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Determine the invariant subspace of \(A=\left[\begin{array}{ll}2 & -4 \\ 5 & -2\end{array}\right]\) viewed as a linear operator on (a) \(\mathbf{R}^{2},(\mathrm{b}) \mathbf{C}^{2}\).

Short Answer

Expert verified
For the linear operator A, there are no invariant subspaces in 鈩澛 since the eigenvectors are not real. However, in 鈩偮, there are two invariant subspaces: 1. The line spanned by the eigenvector associated with eigenvalue 位鈧, given by x鈧 = \((2 - 2\sqrt{2})x鈧乗) / 4. 2. The line spanned by the eigenvector associated with eigenvalue 位鈧, given by x鈧 = \((2 + 2\sqrt{2})x鈧乗) / 4.

Step by step solution

01

Find the eigenvalues of A

To find the eigenvalues of A, we need to solve the characteristic equation, given by det(A - 位I) = 0, where 位 is an eigenvalue and I is the identity matrix. For A = \(\begin{bmatrix} 2 & -4\\ 5 & -2 \end{bmatrix}\), we get: \(|A - 位I| = \begin{vmatrix} 2 - 位 & -4 \\ 5 & -2 - 位 \end{vmatrix} = (2 - 位)(-2 - 位) - (-4)(5) = 位虏 - 8\)
02

Solve for the eigenvalues 位

To determine the eigenvalues, we solve the equation 位虏 - 8 = 0. 位虏 - 8 = (位 + 2\(\sqrt{2}\))(位 - 2\(\sqrt{2}\)) = 0 Therefore, we have two eigenvalues: 位鈧 = 2\(\sqrt{2}\) and 位鈧 = -2\(\sqrt{2}\).
03

Find the eigenvectors of A

For each eigenvalue, we want to solve (A - 位I)x = 0, where x is an eigenvector. For 位鈧 = 2\(\sqrt{2}\): \( (A - 位鈧両)x = \begin{bmatrix} 2 - 2\sqrt{2} & -4 \\ 5 & -2 + 2\sqrt{2} \end{bmatrix} \begin{bmatrix} x鈧 \\ x鈧 \end{bmatrix} = \begin{bmatrix} 0 \\ 0 \end{bmatrix}\) The system of equations can be simplified to: \( (2 - 2\sqrt{2})x鈧 - 4x鈧 = 0 \) \( 5x鈧 + (2\sqrt{2} - 2)x鈧 = 0 \) Any non-zero solution to this system is an eigenvector, observing that, x鈧 = \((2 - 2\sqrt{2})x鈧乗) / 4 is a valid eigenvector. For 位鈧 = -2\(\sqrt{2}\): \( (A - 位鈧侷)x = \begin{bmatrix} 2 + 2\sqrt{2} & -4 \\ 5 & -2 - 2\sqrt{2} \end{bmatrix} \begin{bmatrix} x鈧 \\ x鈧 \end{bmatrix} = \begin{bmatrix} 0 \\ 0 \end{bmatrix}\) This system of equations also leads to x鈧 = \((2 + 2\sqrt{2})x鈧乗) / 4 being a valid eigenvector.
04

Determine the invariant subspaces

The eigenvectors form the invariant subspaces for the linear operator A. (a) When A acts on 鈩澛: The eigenvectors corresponding to 位鈧 and 位鈧 are not real, so there are no invariant subspaces in 鈩澛. (b) When A acts on 鈩偮: The eigenvectors form two distinct lines: Invariant subspace 1: The line spans by the eigenvector associated with eigenvalue 位鈧, given by x鈧 = \((2 - 2\sqrt{2})x鈧乗) / 4. Invariant subspace 2: The line spans by the eigenvector associated with eigenvalue 位鈧, given by x鈧 = \((2 + 2\sqrt{2})x鈧乗) / 4. These two lines are the invariant subspaces of A acting as a linear operator on 鈩偮.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Eigenvalues
When we speak about eigenvalues, we're referring to special numbers associated with a matrix or a linear transformation鈥攊n this case, the matrix \(A\). These numbers give us insight into the behavior of the transformation. To find them, we solve the characteristic equation \(\text{det}(A - \lambda I) = 0\), where \(I\) represents the identity matrix and \(\lambda\) the eigenvalues we seek.
In our example, the characteristic equation simplifies to \(\lambda^2 - 8 = 0\). Solving gives us the eigenvalues \(\lambda_1 = 2\sqrt{2}\) and \(\lambda_2 = -2\sqrt{2}\). These hint at the directions along which our transformation affects the vector space most distinctly. Understanding eigenvalues is crucial as they relate closely to invariant subspaces, helping in predicting the transformation's effects.
Eigenvectors
Eigenvectors accompany eigenvalues and represent the directions in which the linear transformation stretches or compresses the space. Calculating them involves solving \((A - \lambda I)\mathbf{x} = 0\), where \(\mathbf{x}\) is the eigenvector of interest.
For our matrix \(A\) with eigenvalues \(\lambda_1 = 2\sqrt{2}\) and \(\lambda_2 = -2\sqrt{2}\), we solve separately for each \(\lambda\). The solutions \(x_2 = \frac{(2 - 2\sqrt{2})x_1}{4}\) and \(x_2 = \frac{(2 + 2\sqrt{2})x_1}{4}\) describe the eigenvectors.
These vectors pinpoint directions that remain unchanged in direction under transformation by \(A\), highlighting the shape and orientation of invariant subspaces.
Linear Operator
A linear operator can be thought of as a function mapping vectors to vectors in a linear manner. It means if you apply the operator to a combination of vectors, the result is the same as applying the operator to each vector individually and combining the results. In mathematical terms, if \(T\) is our linear operator, then \(T(a\mathbf{u} + b\mathbf{v}) = aT(\mathbf{u}) + bT(\mathbf{v})\) for any scalars \(a, b\) and vectors \(\mathbf{u}, \mathbf{v}\).
Our matrix \(A = \begin{bmatrix} 2 & -4 \ 5 & -2 \end{bmatrix}\) acts as a linear operator, transforming input vectors. The way it transforms vectors is encapsulated by its eigenvalues and eigenvectors, and profoundly affects the concept of invariant subspaces. This transformation is explored in both real and complex vector spaces, revealing more structure in the latter due to the nature of complex numbers.
Complex Vector Space
A complex vector space extends the idea of real vector spaces by allowing vectors to have complex numbers as components. This flexibility is fundamental in finding solutions to certain equations, like differential equations, that might not have real-number solutions.
In our exercise, the matrix \(A\) exhibited no real invariant subspaces when acting on \(\mathbb{R}^2\), due to its complex eigenvalues and eigenvectors. However, when considered in \(\mathbb{C}^2\), it shows two invariant subspaces corresponding to its complex eigenvectors.
  • Invariant Subspace 1: Defined by the eigenvector related to \(\lambda_1 = 2\sqrt{2}\), with the relational equation \(x_2 = \frac{(2 - 2\sqrt{2})x_1}{4}\).
  • Invariant Subspace 2: Defined by the eigenvector linked to \(\lambda_2 = -2\sqrt{2}\), with \(x_2 = \frac{(2 + 2\sqrt{2})x_1}{4}\).

Understanding the complex vector space's role is crucial for delving deeper into linear algebra, facilitating solutions that real numbers alone can't provide.

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Most popular questions from this chapter

Prove Theorem 10.1: Let \(T: V \rightarrow V\) be a linear operator whose characteristic polynomial factors into linear polynomials. Then \(V\) has a basis in which \(T\) is represented by a triangular matrix. The proof is by induction on the dimension of \(V\). If \(\operatorname{dim} V=1\), then every matrix representation of \(T\) is a \(1 \times 1\) matrix, which is triangular. Now suppose \(\operatorname{dim} V=n>1\) and that the theorem holds for spaces of dimension less than \(n\). Because the characteristic polynomial of \(T\) factors into linear polynomials, \(T\) has at least one eigenvalue and so at least one nonzero eigenvector \(v,\) say \(T(v)=a_{11} v .\) Let \(W\) be the one- dimensional subspace spanned by \(v\) Set \(\bar{V}=V / W .\) Then (Problem 10.26 ) \(\operatorname{dim} \bar{V}=\operatorname{dim} V-\operatorname{dim} W=n-1 .\) Note also that \(W\) is invariant under \(T .\) By Theorem \(10.16, T\) induces a linear operator \(T\) on \(V\) whose minimal polynomial divides the minimal polynomial of \(T .\) Because the characteristic polynomial of \(T\) is a product of linear polynomials, so is its minimal polynomial, and hence, so are the minimal and characteristic polynomials of \(\bar{T}\). Thus, \(\bar{V}\) and \(\bar{T}\) satisfy the hypothesis of the theorem. Hence, by induction, there exists a basis \(\left\\{\bar{v}_{2}, \ldots, \bar{v}_{n}\right\\}\) of \(\bar{V}\) such that \\[ \begin{array}{l} \bar{T}\left(\bar{v}_{2}\right)=a_{22} \bar{v}_{2} \\ \bar{T}\left(\bar{v}_{3}\right)=a_{32} \bar{v}_{2}+a_{33} \bar{v}_{3} \\ \bar{T}\left(\bar{v}_{n}\right)=a_{n 2} \bar{v}_{n}+a_{n 3} \bar{v}_{3}+\cdots+a_{n n} \bar{v}_{n} \end{array} \\] Now let \(v_{2}, \ldots, v_{n}\) be elements of \(V\) that belong to the cosets \(v_{2}, \ldots, v_{n},\) respectively. Then \(\left\\{v, v_{2}, \ldots, v_{n}\right\\}\) is a basis of \(V\) (Problem 10.26 ). Because \(\bar{T}\left(v_{2}\right)=a_{22} \bar{v}_{2},\) we have \\[ \bar{T}\left(\bar{v}_{2}\right)-a_{22} \bar{v}_{22}=0, \quad \text { and so } \quad T\left(v_{2}\right)-a_{22} v_{2} \in W \\] But \(W\) is spanned by \(v ;\) hence, \(T\left(v_{2}\right)-a_{22} v_{2}\) is a multiple of \(v,\) say, \\[ T\left(v_{2}\right)-a_{22} v_{2}=a_{21} v, \quad \text { and } \\] so \(\quad T\left(v_{2}\right)=a_{21} v+a_{22} v_{2}\) Similarly, for \(i=3, \ldots, n\) \\[ T\left(v_{i}\right)-a_{i 2} v_{2}-a_{i 3} v_{3}-\cdots-a_{i i} v_{i} \in W, \quad \text { and so } \quad T\left(v_{i}\right)=a_{i 1} v+a_{i 2} v_{2}+\cdots+a_{i i} v_{i} \\] Thus, \\[ T(v)=a_{11} v \\] \\[ \begin{array}{l} T\left(v_{2}\right)=a_{21} v+a_{22} v_{2} \\ T\left(v_{n}\right)=a_{n 1} v+a_{n 2} v_{2}+\cdots+a_{n n} v_{n} \end{array} \\] and hence the matrix of \(T\) in this basis is triangular.

Suppose \(A\) is a supertriangular matrix (i.e., all entries on and below the main diagonal are 0 ). Show that \(A\) is nilpotent.

Find the rational canonical form for the four-square Jordan block with \(\lambda^{\prime}\) s on the diagonal.

Let \(A=\left[\begin{array}{ccccc}0 & 1 & 1 & 0 & 1 \\ 0 & 0 & 1 & 1 & 1 \\ 0 & 0 & 0 & 0 & 0 \\ 0 & 0 & 0 & 0 & 0 \\ 0 & 0 & 0 & 0 & 0\end{array}\right]\) and \(B=\left[\begin{array}{ccccc}0 & 1 & 1 & 0 & 0 \\ 0 & 0 & 1 & 1 & 1 \\ 0 & 0 & 0 & 1 & 1 \\ 0 & 0 & 0 & 0 & 0 \\ 0 & 0 & 0 & 0 & 0\end{array}\right] .\) The reader can verify that \(A\) and \(B\) are both nilpotent of index \(3 ;\) that is, \(A^{3}=0\) but \(A^{2} \neq 0,\) and \(B^{3}=0\) but \(B^{2} \neq 0 .\) Find the nilpotent matrices \(M_{A}\) and \(M_{B}\) in canonical form that are similar to \(A\) and \(B,\) respectively. Because \(A\) and \(B\) are nilpotent of index \(3, M_{A}\) and \(M_{B}\) must each contain a Jordan nilpotent block of order \(3,\) and none greater then \(3 .\) Note that \(\operatorname{rank}(A)=2\) and \(\operatorname{rank}(B)=3,\) so nullity \((A)=5-2=3\) and nullity \((B)=5-3=2 .\) Thus, \(M_{A}\) must contain three diagonal blocks, which must be one of order 3 and two of order \(1 ;\) and \(M_{B}\) must contain two diagonal blocks, which must be one of order 3 and one of order 2 Namely, \\[ M_{A}=\left[\begin{array}{ccccc} 0 & 1 & 0 & 0 & 0 \\ 0 & 0 & 1 & 0 & 0 \\ 0 & 0 & 0 & 0 & 0 \\ 0 & 0 & 0 & 0 & 0 \\ 0 & 0 & 0 & 0 & 0 \end{array}\right] \quad \text { and } \quad M_{B}=\left[\begin{array}{ccccc} 0 & 1 & 0 & 0 & 0 \\ 0 & 0 & 1 & 0 & 0 \\ 0 & 0 & 0 & 0 & 0 \\ 0 & 0 & 0 & 0 & 1 \\ 0 & 0 & 0 & 0 & 0 \end{array}\right] \\]

Let \(U\) and \(W\) be subspaces of \(V\) such that \(W \subset U \subset V .\) Note that any coset \(u+W\) of \(W\) in \(U\) may also be viewed as a coset of \(W\) in \(V\), because \(u \in U\) implies \(u \in V ;\) hence, \(U / W\) is a subset of \(V / W\). Prove that (i) \(U / W\) is a subspace of \(V / W\) (ii) \(\operatorname{dim}(V / W)-\operatorname{dim}(U / W)=\operatorname{dim}(V / U)\)

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