum_{s=0}^{n-1} \mathbf{A}^s \sum_{k_1,k_2,\ldots,k_{n-1}} \prod_{l=1}^{n-1} \frac{(-1)^{k_l + 1}}{l^{k_l}k_l!} \operatorname{tr}\left(\mathbf{A}^l\right)^{k_l}, where is size of , and is the trace of matrix given by the sum of the main diagonal. The sum is taken over and the sets of all k_l \geq 0 satisfying the linear Diophantine equation : s + \sum_{l=1}^{n-1} lk_l = n - 1 The formula can be rewritten in terms of complete Bell polynomials of arguments t_l = - (l - 1)! \operatorname{tr}\left(A^l\right) as : \mathbf{A}^{-1} = \frac{1}{\det(\mathbf{A})} \sum_{s=1}^n \mathbf{A}^{s-1} \frac{(-1)^{n - 1}}{(n - s)!} B_{n-s}(t_1, t_2, \ldots, t_{n-s}) That is described in more detail under Cayley–Hamilton method. Eigendecomposition If matrix can be eigendecomposed, and if none of its eigenvalues are zero, then is invertible and its inverse is given by : \mathbf{A}^{-1} = \mathbf{Q}\mathbf{\Lambda}^{-1}\mathbf{Q}^{-1}, where is the square matrix whose th column is the eigenvector q_i of , and is the diagonal matrix whose diagonal entries are the corresponding eigenvalues, that is, \Lambda_{ii} = \lambda_i. If is symmetric, is guaranteed to be an orthogonal matrix, therefore \mathbf{Q}^{-1} = \mathbf{Q}^\mathrm{T} . Furthermore, because is a diagonal matrix, its inverse is easy to calculate: : \left[\Lambda^{-1}\right]_{ii} = \frac{1}{\lambda_i} Cholesky decomposition If matrix is positive definite, then its inverse can be obtained as : \mathbf{A}^{-1} = \left(\mathbf{L}^*\right)^{-1} \mathbf{L}^{-1} , where is the lower triangular Cholesky decomposition of , and denotes the conjugate transpose of . Analytic solution Writing the transpose of the matrix of cofactors, known as an adjugate matrix, may also be an efficient way to calculate the inverse of small matrices, but the recursive method is inefficient for large matrices. To determine the inverse, we calculate a matrix of cofactors: : \mathbf{A}^{-1} = {1 \over \begin{vmatrix}\mathbf{A}\end{vmatrix}}\mathbf{C}^\mathrm{T} = {1 \over \begin{vmatrix}\mathbf{A}\end{vmatrix}} \begin{pmatrix} \mathbf{C}_{11} & \mathbf{C}_{21} & \cdots & \mathbf{C}_{n1} \\ \mathbf{C}_{12} & \mathbf{C}_{22} & \cdots & \mathbf{C}_{n2} \\ \vdots & \vdots & \ddots & \vdots \\ \mathbf{C}_{1n} & \mathbf{C}_{2n} & \cdots & \mathbf{C}_{nn} \\ \end{pmatrix} so that : \left(\mathbf{A}^{-1}\right)_{ij} = {1 \over \begin{vmatrix}\mathbf{A}\end{vmatrix}}\left(\mathbf{C}^{\mathrm{T}}\right)_{ij} = {1 \over \begin{vmatrix}\mathbf{A}\end{vmatrix}}\left(\mathbf{C}_{ji}\right) where is the determinant of , is the matrix of cofactors, and represents the matrix transpose. Inversion of 2 × 2 matrices The cofactor equation listed above yields the following result for matrices. Inversion of these matrices can be done as follows: : \mathbf{A}^{-1} = \begin{bmatrix} a & b \\ c & d \\ \end{bmatrix}^{-1} = \frac{1}{\det \mathbf{A}} \begin{bmatrix} \,\,\,d & \!\!-b \\ -c & \,a \\ \end{bmatrix} = \frac{1}{ad - bc} \begin{bmatrix} \,\,\,d & \!\!-b \\ -c & \,a \\ \end{bmatrix} This is possible because is the reciprocal of the determinant of the matrix in question, and the same strategy could be used for other matrix sizes. The Cayley–Hamilton method gives : \mathbf{A}^{-1} = \frac{1}{\det \mathbf{A}} \left[ \left( \operatorname{tr}\mathbf{A} \right) \mathbf{I} - \mathbf{A} \right] Inversion of 3 × 3 matrices A computationally efficient matrix inversion is given by : \mathbf{A}^{-1} = \begin{bmatrix} a & b & c\\ d & e & f \\ g & h & i\\ \end{bmatrix}^{-1} = \frac{1}{\det(\mathbf{A})} \begin{bmatrix} \, A & \, B & \,C \\ \, D & \, E & \, F \\ \, G & \, H & \, I\\ \end{bmatrix}^\mathrm{T} = \frac{1}{\det(\mathbf{A})} \begin{bmatrix} \, A & \, D & \,G \\ \, B & \, E & \,H \\ \, C & \,F & \, I\\ \end{bmatrix} (where the scalar is not to be confused with the matrix ). If the determinant is non-zero, the matrix is invertible, with the entries of the intermediary matrix on the right side above given by : \begin{alignat}{6} A &={}& (ei - fh), &\quad& D &={}& -(bi - ch), &\quad& G &={}& (bf - ce), \\ B &={}& -(di - fg), &\quad& E &={}& (ai - cg), &\quad& H &={}& -(af - cd), \\ C &={}& (dh - eg), &\quad& F &={}& -(ah - bg), &\quad& I &={}& (ae - bd). \\ \end{alignat} The determinant of can be computed by applying the rule of Sarrus as follows: : \det(\mathbf{A}) = aA + bB + cC The Cayley–Hamilton decomposition gives : \mathbf{A}^{-1} = \frac{1}{\det (\mathbf{A})}\left( \tfrac{1}{2}\left[ (\operatorname{tr}\mathbf{A})^{2} - \operatorname{tr}(\mathbf{A}^{2})\right] \mathbf{I} - \mathbf{A}\operatorname{tr}\mathbf{A} + \mathbf{A}^{2}\right) The general inverse can be expressed concisely in terms of the cross product and triple product. If a matrix \mathbf{A} = \begin{bmatrix} \mathbf{x}_0 & \mathbf{x}_1 & \mathbf{x}_2\end{bmatrix} (consisting of three column vectors, \mathbf{x}_0, \mathbf{x}_1, and \mathbf{x}_2) is invertible, its inverse is given by : \mathbf{A}^{-1} = \frac{1}{\det(\mathbf A)}\begin{bmatrix} {(\mathbf{x}_1\times\mathbf{x}_2)}^\mathrm{T} \\ {(\mathbf{x}_2\times\mathbf{x}_0)}^\mathrm{T} \\ {(\mathbf{x}_0\times\mathbf{x}_1)}^\mathrm{T} \end{bmatrix} The determinant of , , is equal to the triple product of , , and —the volume of the parallelepiped formed by the rows or columns: : \det(\mathbf{A}) = \mathbf{x}_0\cdot(\mathbf{x}_1\times\mathbf{x}_2) The correctness of the formula can be checked by using cross- and triple-product properties and by noting that for groups, left and right inverses always coincide. Intuitively, because of the cross products, each row of is orthogonal to the non-corresponding two columns of (causing the off-diagonal terms of \mathbf{I} = \mathbf{A}^{-1}\mathbf{A} be zero). Dividing by : \det(\mathbf{A}) = \mathbf{x}_0\cdot(\mathbf{x}_1\times\mathbf{x}_2) causes the diagonal entries of to be unity. For example, the first diagonal is: : 1 = \frac{1}{\mathbf{x_0}\cdot(\mathbf{x}_1\times\mathbf{x}_2)} \mathbf{x_0}\cdot(\mathbf{x}_1\times\mathbf{x}_2) Inversion of 4 × 4 matrices With increasing dimension, expressions for the inverse of get complicated. For , the Cayley–Hamilton method leads to an expression that is still tractable: :\begin{align} \mathbf{A}^{-1} = \frac{1}{\det(\mathbf{A})}\Bigl( &\tfrac{1}{6}\bigl( (\operatorname{tr}\mathbf{A})^{3} - 3\operatorname{tr}\mathbf{A}\operatorname{tr}(\mathbf{A}^{2}) + 2\operatorname{tr}(\mathbf{A}^{3})\bigr) \mathbf{I} \\[-3mu] &\ \ \ - \tfrac{1}{2}\mathbf{A}\bigl((\operatorname{tr}\mathbf{A})^{2} - \operatorname{tr}(\mathbf{A}^{2})\bigr) + \mathbf{A}^{2}\operatorname{tr}\mathbf{A} - \mathbf{A}^{3} \Bigr) \end{align} Blockwise inversion Let \mathbf M = \begin{bmatrix} \mathbf{A} & \mathbf{B} \\ \mathbf{C} & \mathbf{D} \end{bmatrix} where , , and are matrix sub-blocks of arbitrary size and \mathbf M / \mathbf A := \mathbf D - \mathbf C \mathbf A^{-1} \mathbf B is the Schur complement of . ( must be square, so that it can be inverted. Furthermore, and must be nonsingular.) Matrices can also be inverted blockwise by using the analytic inversion formula: {{NumBlk \begin{bmatrix} \mathbf{A}^{-1} + \mathbf{A}^{-1}\mathbf{B}\ (\mathbf M / \mathbf A)^{-1}\mathbf{CA}^{-1} & -\mathbf{A}^{-1}\mathbf{B}\left(\mathbf M / \mathbf A \right)^{-1} \\ -\left(\mathbf M / \mathbf A \right)^{-1}\mathbf{CA}^{-1} & \left(\mathbf M / \mathbf A \right)^{-1} \end{bmatrix}, }} The strategy is particularly advantageous if is diagonal and is a small matrix, since they are the only matrices requiring inversion. The nullity theorem says that the nullity of equals the nullity of the sub-block in the lower right of the inverse matrix, and that the nullity of equals the nullity of the sub-block in the upper right of the inverse matrix. The inversion procedure that led to Equation () performed matrix block operations that operated on and first. Instead, if and are operated on first, and provided and are nonsingular, the result is {{NumBlk \begin{bmatrix} \mathbf{A} & \mathbf{B} \\ \mathbf{C} & \mathbf{D} \end{bmatrix}^{-1} = \begin{bmatrix} \left( \mathbf M / \mathbf D \right)^{-1} & -\left( \mathbf M / \mathbf D \right)^{-1}\mathbf{BD}^{-1} \\ -\mathbf{D}^{-1}\mathbf{C}\left(\mathbf M / \mathbf D\right)^{-1} & \quad \mathbf{D}^{-1} + \mathbf{D}^{-1}\mathbf{C}\left(\mathbf M / \mathbf D\right)^{-1}\mathbf{BD}^{-1} \end{bmatrix}. }} Equating the upper-left sub-matrices of Equations () and () leads to {{NumBlk \left(\mathbf{A} - \mathbf{BD}^{-1}\mathbf{C}\right)^{-1} &= \mathbf{A}^{-1} + \mathbf{A}^{-1}\mathbf{B}\left(\mathbf{D} - \mathbf{CA}^{-1}\mathbf{B}\right)^{-1}\mathbf{CA}^{-1} \\ \left(\mathbf{A} - \mathbf{BD}^{-1}\mathbf{C}\right)^{-1}\mathbf{BD}^{-1} &= \mathbf{A}^{-1}\mathbf{B}\left(\mathbf{D} - \mathbf{CA}^{-1}\mathbf{B}\right)^{-1} \\ \mathbf{D}^{-1}\mathbf{C}\left(\mathbf{A} - \mathbf{BD}^{-1}\mathbf{C}\right)^{-1} &= \left(\mathbf{D} - \mathbf{CA}^{-1}\mathbf{B}\right)^{-1}\mathbf{CA}^{-1} \\ \mathbf{D}^{-1} + \mathbf{D}^{-1}\mathbf{C}\left(\mathbf{A} - \mathbf{BD}^{-1}\mathbf{C}\right)^{-1}\mathbf{BD}^{-1} &= \left(\mathbf{D} - \mathbf{CA}^{-1}\mathbf{B}\right)^{-1} \end{align} }} where Equation () is the Woodbury matrix identity, which is equivalent to the binomial inverse theorem. If and are both invertible, then the above two block matrix inverses can be combined to provide the simple factorization {{NumBlk \begin{bmatrix} \left(\mathbf{A} - \mathbf{B} \mathbf{D}^{-1} \mathbf{C}\right)^{-1} & \mathbf{0} \\ \mathbf{0} & \left(\mathbf{D} - \mathbf{C} \mathbf{A}^{-1} \mathbf{B}\right)^{-1} \end{bmatrix} \begin{bmatrix} \mathbf{I} & -\mathbf{B} \mathbf{D}^{-1} \\ -\mathbf{C} \mathbf{A}^{-1} & \mathbf{I} \end{bmatrix}. }} By the Weinstein–Aronszajn identity, one of the two matrices in the block-diagonal matrix is invertible exactly when the other is. This formula simplifies significantly when the upper right block matrix is the zero matrix. This formulation is useful when the matrices and have relatively simple inverse formulas (or pseudo inverses in the case where the blocks are not all square. In this special case, the block matrix inversion formula stated in full generality above becomes :\begin{bmatrix} \mathbf{A} & \mathbf{0} \\ \mathbf{C} & \mathbf{D} \end{bmatrix}^{-1} = \begin{bmatrix} \mathbf{A}^{-1} & \mathbf{0} \\ -\mathbf{D}^{-1}\mathbf{CA}^{-1} & \mathbf{D}^{-1} \end{bmatrix} If the given invertible matrix is a symmetric matrix with invertible block the following block inverse formula holds Research into matrix multiplication complexity shows that there exist matrix multiplication algorithms with a complexity of operations, while the best proven lower bound is . By Neumann series If a matrix has the property that : \lim_{n \to \infty} (\mathbf I - \mathbf A)^n = 0 then is nonsingular and its inverse may be expressed by a Neumann series: : \mathbf A^{-1} = \sum_{n = 0}^\infty (\mathbf I - \mathbf A)^n Truncating the sum results in an "approximate" inverse which may be useful as a preconditioner. Note that a truncated series can be accelerated exponentially by noting that the Neumann series is a geometric sum. As such, it satisfies : \sum_{n=0}^{2^L-1} (\mathbf I - \mathbf A)^n = \prod_{l=0}^{L-1}\left(\mathbf I + (\mathbf I - \mathbf A)^{2^l}\right) Therefore, only matrix multiplications are needed to compute terms of the sum. More generally, if is "near" the invertible matrix in the sense that : \lim_{n \to \infty} \left(\mathbf I - \mathbf X^{-1} \mathbf A\right)^n = 0 \mathrm{~~or~~} \lim_{n \to \infty} \left(\mathbf I - \mathbf A \mathbf X^{-1}\right)^n = 0 then is nonsingular and its inverse is : \mathbf A^{-1} = \sum_{n = 0}^\infty \left(\mathbf X^{-1} (\mathbf X - \mathbf A)\right)^n \mathbf X^{-1}~ If it is also the case that has rank 1 then this simplifies to : \mathbf A^{-1} = \mathbf X^{-1} - \frac{\mathbf X^{-1} (\mathbf A - \mathbf X) \mathbf X^{-1}}{1 + \operatorname{tr}\left(\mathbf X^{-1} (\mathbf A - \mathbf X)\right)}~ p-adic approximation If is a matrix with integer or rational entries, and we seek a solution in arbitrary-precision rationals, a -adic approximation method converges to an exact solution in , assuming standard matrix multiplication is used. The method relies on solving linear systems via Dixon's method of -adic approximation (each in ) and is available as such in software specialized in arbitrary-precision matrix operations, for example, in IML. Reciprocal basis vectors method Given an square matrix \mathbf{X} = \left[ x^{ij} \right] , 1 \leq i,j \leq n , with rows interpreted as vectors \mathbf{x}_{i} = x^{ij} \mathbf{e}_{j} (Einstein summation assumed) where the \mathbf{e}_{j} are a standard orthonormal basis of Euclidean space \mathbb{R}^{n} (\mathbf{e}_{i} = \mathbf{e}^{i}, \mathbf{e}_{i} \cdot \mathbf{e}^{j} = \delta_i^j), then using Clifford algebra (or geometric algebra) we compute the reciprocal (sometimes called dual) column vectors: :\mathbf{x}^{i} = x_{ji} \mathbf{e}^{j} = (-1)^{i-1} (\mathbf{x}_{1} \wedge\cdots\wedge ()_{i} \wedge\cdots\wedge\mathbf{x}_{n}) \cdot (\mathbf{x}_{1} \wedge\ \mathbf{x}_{2} \wedge\cdots\wedge\mathbf{x}_{n})^{-1} as the columns of the inverse matrix \mathbf{X}^{-1} = [x_{ji}]. Note that, the place "()_{i}" indicates that "\mathbf{x}_{i}" is removed from that place in the above expression for \mathbf{x}^{i}. We then have \mathbf{X}\mathbf{X}^{-1} = \left[ \mathbf{x}_{i} \cdot \mathbf{x}^{j} \right] = \left[ \delta_{i}^{j} \right] = \mathbf{I}_{n} , where \delta_{i}^{j} is the Kronecker delta. We also have \mathbf{X}^{-1}\mathbf{X} = \left[\left(\mathbf{e}_{i}\cdot\mathbf{x}^{k}\right)\left(\mathbf{e}^{j}\cdot\mathbf{x}_{k}\right)\right] = \left[\mathbf{e}_{i}\cdot\mathbf{e}^{j}\right] = \left[\delta_{i}^{j}\right] = \mathbf{I}_{n}, as required. If the vectors \mathbf{x}_{i} are not linearly independent, then (\mathbf{x}_{1} \wedge \mathbf{x}_{2} \wedge\cdots\wedge\mathbf{x}_{n}) = 0 and the matrix \mathbf{X} is not invertible (has no inverse). == Properties ==

Singularity Over a field, a square matrix that is not invertible is called singular or degenerate. A square matrix with entries in a field is singular if and only if its determinant is zero. Invertible matrix theorem Let be a square -by- matrix over a field (e.g., the field of real numbers). The following statements are equivalent, i.e., they are either all true or all false for any given matrix: • is invertible, i.e. it has an inverse under matrix multiplication, i.e., there exists a such that . (In that statement, "invertible" can equivalently be replaced with "left-invertible" or "right-invertible" in which one-sided inverses are considered.) • The linear transformation mapping to is invertible, i.e., it has an inverse under function composition. (There, again, "invertible" can equivalently be replaced with either "left-invertible" or "right-invertible".) • The transpose is an invertible matrix. • is row-equivalent to the -by- identity matrix . • is column-equivalent to the -by- identity matrix . • has pivot positions. • has full rank: . • has a trivial kernel: {{math|1=ker(A) = {0}.}} • The linear transformation mapping to is bijective; that is, the equation has exactly one solution for each in . (There, "bijective" can equivalently be replaced with "injective" or "surjective".) • The columns of form a basis of . (In this statement, "basis" can equivalently be replaced with either "linearly independent set" or "spanning set") • The rows of form a basis of . (Similarly, here, "basis" can equivalently be replaced with either "linearly independent set" or "spanning set") • The determinant of is nonzero: . In general, a square matrix over a commutative ring is invertible if and only if its determinant is a unit (i.e. multiplicatively invertible element) of that ring. • The number 0 is not an eigenvalue of . (More generally, a number \lambda is an eigenvalue of if the matrix \mathbf{A}-\lambda \mathbf{I} is singular, where is the identity matrix.) • The matrix can be expressed as a finite product of elementary matrices. Other properties Furthermore, the following properties hold for an invertible matrix : • (\mathbf A^{-1})^{-1} = \mathbf A • (k \mathbf A)^{-1} = k^{-1} \mathbf A^{-1} for nonzero scalar • (\mathbf{Ax})^+ = \mathbf x^+ \mathbf A^{-1} if has orthonormal columns, where denotes the Moore–Penrose inverse and is a vector • (\mathbf A^\mathrm{T})^{-1} = (\mathbf A^{-1})^\mathrm{T} • For any invertible -by- matrices and , (\mathbf{AB})^{-1} = \mathbf B^{-1} \mathbf A^{-1}. More generally, if \mathbf A_1, \dots, \mathbf A_k are invertible -by- matrices, then (\mathbf A_1 \mathbf A_2 \cdots \mathbf A_{k-1} \mathbf A_k)^{-1} = \mathbf A_k^{-1} \mathbf A_{k-1}^{-1} \cdots \mathbf A_2^{-1} \mathbf A_1^{-1}. • \det \mathbf A^{-1} = (\det \mathbf A)^{-1}. • Left and right inverses are equal. That is, if \mathbf{LA} = \mathbf I and \mathbf{AR} = \mathbf I then \mathbf L = \mathbf L(\mathbf{AR}) = (\mathbf{LA}) \mathbf R = \mathbf R. The rows of the inverse matrix of a matrix are orthonormal to the columns of (and vice versa interchanging rows for columns). To see this, suppose that where the rows of are denoted as v_i^{\mathrm{T}} and the columns of as u_j for 1 \leq i,j \leq n. Then clearly, the Euclidean inner product of any two v_i^{\mathrm{T}} u_j = \delta_{i,j}. This property can also be useful in constructing the inverse of a square matrix in some instances, where a set of orthogonal vectors (but not necessarily orthonormal vectors) to the columns of are known. In which case, one can apply the iterative Gram–Schmidt process to this initial set to determine the rows of the inverse . A matrix that is its own inverse (i.e., a matrix such that and consequently ) is called an involutory matrix. In relation to its adjugate The adjugate of a matrix can be used to find the inverse of as follows: If is an invertible matrix, then : \mathbf{A}^{-1} = \frac{1}{\det(\mathbf{A})} \operatorname{adj}(\mathbf{A}) In relation to the identity matrix It follows from the associativity of matrix multiplication that if : \mathbf{AB} = \mathbf{I} \ for finite square matrices and , then also : \mathbf{BA} = \mathbf{I}\ Density Over the field of real numbers, the set of singular -by- matrices, considered as a subset of {{tmath|\mathbb R^{n \times n},}} is a null set, that is, has Lebesgue measure zero. That is true because singular matrices are the roots of the determinant function. It is a continuous function because it is a polynomial in the entries of the matrix. Thus in the language of measure theory, almost all -by- matrices are invertible. Furthermore, the set of -by- invertible matrices is open and dense in the topological space of all -by- matrices. Equivalently, the set of singular matrices is closed and nowhere dense in the space of -by- matrices. In practice, however, non-invertible matrices may be encountered. In numerical calculations, matrices that are invertible but close to a non-invertible matrix may still be problematic and are said to be ill-conditioned. == Derivative of the matrix inverse ==

Suppose that the invertible matrix A depends on a parameter t. Then the derivative of the inverse of A with respect to t is given by : \frac{\mathrm{d}}{\mathrm{d}t} \mathbf{A}^{-1} = - \mathbf{A}^{-1} \frac{\mathrm{d}\mathbf{A}}{\mathrm{d}t} \mathbf{A}^{-1} To derive the above expression for the derivative of the inverse of A, one can differentiate the definition of the matrix inverse \mathbf{A}^{-1}\mathbf{A}=\mathbf{I} using the product rule, and then solve for the derivative of the inverse of A: : \mathbf{0} = \frac{\mathrm{d}\mathbf{I}}{\mathrm{d}t} = \frac{\mathrm{d}(\mathbf{A}^{-1}\mathbf{A})}{\mathrm{d}t} = \frac{\mathrm{d}(\mathbf{A}^{-1})}{\mathrm{d}t}\mathbf{A} + \mathbf{A}^{-1}\frac{\mathrm{d}\mathbf{A}}{\mathrm{d}t} Subtracting \mathbf{A}^{-1}\frac{\mathrm{d}\mathbf{A}}{\mathrm{d}t} from both ends of this formula, and multiplying on the right by \mathbf{A}^{-1} finishes the derivation. If \varepsilon is a small number then the derivative formula gives: : \left(\mathbf{A} + \varepsilon\mathbf{X}\right)^{-1} = \mathbf{A}^{-1} - \varepsilon \mathbf{A}^{-1} \mathbf{X} \mathbf{A}^{-1} + \mathcal{O}(\varepsilon^2)\, Given a positive integer n, : \begin{align} \frac{ \mathrm{d}}{ \mathrm{d}t} \mathbf{A}^{n} &= \sum_{i=1}^n \mathbf{A}^{i-1}\frac{ \mathrm{d}\mathbf{A}}{ \mathrm{d}t}\mathbf{A}^{n-i},\\ \frac{ \mathrm{d}}{ \mathrm{d}t} \mathbf{A}^{-n} &= -\sum_{i=1}^n \mathbf{A}^{-i}\frac{ \mathrm{d}\mathbf{A}}{ \mathrm{d}t}\mathbf{A}^{-(n+1-i)} \end{align} In particular, : \begin{align} (\mathbf{A} + \varepsilon \mathbf{X})^{n} &= \mathbf{A}^{n} + \varepsilon \sum_{i=1}^n \mathbf{A}^{i-1}\mathbf{X}\mathbf{A}^{n-i} + \mathcal{O}\left(\varepsilon^2\right),\\ (\mathbf{A} + \varepsilon \mathbf{X})^{-n} &= \mathbf{A}^{-n} - \varepsilon \sum_{i=1}^n \mathbf{A}^{-i}\mathbf{X}\mathbf{A}^{-(n+1-i)} + \mathcal{O}\left(\varepsilon^2\right) \end{align} == Generalizations ==

Non-square matrices Non-square matrices, i.e. -by- matrices for which , do not have an inverse. However, in some cases such a matrix may have a left inverse or right inverse. If is -by- and the rank of is equal to , (), then has a left inverse, an -by- matrix such that . If has rank (), then it has a right inverse, an -by- matrix such that . Some of the properties of inverse matrices are shared by generalized inverses (such as the Moore–Penrose inverse), which can be defined for any m-by-n matrix. In Abstract algebra While the most common case is that of matrices over the real or complex numbers, all of those definitions can be given for matrices over any algebraic structure equipped with addition and multiplication (i.e. rings). However, in the case of a ring being commutative, the condition for a square matrix to be invertible is that its determinant is invertible in the ring, which in general is a stricter requirement than it being nonzero. For a noncommutative ring, the usual determinant is not defined. The conditions for existence of left-inverse or right-inverse are more complicated, since a notion of rank does not exist over rings. The set of invertible matrices together with the operation of matrix multiplication and entries from ring form a group, the general linear group of degree , denoted . == Applications ==

For most practical applications, it is not necessary to invert a matrix to solve a system of linear equations; however, for a unique solution, it is necessary for the matrix involved to be invertible. Decomposition techniques like LU decomposition are much faster than inversion, and various fast algorithms for special classes of linear systems have also been developed. Regression/least squares Although an explicit inverse is not necessary to estimate the vector of unknowns, it is the easiest way to estimate their accuracy and is found in the diagonal of a matrix inverse (the posterior covariance matrix of the vector of unknowns). However, faster algorithms to compute only the diagonal entries of a matrix inverse are known in many cases. Matrix inverses in real-time simulations Matrix inversion plays a significant role in computer graphics, particularly in 3D graphics rendering and 3D simulations. Examples include screen-to-world ray casting, world-to-subspace-to-world object transformations, and physical simulations. Matrix inverses in MIMO wireless communication Matrix inversion also plays a significant role in the MIMO (Multiple-Input, Multiple-Output) technology in wireless communications. The MIMO system consists of N transmit and M receive antennas. Unique signals, occupying the same frequency band, are sent via N transmit antennas and are received via M receive antennas. The signal arriving at each receive antenna will be a linear combination of the N transmitted signals forming an N × M transmission matrix H. It is crucial for the matrix H to be invertible so that the receiver can figure out the transmitted information. == See also ==