/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 77 Suppose \(A\) is a complex matri... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

Suppose \(A\) is a complex matrix. Show that \(A A^{H}\) and \(A^{H} A\) are Hermitian.

Short Answer

Expert verified
We showed that \(AA^H\) and \(A^H A\) are both Hermitian by using properties of conjugate transpose and matrix multiplication. Specifically, we demonstrated that \((AA^H)^H = AA^H\) and \((A^H A)^H = A^H A\), which confirms that both products are Hermitian matrices as they are equal to their conjugate transpose.

Step by step solution

01

Compute the conjugate transpose of AA^H

First, let's find the conjugate transpose of the matrix product AA^H. To do this, we must use the properties of conjugate transpose and matrix multiplication: (AA^H)^H = (A^H)^H A^H
02

Simplify (A^H)^H

Recall the property that taking the conjugate transpose twice will give you the original matrix back: (A^H)^H = A
03

Substitute back

Now we can substitute Step 2 back into the result from Step 1: (AA^H)^H = AA^H As we have shown that the conjugate transpose of AA^H is equal to AA^H itself, it follows that AA^H is Hermitian.
04

Compute the conjugate transpose of A^H A

Next, let's find the conjugate transpose of the matrix product A^H A. We will use the same properties as in Step 1: (A^H A)^H = AH A^H
05

Simplify substituting A^H

Recall from step 2 that the conjugate transpose of A^H is the original matrix A. Substitute this into the result from Step 4: (A^H A)^H = A^H A As the conjugate transpose of A^H A is equal to A^H A itself, it follows that A^H A is also Hermitian. Since we have proven that AA^H and A^H A are both Hermitian matrices, the given exercise is complete.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Find \(2 \times 2\) invertible matrices \(A\) and \(B\) such that \(A+B \neq 0\) and \(A+B\) is not invertible.

Pendular Motion. It is well known that the motion of a pendulum is approximated by the differential equation $$ \theta^{\prime \prime}+\frac{g}{l} \theta=0, $$where \(\theta(t)\) is the angle in radians that the pendulum makes with a vertical line at time \(t\) (see Figure 2.8), interpreted so that \(\theta\) is positive if the pendulum is to the right and negative if the pendulum is to the left of the vertical line as viewed by the reader. Here \(l\) is the length of the pendulum and \(g\) is the magnitude of acceleration due to gravity. The variable \(t\) and constants \(l\) and \(g\) must be in compatible units (e.g., \(t\) in seconds, \(l\) in meters, and \(g\) in meters per second per second). (a) Express an arbitrary solution to this equation as a linear combination of two real-valued solutions. (b) Find the unique solution to the equation that satisfies the conditions $$ \theta(0)=\theta_{0}>0 \text { and } \theta^{\prime}(0)=0 \text {. } $$ (The significance of these conditions is that at time \(t=0\) the pendulum is released from a position displaced from the vertical by \(\theta_{0}\).) (c) Prove that it takes \(2 \pi \sqrt{l / g}\) units of time for the pendulum to make one circuit back and forth. (This time is called the period of the pendulum.)

Find the inverses of \(A=\left[\begin{array}{lll}1 & 1 & 2 \\ 1 & 2 & 5 \\ 1 & 3 & 7\end{array}\right]\) and \(B=\left[\begin{array}{rrr}1 & -1 & 1 \\ 0 & 1 & -1 \\ 1 & 3 & -2\end{array}\right] .[\text { Hint: See Problem } 2.19 .]\)

Let \(V\) and \(W\) be vector spaces with subspaces \(V_{1}\) and \(W_{1}\), respectively. If \(\mathrm{T}: \mathrm{V} \rightarrow \mathrm{W}\) is linear, prove that \(\mathrm{T}\left(\mathrm{V}_{1}\right)\) is a subspace of \(\mathrm{W}\) and that $\left\\{x \in \mathrm{V}: \mathrm{T}(x) \in \mathrm{W}_{1}\right\\}\( is a subspace of \)\mathrm{V}$.

Prove the following generalization of Theorem 2.23. Let $\mathrm{T}: \mathrm{V} \rightarrow \mathrm{W}$ be a linear transformation from a finite- dimensional vector space \(V\) to a finite-dimensional vector space W. Let \(\beta\) and \(\beta^{\prime}\) be ordered bases for \(\mathrm{V}\), and let \(\gamma\) and \(\gamma^{\prime}\) be ordered bases for \(\mathrm{W}\). Then $[\mathrm{T}]_{\beta}^{\gamma}^{\prime}=P^{-1}[\mathrm{~T}]_{\beta}^{\gamma} Q\(, where \)Q\( is the matrix that changes \)\beta^{\prime}$-coordinates into \(\beta\)-coordinates and \(P\) is the matrix that changes \(\gamma^{\prime}\)-coordinates into \(\gamma\)-coordinates.

See all solutions

Recommended explanations on Math Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.