Quick question about Hermitian operators

In summary, Hermitian operators have real eigenvalues, but not all operators with real eigenvalues are Hermitian. A matrix is normal if and only if it can be diagonalized by a unitary transformation, and Hermitian matrices are always normal. However, abnormal matrices may have real eigenvalues and non-orthogonal eigenvectors.
  • #1
dEdt
288
2
If H is a Hermitian operator, then its eigenvalues are real. Is the converse true?
 
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  • #2
No. Take as counterexample the matrix [tex]\left(\begin{array}{cc} 0 & 1\\ 0 & 0 \end{array}\right).[/tex]
However, if you know that the operator is normal (that is: if [itex]AA^*=A^*A[/itex]), then it is true that it is Hermitian iff the eigenvalues are real.
 
  • #3
micromass said:
No. Take as counterexample the matrix [tex]\left(\begin{array}{cc} 0 & 1\\ 0 & 0 \end{array}\right).[/tex]
However, if you know that the operator is normal (that is: if [itex]AA^*=A^*A[/itex]), then it is true that it is Hermitian iff the eigenvalues are real.

Good counterexample!

A few more useful rules: a matrix ##M## has "good" eigenvectors if and only if it is normal. "Good" eigenvectors means it is possible to choose eigenvectors such that they form an orthonormal basis for whatever vector space ##M## acts on.

Equivalently, a matrix is normal if and only if it can be diagonalized by a unitary transformation:
##
M = U D U^{-1}
##
for some unitary matrix ##U## and diagonal matrix ##D## whose diagonal elements are eigenvalues of ##M##.

Hermitian matrices are always normal, and their eigenvalues are always real. But if ##M## is abnormal, it might have real eigenvalues and "bad" eigenvectors which are not orthogonal. Here's an example:

##
\left[\begin{array}{cc}
1 & 1 \\
0 & 2 \\
\end{array}\right]
##

This thing has eigenvalues 1 and 2, but its eigenvectors

##
\left[\begin{array}{c}
1 \\ 0 \\
\end{array}\right]
\quad
\left[\begin{array}{c}
1 \\ 1 \\
\end{array}\right]
##

are not orthogonal to each other.

The example micromass gave is even more badly-behaved: it is defective, which means it doesn't have enough linearly-independent eigenvectors to span the vector space. So we can't even form a "bad" basis using its eigenvectors.
 
Last edited:

What are Hermitian operators?

Hermitian operators are mathematical entities used in quantum mechanics to represent physical observables, such as position, momentum, and energy. They are self-adjoint operators that have the property of being equal to their own conjugate transpose.

What is the significance of Hermitian operators?

Hermitian operators have several important properties that make them useful in quantum mechanics. They have real eigenvalues, which correspond to measurable quantities in experiments. They also have orthogonal eigenvectors, which can be used to construct a complete basis for representing any quantum state.

How are Hermitian operators related to observables in quantum mechanics?

In quantum mechanics, physical observables are represented by Hermitian operators. The measurement of an observable corresponds to finding the eigenvalue of the associated Hermitian operator. This allows us to make predictions about the outcomes of measurements on quantum systems.

Can all operators in quantum mechanics be represented as Hermitian operators?

No, not all operators in quantum mechanics are Hermitian. However, any operator can be decomposed into a sum of a Hermitian operator and an anti-Hermitian operator. The Hermitian part represents the observable quantity, while the anti-Hermitian part has no physical meaning.

What is the relationship between Hermitian operators and unitary operators?

Unitary operators are a special type of Hermitian operator that represent transformations that preserve the length of a quantum state vector. This means that unitary operators are responsible for the time evolution of quantum systems. Additionally, Hermitian operators can be diagonalized using unitary operators.

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