Eigenpairs and Hermitian matrices

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Homework Help Overview

The discussion revolves around constructing a Hermitian matrix given specific eigenpairs. Participants explore the properties of Hermitian matrices and the implications of choosing different eigenvalues and eigenvectors.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the choice of eigenvalues and eigenvectors, questioning whether any values can be selected. They also explore the relationship between eigenpairs and the construction of Hermitian matrices, considering the diagonalization process and the conditions for unitarity.

Discussion Status

The conversation is active, with participants providing insights into the construction of the matrix and the necessary conditions for it to be Hermitian. Some participants express confusion about the problem's complexity, while others clarify the requirements for the eigenvectors and their normalization.

Contextual Notes

Participants note that the problem may involve arbitrary choices for eigenvalues and eigenvectors, leading to discussions about the implications of these choices on the Hermitian matrix's properties.

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Homework Statement



Choose [tex]\lambda_{1}, \lambda_{2}, \lambda_{3}[/tex] along with a set of vectors [tex]{v_{1},v_{2},v_{3}}[/tex] and construct an Hermitian matrix H with the eigenpairs [tex](\lambda_{1},v_{1}),(\lambda_{2},v_{2}),(\lambda_{3},v_{3})[/tex]

Homework Equations





The Attempt at a Solution


[tex]\lambda_{1} = 2[/tex]
[tex]\lambda_{2} = -2[/tex]

[tex]v_{1} = \widehat{i}+2\widehat{j}[/tex]
[tex]v_{2} = \widehat{i}-2\widehat{j}[/tex]

[tex]u_{1} = \frac{1}{\sqrt{5}}\left(\widehat{i} + 2\widehat{j} \right)[/tex]
[tex]u_{2} = \frac{1}{\sqrt{5}}\left(\widehat{i} - 2\widehat{j}\right)[/tex]

[tex]v_{3} = u_{1} \times u_{2} = -\frac{4}{5}\widehat{k}[/tex]

[tex]u_{3} = -\widehat{k}[/tex]

[tex]Basis: \ U = \left\{ u_{1},u_{2},u_{3} \right}\}[/tex]

[tex]H = \left| \begin{array}{ccc} 2 & 0 & 0 \\ 0 & -2 & 0 \\ 0 & 0 & 1 \end{array} \right|[/tex]

How does this look?
 
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can you choose any values here?

why not just
[tex]\lambda_{1} = 1[/tex]
[tex]\lambda_{2} = 2[/tex]
[tex]\lambda_{3} = 3[/tex]

and
[tex]u_{1} = (1,0,0)[/tex]
[tex]u_{2} = (0,1,0)[/tex]
[tex]u_{3} = (0,0,1)[/tex]

then
[tex]H = \left| \begin{array}{ccc} 1 & 0 & 0 \\ 0 & 2& 0 \\ 0 & 0 & 3 \end{array} \right|[/tex]
 
If that's all this is, am I misunderstanding or is this a really trivial question?
 
maybe it asking if you are given arbitrary
[tex]u_1, u_2, u_3[/tex]
and corresponding eigenvalues
[tex]\lambda_1, \lambda_2, \lambda_3[/tex]
can you find a hermitian matrix H, with the given eigenpairs?

one way you could do is assume you have found H and it can be diagonalised (which you know it can, from the eigenvectors), then the diagonal form of H is
[tex]D = P^{-1}.H.P[/tex]

where
[tex]D = \left| \begin{array}{ccc} \lambda_1 & 0 & 0 \\ 0 & \lambda_2& 0 \\ 0 & 0 & \lambda_3 \end{array} \right|[/tex]

now the matrix P is simply given by the eigenvectors
where
[tex]P = \left| \begin{array}{ccc} u_1, u_2, u_3 \end{array} \right|[/tex]

then H is
[tex]H = PDP^{-1}[/tex]

that gives the eigenpairs, however I doubt it would automatically be hermitian... for that you need, where the star means conjugate transpose
[tex]H = H^*[/tex]


so running that through
[tex]PDP^{-1} = (PDP^{-1})^* = P^{-1}^*D^*P^* = P^{-1}^*DP^*[/tex]

hmmm... not totally sure where to go now
 
Last edited:
maybe a little left & right muliplication
[tex]D = P^{-1}(PDP^{-1})P = (P^{-1}P^{-1}^*)D(P^*P)[/tex]

this will be satisfied if P is unitary
[tex]P^*P = PP^* = I[/tex]
 
from before P is given by the eigenvectors (choose up to some multiplicative constant)
[tex]P = \left| \begin{array}{ccc} u_1, u_2, u_3 \end{array} \right|[/tex]

so in subscript form if j is the eigenvector and i is it's component, write
[tex]P = P_{ij} = u_{j}^{(i)}[/tex]

now for the transpose conjugate of a matrix
[tex]P^* = (P^*)_{ij} = \bar{P}_{ji} = \bar{u}_{i}^{(j)}[/tex]

matrix multipication is given by (with summation over the repeated indice)
[tex]P^*P = (P^*)_{ij}P_{jk} = \bar{u}_{i}^{(j)} u_{k}^{(j)}[/tex]
which looks just like a complex inner product between eigenvectors

so to satisfy the unitary condition we were looking for
[tex]PP^* = I \rightarrow \bar{u}_{i}^{(j)} u_{k}^{(j)} = \delta_{ik}[/tex]

ie. all the columns of P must form an orthonormal basis, which is a property of unitary matricies in general. So the condition will be satisfied if you just normalise your eigenvectors to length 1.

got a bit carried away there... but from this you should be able to write the general form of H no worries
 
Ok that helps. I guess I got confused and thought he was looking for D, but I think you're right; I think he's looking for PDP-1

Thanks!
 

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