Non-Hermitian wavefunctions and their solutions

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Discussion Overview

The discussion revolves around non-Hermitian wavefunctions and their implications for deriving real and trivial values for observables in quantum mechanics. Participants explore various approaches, definitions, and the mathematical framework surrounding the topic, including numerical calculations and the role of operators.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants inquire about the nature of non-Hermitian wavefunctions and their significance in quantum mechanics.
  • One participant suggests expanding non-Hermitian functions in a power series to evaluate observables, though they express uncertainty about the validity of this approach.
  • Another participant emphasizes the importance of the hermicity of operators rather than wavefunctions in quantum mechanics.
  • There is a discussion about the Dirac notation and its application, with some participants questioning the clarity of its use in the context of non-Hermitian wavefunctions.
  • A later reply proposes constructing wavepackets as a potential solution to the original question regarding non-Hermitian Hamiltonians.
  • Some participants express frustration with perceived gaps in foundational knowledge among others, suggesting that a better understanding of basic principles is necessary for productive discussion.
  • There is a contention regarding the nature of Gaussian wave packets and their relationship to hermicity, with differing views on whether they can be purely real and non-Hermitian.

Areas of Agreement / Disagreement

Participants do not reach consensus on the definitions and implications of non-Hermitian wavefunctions. Multiple competing views remain regarding the validity of proposed approaches and the foundational knowledge required to engage in the discussion.

Contextual Notes

Some statements reflect a lack of clarity in the definitions of terms such as "Hermitian" and "non-Hermitian," as well as the application of Dirac notation. There are unresolved questions about the mathematical treatment of wavefunctions and operators in quantum mechanics.

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.
 
Last edited:
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.
 
  • #10
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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