Undergrad Non-Hermitian wavefunctions and their solutions

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The discussion centers on the challenges of working with non-Hermitian wavefunctions in quantum mechanics and the derivation of real observable values through numerical methods. Participants express concerns about the foundational knowledge required to engage with this topic, suggesting that understanding linear algebra and quantum mechanics basics is essential. A proposed method involves expanding non-Hermitian functions into power series and evaluating their components, although this approach raises questions about the validity of the results. The conversation highlights the importance of distinguishing between wavefunctions and operators, emphasizing that the hermicity of operators is crucial in quantum mechanics. Ultimately, constructing wavepackets is suggested as a potential solution for obtaining meaningful results from non-Hermitian models.
SemM
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I was wondering if anyone has worked with non-Hermitian wavefunctions, and know of an approach to derive real and trivial values for their observables using numerical calculations?

Cheers
 
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What's a non-Hermitian wave function?
 
SemM said:
I was wondering if anyone has worked with non-Hermitian wavefunctions, and know of an approach to derive real and trivial values for their observables using numerical calculations?

Cheers

Your posts are fascinating. You seem to be ploughing through QM without having learned the basics - and having no intention of learning the basics. Perhaps eventually you will be able to put things together consistently without ever having learned, say, the definition of and difference between a vector and an operator!

Personally, I doubt it. I recommend a first course in linear algebra.
 
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PeroK said:
Your posts are fascinating. You seem to be ploughing through QM without having learned the basics - and having no intention of learning the basics. Perhaps eventually you will be able to put things together consistently without ever having learned, say, the definition of and difference between a vector and an operator!

Personally, I doubt it. I recommend a first course in linear algebra.

Haha, thanks , it is indeed true, but its not true that I don't want to learn the basics. I did an engineering in chemistry, with plenty of math, but zero QM. All QM is by self-learning, so, given the interest in important subjects, coupled with no experience in courses in QM, a bunch of strange questions do indeed arise.

I thought about a solution to this original question, but I am not sure:

What if I expand the function which has no hermitian counter-part in terms of a power-series, then I perform the evaluation of each series component using the form ##\langle \psi | d/dx | \psi*\rangle## and at the end sum up only those that have a hermitian counterpart? Sounds like a lazy form of shortcutting to me, but maybe its the only way to get some estimate. However, a closer thought suggests that each component of a series of say ##e^{-kx}## would be something like ##1/x-2/x^2-3/x^4-1/x^8+..## which have no hermitian counterpart. So back at the original question.
 
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SemM said:
I'm not aware of any significant work on the hermicity of wave functions. In QM, what is important is the hermicity of operators, which is what the link you posted above is about. This is also, I think, what has triggered @PeroK's reply. You seem to be confusing operators and wave functions.

To come back to the OP, most often the eigenfunctions of Hamiltonians can be chosen purely real, so they are definitely not Hermitian functions.

SemM said:
##\langle \psi | d/dx | \psi*\rangle##
This notation doesn't make sense to me. If you are using the Dirac notation, then there is no particular basis, so the ##d/dx## of a ket doesn't make sense. Likewise for the inclusion of a ##^*## in the ket, if it is to mean complex conjugation.
 
DrClaude said:
I'm not aware of any significant work on the hermicity of wave functions. In QM, what is important is the hermicity of operators, which is what the link you posted above is about. This is also, I think, what has triggered @PeroK's reply. You seem to be confusing operators and wave functions.

To come back to the OP, most often the eigenfunctions of Hamiltonians can be chosen purely real, so they are definitely not Hermitian functions.This notation doesn't make sense to me. If you are using the Dirac notation, then there is no particular basis, so the ##d/dx## of a ket doesn't make sense. Likewise for the inclusion of a ##^*## in the ket, if it is to mean complex conjugation.
It is difficult to use a common language here, because some are physicsts and some are mathematicians. This Dirac notation can also be given as

\begin{equation}
\int \psi p \psi^*dx
\end{equation}

and is the expectation value of the momentum operator.

Thanks
 
SemM said:
because some are physicsts and some are mathematicians
This ha nothing to do with it. What you wrote simply does not make any sense. It is definitely not the same as you wrote in your last post. I would suggest taking three steps back and learn the fundamentals of Hilbert spaces and Dirac notation to represent elements in the Hilbert space.
 
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Anyway, the solution to this problem is to construct wavepackets, for those who are wondering, or should the original Hamiltonian be non-Hermitian, then refer to "Making sense of non-Hermitian Hamiltonians" by Carl Bender.

These conversations must yield an answer and not just critics, otherwise PF becomes a gladiator arena, with no pedagogic or informational role.
 
  • #11
SemM said:
Anyway, the solution to this problem is to construct wavepackets,
I don't get it. The most common wave packet, a Gaussian wave packet, can be purely real, hence non-Hermitian.

SemM said:
These conversations must yield an answer and not just critics, otherwise PF becomes a gladiator arena, with no pedagogic or informational role.
The problem is the questions you ask, along with the replies you give, show a lack of basic knowledge. It is extremely pedagogical for people to reply that you must take steps back and try and get proper basic knowledge first.

Let me translate what these threads of yours sound to me. OP: "What is the colour of a hydrogen atom?" Followed up by question asking what do you mean by color of an atom, and a back and forth about basic principles, to be concluded by you saying "You should simply have answered blue."
 
  • #12
DrClaude said:
I don't get it. The most common wave packet, a Gaussian wave packet, can be purely real, hence non-Hermitian.The problem is the questions you ask, along with the replies you give, show a lack of basic knowledge. It is extremely pedagogical for people to reply that you must take steps back and try and get proper basic knowledge first.

Let me translate what these threads of yours sound to me. OP: "What is the colour of a hydrogen atom?" Followed up by question asking what do you mean by color of an atom, and a back and forth about basic principles, to be concluded by you saying "You should simply have answered blue."

I didnt say the wavepacket must be non-hermitian. I said that constructing wavepackets is a way to find a solution to a model that does not give real and trivial expectation values for its observables.
 

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