Help with expected value of non-hermitian operators

In summary, when dealing with a Hermitian operator, the expectation value can be calculated using the probabilities of each eigenvalue and the normalization of these values. However, for non-hermitian operators, there is no guarantee that the eigenbasis will be orthonormal, making it more difficult to calculate the expectation value. While there are some ways to adapt the formula for non-hermitian operators, it is important to be careful and consider the physics behind it. Quantum field theory is an example of a field where non-hermitian operators are used extensively.
  • #1
lemma28
18
1
I know that with an Hermitian operator the expectation value can be found by calculating the (relative) probabilities of each eigenvalue: square modulus of the projection of the state-vector along the corresponding eigenvector.
The normalization of these values give the absolute probabilities.
Alternatively it's possible to calculate directly the expectation value by the compact formula <A>=<psi|A|psi>.

I got stumbled considering what adjustment to take in case of an operator that is not Hermitian.
In this case the eigenbasis is not orthonormal. But I feel that there should be some way to calculate the expectation value of the operator nonetheless.

Am I wrong? Or there's no meaningful way to define it in the non hermitian case?

If the procedure is more or less the same with some adaptation to make then:

Which projection to take? the components in the eigenbasis or the orthogonal projections of psi along the eigenvectors?
Is there an analog of the formula <A>=<psi|A|psi> that is correct in the non.orthonormal basis?

Any help appreciated
Thanks
 
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  • #2
Well, the problem with the eigenbasis is even worse than you think it is. Let's use the harmonic oscillator as an example to illustrate a few points:

The creation operator has no eigenkets! To see this, let's take a look at what a normal eigenket would look like in the harmonic oscillator basis:
[tex]
| \lambda \rangle = \sum_n c_n |n \rangle
[/tex]
So, you act the raising operator on it, but where do you get the lowest nonzero term? Gotta create it from somewhere, but there's nothing there!

That said, the expectation value of an operator [tex]\mathcal{O}[/tex] for a state [tex]|\Psi\rangle[/tex] is pretty much defined as
[tex]
\langle \mathcal{O} \rangle = \langle \Psi | \left ( \mathcal{O} | \Psi \rangle \right )
[/tex]
For hermitian operators, the fact that the operator acts on the ket is irrelevent, but for non-hermitian operators, there is a possibly big difference, so you just have to be careful about what you do with non-hermitian operators more so than hermitian operators.
 
  • #4
lemma28:” Help with expected value of non-hermitian operators”

Quantum River:” there seems to be a lot of physics in the non-hermitian operators”

Notice that entire QFT is formulated in terms of non-hermitian operators (second quantization).
 

1. What is expected value in the context of non-hermitian operators?

Expected value refers to the average or most likely value of a specific variable or outcome. In the context of non-hermitian operators, it is a measure of the average value of an observable property of a quantum system.

2. How is expected value calculated for non-hermitian operators?

The expected value of a non-hermitian operator is calculated by taking the inner product of the operator with the quantum state vector, and then taking the complex conjugate of that inner product. This can be represented mathematically as ⟨Ψ|A|Ψ⟩*, where Ψ is the quantum state vector and A is the non-hermitian operator.

3. Can expected value be negative for non-hermitian operators?

Yes, the expected value of a non-hermitian operator can be negative. This is because non-hermitian operators can have complex eigenvalues, which can result in negative expected values. However, the overall expected value of a non-hermitian operator is still a useful measure of the average value of an observable property.

4. How is expected value used in quantum mechanics?

Expected value is an important concept in quantum mechanics as it allows us to make predictions about the behavior of quantum systems. By calculating the expected value of a non-hermitian operator, we can determine the most likely outcome of a measurement of that system.

5. Are there any limitations to using expected value for non-hermitian operators?

One limitation of using expected value for non-hermitian operators is that it does not provide us with information about the spread or variability of the values. Additionally, it may not accurately represent the behavior of highly entangled systems. Other measures, such as variance, may be more useful in these cases.

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