Finding a matrix $A$ that satisfies specific conditions is a fundamental problem in linear algebra. The conditions can vary widely, ranging from simple matrix equations to more complex constraints involving eigenvalues, eigenvectors, or other matrix properties. This exploration looks at various scenarios and methods for finding such a matrix $A$ Most people skip this — try not to. That alone is useful..
People argue about this. Here's where I land on it.
Introduction
The quest to "find the matrix A such that" is a common task in numerous mathematical and computational contexts. In real terms, the nature of the problem hinges significantly on the conditions imposed on $A$. These conditions can involve relationships with other matrices, specific characteristics like being invertible or symmetric, or even constraints related to its eigenvalues and eigenvectors. Which means, understanding the different types of conditions and appropriate solution techniques is crucial.
Basic Matrix Equations
One of the simplest scenarios involves finding a matrix $A$ that satisfies a basic matrix equation.
The Equation $AX = B$
Consider the equation $AX = B$, where $A$ is an unknown matrix, and $X$ and $B$ are known matrices. To find $A$, we need to "undo" the multiplication by $X$. If $X$ is invertible, the solution is straightforward Took long enough..
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Condition for Solution: For a solution to exist, the number of rows in $X$ must equal the number of columns in $A$, and the number of rows in $B$ must equal the number of rows in $A$.
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Solution: If $X$ is a square, invertible matrix, we can find $A$ by multiplying both sides of the equation by the inverse of $X$ from the right:
$AX = B$
$AXX^{-1} = BX^{-1}$
$A = BX^{-1}$
Here, $X^{-1}$ is the inverse of matrix $X$. Here's the thing — the solution $A = BX^{-1}$ is unique when $X$ is invertible. Think about it: * Non-Invertible $X$: If $X$ is not invertible or not a square matrix, the problem becomes more complicated. One approach is to use the Moore-Penrose pseudoinverse, denoted as $X^+$.
$A = BX^+$
The pseudoinverse satisfies the properties:
- $XX^+X = X$
- $X^+XX^+ = X^+$
- $(XX^+)^*$ = $XX^+$
- $(X^+X)^*$ = $X^+X$
Where $*$ denotes the conjugate transpose. The matrix $A = BX^+$ minimizes $||AX - B||_F$, where $|| \cdot ||_F$ is the Frobenius norm Easy to understand, harder to ignore. Practical, not theoretical..
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Example: Let's consider the matrices:
$X = \begin{bmatrix} 1 & 2 \ 3 & 4 \end{bmatrix}$ and $B = \begin{bmatrix} 5 & 6 \ 7 & 8 \end{bmatrix}$
First, we find the inverse of $X$:
$X^{-1} = \frac{1}{(1 \cdot 4 - 2 \cdot 3)} \begin{bmatrix} 4 & -2 \ -3 & 1 \end{bmatrix} = -\frac{1}{2} \begin{bmatrix} 4 & -2 \ -3 & 1 \end{bmatrix} = \begin{bmatrix} -2 & 1 \ 3/2 & -1/2 \end{bmatrix}$
Then, we compute $A = BX^{-1}$:
$A = \begin{bmatrix} 5 & 6 \ 7 & 8 \end{bmatrix} \begin{bmatrix} -2 & 1 \ 3/2 & -1/2 \end{bmatrix} = \begin{bmatrix} -10+9 & 5-3 \ -14+12 & 7-4 \end{bmatrix} = \begin{bmatrix} -1 & 2 \ -2 & 3 \end{bmatrix}$
Thus, $A = \begin{bmatrix} -1 & 2 \ -2 & 3 \end{bmatrix}$ Worth keeping that in mind. Surprisingly effective..
The Equation $XA = B$
Now consider the equation $XA = B$, where $A$ is the unknown matrix, and $X$ and $B$ are known matrices. Here, we need to "undo" the multiplication by $X$ from the left Most people skip this — try not to..
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Condition for Solution: For a solution to exist, the number of columns in $X$ must equal the number of rows in $A$, and the number of columns in $B$ must equal the number of columns in $A$ Took long enough..
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Solution: If $X$ is a square, invertible matrix, we can find $A$ by multiplying both sides of the equation by the inverse of $X$ from the left:
$XA = B$
$X^{-1}XA = X^{-1}B$
$A = X^{-1}B$
Here, $X^{-1}$ is the inverse of matrix $X$. The solution $A = X^{-1}B$ is unique when $X$ is invertible.
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Non-Invertible $X$: If $X$ is not invertible or not a square matrix, we use the Moore-Penrose pseudoinverse, denoted as $X^+$ Worth keeping that in mind..
$A = X^+B$
Here, $A = X^+B$ minimizes $||XA - B||_F$.
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Example: Let's consider the matrices:
$X = \begin{bmatrix} 1 & 2 \ 3 & 4 \end{bmatrix}$ and $B = \begin{bmatrix} 5 & 6 \ 7 & 8 \end{bmatrix}$
First, we find the inverse of $X$:
$X^{-1} = \frac{1}{(1 \cdot 4 - 2 \cdot 3)} \begin{bmatrix} 4 & -2 \ -3 & 1 \end{bmatrix} = -\frac{1}{2} \begin{bmatrix} 4 & -2 \ -3 & 1 \end{bmatrix} = \begin{bmatrix} -2 & 1 \ 3/2 & -1/2 \end{bmatrix}$
Then, we compute $A = X^{-1}B$:
$A = \begin{bmatrix} -2 & 1 \ 3/2 & -1/2 \end{bmatrix} \begin{bmatrix} 5 & 6 \ 7 & 8 \end{bmatrix} = \begin{bmatrix} -10+7 & -12+8 \ 15/2-7/2 & 18/2-8/2 \end{bmatrix} = \begin{bmatrix} -3 & -4 \ 4 & 5 \end{bmatrix}$
Honestly, this part trips people up more than it should.
Thus, $A = \begin{bmatrix} -3 & -4 \\ 4 & 5 \end{bmatrix}$.
The Equation $XAY = B$
This equation involves solving for $A$ when it is pre-multiplied by $X$ and post-multiplied by $Y$, where $X$, $Y$, and $B$ are known matrices But it adds up..
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Condition for Solution: For a solution to exist, the dimensions of $X$, $A$, $Y$, and $B$ must be compatible. Specifically, if $X$ is $m \times n$, $A$ is $n \times p$, and $Y$ is $p \times q$, then $B$ must be $m \times q$ Easy to understand, harder to ignore..
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Solution: If $X$ and $Y$ are invertible, the solution is:
$XAY = B$
$X^{-1}XAYY^{-1} = X^{-1}BY^{-1}$
$A = X^{-1}BY^{-1}$
Here, $X^{-1}$ and $Y^{-1}$ are the inverses of matrices $X$ and $Y$, respectively Small thing, real impact..
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Non-Invertible $X$ and $Y$: If $X$ and $Y$ are not invertible, we use the Moore-Penrose pseudoinverses $X^+$ and $Y^+$:
$A = X^+BY^+$
This solution minimizes $||XAY - B||_F$ It's one of those things that adds up..
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Example: Let's consider the matrices:
$X = \begin{bmatrix} 1 & 2 \ 3 & 4 \end{bmatrix}$, $Y = \begin{bmatrix} 5 & 6 \ 7 & 8 \end{bmatrix}$, and $B = \begin{bmatrix} 9 & 10 \ 11 & 12 \end{bmatrix}$
First, we find the inverses of $X$ and $Y$:
$X^{-1} = \begin{bmatrix} -2 & 1 \ 3/2 & -1/2 \end{bmatrix}$ and $Y^{-1} = \frac{1}{(5 \cdot 8 - 6 \cdot 7)} \begin{bmatrix} 8 & -6 \ -7 & 5 \end{bmatrix} = -\frac{1}{2} \begin{bmatrix} 8 & -6 \ -7 & 5 \end{bmatrix} = \begin{bmatrix} -4 & 3 \ 7/2 & -5/2 \end{bmatrix}$
Then, we compute $A = X^{-1}BY^{-1}$:
$A = \begin{bmatrix} -2 & 1 \ 3/2 & -1/2 \end{bmatrix} \begin{bmatrix} 9 & 10 \ 11 & 12 \end{bmatrix} \begin{bmatrix} -4 & 3 \ 7/2 & -5/2 \end{bmatrix}$
First, we compute the product of the first two matrices:
$\begin{bmatrix} -2 & 1 \ 3/2 & -1/2 \end{bmatrix} \begin{bmatrix} 9 & 10 \ 11 & 12 \end{bmatrix} = \begin{bmatrix} -18+11 & -20+12 \ 27/2-11/2 & 30/2-12/2 \end{bmatrix} = \begin{bmatrix} -7 & -8 \ 8 & 9 \end{bmatrix}$
Then, we compute the product of the result and $Y^{-1}$:
$A = \begin{bmatrix} -7 & -8 \ 8 & 9 \end{bmatrix} \begin{bmatrix} -4 & 3 \ 7/2 & -5/2 \end{bmatrix} = \begin{bmatrix} 28-28 & -21+20 \ -32+63/2 & 24-45/2 \end{bmatrix} = \begin{bmatrix} 0 & -1 \ -1/2 & 3/2 \end{bmatrix}$
Thus, $A = \begin{bmatrix} 0 & -1 \ -1/2 & 3/2 \end{bmatrix}$ And it works..
Finding A with Specific Properties
Sometimes, the requirement is to find a matrix $A$ with certain specific properties Not complicated — just consistent..
Symmetric Matrix
A matrix $A$ is symmetric if $A = A^T$, where $A^T$ is the transpose of $A$. But to find a symmetric matrix $A$, we need to check that the elements satisfy $a_{ij} = a_{ji}$ for all $i$ and $j$. * Example: Find a $3 \times 3$ symmetric matrix $A$.
$A = \begin{bmatrix} a & b & c \\ b & d & e \\ c & e & f \end{bmatrix}$
Here, $a, b, c, d, e, f$ can be any real numbers. As an example, we can set $a = 1, b = 2, c = 3, d = 4, e = 5, f = 6$.
Then,
$A = \begin{bmatrix} 1 & 2 & 3 \\ 2 & 4 & 5 \\ 3 & 5 & 6 \end{bmatrix}$
Orthogonal Matrix
A matrix $A$ is orthogonal if $AA^T = A^TA = I$, where $I$ is the identity matrix. In practice, the columns (and rows) of an orthogonal matrix are orthonormal vectors. Finding an orthogonal matrix involves ensuring that the dot product of each distinct pair of columns (or rows) is zero and that each column (or row) has a Euclidean norm of 1.
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Example: Find a $2 \times 2$ orthogonal matrix $A$.
Let $A = \begin{bmatrix} a & b \ c & d \end{bmatrix}$.
For $A$ to be orthogonal, we need:
$AA^T = \begin{bmatrix} a & b \ c & d \end{bmatrix} \begin{bmatrix} a & c \ b & d \end{bmatrix} = \begin{bmatrix} a^2 + b^2 & ac + bd \ ac + bd & c^2 + d^2 \end{bmatrix} = \begin{bmatrix} 1 & 0 \ 0 & 1 \end{bmatrix}$
This gives us the equations:
- $a^2 + b^2 = 1$
- $c^2 + d^2 = 1$
- $ac + bd = 0$
A general solution is:
$A = \begin{bmatrix} \cos(\theta) & -\sin(\theta) \ \sin(\theta) & \cos(\theta) \end{bmatrix}$
Here's a good example: if $\theta = \frac{\pi}{4}$:
$A = \begin{bmatrix} \frac{\sqrt{2}}{2} & -\frac{\sqrt{2}}{2} \ \frac{\sqrt{2}}{2} & \frac{\sqrt{2}}{2} \end{bmatrix}$
Involutory Matrix
A matrix $A$ is involutory if $A^2 = I$, where $I$ is the identity matrix.
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Example: Find a $2 \times 2$ involutory matrix $A$.
Let $A = \begin{bmatrix} a & b \ c & d \end{bmatrix}$ Simple as that..
For $A$ to be involutory, we need:
$A^2 = \begin{bmatrix} a & b \ c & d \end{bmatrix} \begin{bmatrix} a & b \ c & d \end{bmatrix} = \begin{bmatrix} a^2 + bc & ab + bd \ ac + cd & bc + d^2 \end{bmatrix} = \begin{bmatrix} 1 & 0 \ 0 & 1 \end{bmatrix}$
This gives us the equations:
- $a^2 + bc = 1$
- $d^2 + bc = 1$
- $ab + bd = 0$
- $ac + cd = 0$
From equations 3 and 4, we have $b(a + d) = 0$ and $c(a + d) = 0$. If $a + d \neq 0$, then $b = 0$ and $c = 0$, leading to $a^2 = 1$ and $d^2 = 1$. Thus, $a = \pm 1$ and $d = \pm 1$.
This is the bit that actually matters in practice.
If $a + d = 0$, then $d = -a$, and $a^2 + bc = 1$.
A simple solution is:
$A = \begin{bmatrix} 1 & 0 \\ 0 & -1 \end{bmatrix}$
Another solution is:
$A = \begin{bmatrix} 0 & 1 \\ 1 & 0 \end{bmatrix}$
Nilpotent Matrix
A matrix $A$ is nilpotent if there exists a positive integer $k$ such that $A^k = 0$, where $0$ is the zero matrix. In practice, the smallest such $k$ is the nilpotency index. * Example: Find a $2 \times 2$ nilpotent matrix $A$.
Let $A = \begin{bmatrix} a & b \\ c & d \end{bmatrix}$.
For $A$ to be nilpotent, we need $A^2 = 0$:
$A^2 = \begin{bmatrix} a & b \\ c & d \end{bmatrix} \begin{bmatrix} a & b \\ c & d \end{bmatrix} = \begin{bmatrix} a^2 + bc & ab + bd \\ ac + cd & bc + d^2 \end{bmatrix} = \begin{bmatrix} 0 & 0 \\ 0 & 0 \end{bmatrix}$
This gives us the equations:
1. $a^2 + bc = 0$
2. $ab + bd = 0$
3. $ac + cd = 0$
4. $bc + d^2 = 0$
From equations 2 and 3, we have $b(a + d) = 0$ and $c(a + d) = 0$. If $a + d \neq 0$, then $b = 0$ and $c = 0$, leading to $a^2 = 0$ and $d^2 = 0$.
Thus, $a = 0$ and $d = 0$.
If $a + d = 0$, then $d = -a$, and $a^2 + bc = 0$. Thus, $bc = -a^2$.
A simple solution is:
$A = \begin{bmatrix} 0 & 1 \\ 0 & 0 \end{bmatrix}$
Another solution is:
$A = \begin{bmatrix} a & b \\ -a^2/b & -a \end{bmatrix}$
Eigenvalue and Eigenvector Constraints
Another type of condition involves specifying eigenvalues and eigenvectors That's the part that actually makes a difference..
Finding A with Specific Eigenvalues
If we want to find a matrix $A$ with specific eigenvalues $\lambda_1, \lambda_2, \dots, \lambda_n$, we can use the following approach:
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Diagonal Matrix: Start with a diagonal matrix $D$ with the desired eigenvalues on the diagonal:
$D = \begin{bmatrix} \lambda_1 & 0 & \dots & 0 \ 0 & \lambda_2 & \dots & 0 \ \vdots & \vdots & \ddots & \vdots \ 0 & 0 & \dots & \lambda_n \end{bmatrix}$
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Change of Basis: Choose an invertible matrix $P$ (change of basis matrix). On top of that, 3. Transformation: Compute $A = PDP^{-1}$ That's the part that actually makes a difference..
The matrix $A$ will have the same eigenvalues as $D$, namely $\lambda_1, \lambda_2, \dots, \lambda_n$.
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Example: Find a $2 \times 2$ matrix $A$ with eigenvalues $\lambda_1 = 1$ and $\lambda_2 = 2$ And that's really what it comes down to..
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Let $D = \begin{bmatrix} 1 & 0 \ 0 & 2 \end{bmatrix}$.
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Choose an invertible matrix, say $P = \begin{bmatrix} 1 & 1 \ 0 & 1 \end{bmatrix}$. Then, $P^{-1} = \begin{bmatrix} 1 & -1 \ 0 & 1 \end{bmatrix}$ Simple, but easy to overlook..
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Compute $A = PDP^{-1}$:
$A = \begin{bmatrix} 1 & 1 \ 0 & 1 \end{bmatrix} \begin{bmatrix} 1 & 0 \ 0 & 2 \end{bmatrix} \begin{bmatrix} 1 & -1 \ 0 & 1 \end{bmatrix} = \begin{bmatrix} 1 & 2 \ 0 & 2 \end{bmatrix} \begin{bmatrix} 1 & -1 \ 0 & 1 \end{bmatrix} = \begin{bmatrix} 1 & 1 \ 0 & 2 \end{bmatrix}$
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Most guides skip this. Don't Small thing, real impact..
Thus, $A = \begin{bmatrix} 1 & 1 \\ 0 & 2 \end{bmatrix}$ has eigenvalues 1 and 2.
Finding A with Specific Eigenvectors
If we want to find a matrix $A$ with specific eigenvectors $v_1, v_2, \dots, v_n$ corresponding to eigenvalues $\lambda_1, \lambda_2, \dots, \lambda_n$, we can construct the matrix $A$ as follows:
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Eigenvector Matrix: Form a matrix $P$ with the eigenvectors as columns:
$P = \begin{bmatrix} | & | & & | \ v_1 & v_2 & \dots & v_n \ | & | & & | \end{bmatrix}$
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Eigenvalue Matrix: Form a diagonal matrix $D$ with the corresponding eigenvalues on the diagonal:
$D = \begin{bmatrix} \lambda_1 & 0 & \dots & 0 \ 0 & \lambda_2 & \dots & 0 \ \vdots & \vdots & \ddots & \vdots \ 0 & 0 & \dots & \lambda_n \end{bmatrix}$
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Transformation: Compute $A = PDP^{-1}$.
The matrix $A$ will have the specified eigenvectors and eigenvalues.
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Example: Find a $2 \times 2$ matrix $A$ with eigenvector $v_1 = \begin{bmatrix} 1 \ 0 \end{bmatrix}$ corresponding to eigenvalue $\lambda_1 = 1$ and eigenvector $v_2 = \begin{bmatrix} 1 \ 1 \end{bmatrix}$ corresponding to eigenvalue $\lambda_2 = 2$.
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Let $P = \begin{bmatrix} 1 & 1 \ 0 & 1 \end{bmatrix}$.
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Let $D = \begin{bmatrix} 1 & 0 \ 0 & 2 \end{bmatrix}$.
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Compute $P^{-1} = \begin{bmatrix} 1 & -1 \ 0 & 1 \end{bmatrix}$.
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Compute $A = PDP^{-1}$:
$A = \begin{bmatrix} 1 & 1 \ 0 & 1 \end{bmatrix} \begin{bmatrix} 1 & 0 \ 0 & 2 \end{bmatrix} \begin{bmatrix} 1 & -1 \ 0 & 1 \end{bmatrix} = \begin{bmatrix} 1 & 2 \ 0 & 2 \end{bmatrix} \begin{bmatrix} 1 & -1 \ 0 & 1 \end{bmatrix} = \begin{bmatrix} 1 & 1 \ 0 & 2 \end{bmatrix}$
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The official docs gloss over this. That's a mistake.
Thus, $A = \begin{bmatrix} 1 & 1 \\ 0 & 2 \end{bmatrix}$ has the specified eigenvectors and eigenvalues.
Advanced Techniques
For more complex conditions, one might need to resort to advanced techniques And that's really what it comes down to..
Singular Value Decomposition (SVD)
SVD can be used to find a matrix $A$ that best approximates a given matrix $B$ under certain constraints. Here's one way to look at it: if we want to find a matrix $A$ of a specific rank that is closest to $B$ in the Frobenius norm, we can use SVD.
- Compute SVD: Compute the SVD of $B = U\Sigma V^*$, where $U$ and $V$ are unitary matrices, and $\Sigma$ is a diagonal matrix with singular values $\sigma_1 \geq \sigma_2 \geq \dots \geq \sigma_n \geq 0$.
- Rank Reduction: To find a matrix $A$ of rank $k$ that minimizes $||A - B||_F$, set all but the largest $k$ singular values to zero, creating a new diagonal matrix $\Sigma_k$.
- Reconstruct A: $A = U\Sigma_k V^*$.
Optimization Techniques
In some cases, finding a matrix $A$ might require solving an optimization problem. To give you an idea, if the conditions on $A$ are expressed as a minimization problem:
$\text{minimize } f(A) \text{ subject to } g(A) = 0 \text{ and } h(A) \leq 0$
where $f$ is the objective function, $g$ represents equality constraints, and $h$ represents inequality constraints. Common optimization techniques include gradient descent, Newton's method, and linear programming.
Conclusion
Finding a matrix $A$ that satisfies given conditions is a diverse problem in linear algebra. In real terms, the methods to find $A$ depend heavily on the specific conditions imposed, ranging from simple matrix equations to more complex constraints involving eigenvalues, eigenvectors, and other matrix properties. By understanding these various scenarios and techniques, one can effectively approach and solve a wide range of matrix-related problems.