Non-Hermitian operator for superposition

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Discussion Overview

The discussion revolves around the concept of non-Hermitian operators in quantum mechanics, particularly in relation to the possibility of observing a superposition state where a spin measurement yields both "up" and "down" results. Participants explore the implications of using non-Hermitian operators versus Hermitian operators, focusing on their roles in time evolution and measurement within quantum theory.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Exploratory

Main Points Raised

  • Some participants assert that no Hermitian operator allows for a time evolution where "I observed the spin to be both up and down" is a possible result.
  • Others clarify that the term "Hamiltonian operator" specifically refers to time evolution, while Hermitian operators relate to observables.
  • A participant questions the use of "Hermitian" in reference to time evolution, suggesting it may have been a typo or misunderstanding.
  • There is a discussion about the mathematical implications of non-Hermitian operators, with some noting that they do not yield real eigenvalues, which are necessary for measurement outcomes.
  • One participant inquires whether the absence of such an operator is due to observational limitations or mathematical impossibility, leading to a response that suggests both factors are relevant.
  • Another participant proposes a hypothetical scenario where one might create mathematical models that allow for the observation of superposition, emphasizing the creative aspect of modeling in quantum mechanics.

Areas of Agreement / Disagreement

Participants generally disagree on the implications and definitions surrounding Hermitian and non-Hermitian operators, particularly in the context of measurement and time evolution. The discussion remains unresolved regarding the feasibility of constructing operators that could yield the stated superposition result.

Contextual Notes

Participants express uncertainty about the definitions and roles of operators in quantum mechanics, particularly concerning the distinction between observables and time evolution. There are unresolved questions about the mathematical framework required to model superposition states.

Blue Scallop
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It is said that no Hermitian operator gives a time evolution where "I observed the spin to be both up and down" is a possible result. If you use non-Hermitian operator.. then it's possible.. and what operator is that where it is possible in principle where "I observed the spin to be both up and down"?
 
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Blue Scallop said:
no Hermitian operator gives a time evolution

Do you mean "Hamiltonian operator"? That's the operator that describes time evolution.

Blue Scallop said:
where "I observed the spin to be both up and down" is a possible result

Or do you mean Hermitian operator describing an observable with this property? Observables are not the same thing as time evolution.

Blue Scallop said:
If you use non-Hermitian operator

Then you are not talking about an observable, because a non-Hermitian operator has eigenvalues that are not real numbers, and any result of a measurement must be a real number.

Blue Scallop said:
what operator is that where it is possible in principle where "I observed the spin to be both up and down"?

There isn't one.
 
PeterDonis said:
Do you mean "Hamiltonian operator"? That's the operator that describes time evolution.
Or do you mean Hermitian operator describing an observable with this property? Observables are not the same thing as time evolution.

in thread https://www.physicsforums.com/threads/how-do-you-understand-mwi.908805/page-2 message #24, you yourself used the language "There is no Hermitian operator that gives a time evolution where "I observed the spin to be both up and down" is a possible result."" as in:

"Mathematically, the operation of a measuring device is modeled as a Hermitian operator that describes the device. Applying that operator to the initial state, before the measurement, is how you mathematically compute the state after the measurement; that's how you would derive the time evolution I gave in post #4. There is no Hermitian operator that gives a time evolution where "I observed the spin to be both up and down" is a possible result."

Is that a typo. Why didn't you use "There is no Hamiltonian operator that gives a time evolution where "I observed the spin to be both up and down" is a possible result." What did you use the word Hermitian to refer to time evolution which you just state now is related to observable and not time evolution?

Then you are not talking about an observable, because a non-Hermitian operator has eigenvalues that are not real numbers, and any result of a measurement must be a real number.
There isn't one.
 
Blue Scallop said:

This is better; you should always give a reference if you are referring to something specific like this.

In that post, I was using "time evolution" in a somewhat nonstandard sense, to indicate the operation of entangling the state of a measured system with the state of a measuring device as it is usually modeled. Strictly speaking, in order to model this mathematically, you would have to construct a Hamiltonian for the entire system (measured system plus measuring device) that included the interaction that produces the entanglement. But this is complicated and doesn't really add anything useful to the analysis, so often the whole process is described as I did in post #4 of the thread you linked to, by simply writing down the state of the measured system in the basis of eigenstates of a Hermitian operator (the one that describes the measurement you're making), and describing how each of those eigenstates gets entangled with an appropriate state of the measuring device by the measurement process. This simpler description isn't, strictly speaking, a "time evolution", because we haven't even tried to write down a Hamiltonian; but it describes the process of going from the state of measured system plus measuring device before the measurement, to the state of measured system plus measuring device after the measurement, which is a process that happens in time (though typically a very short amount of time).

None of this changes the final answer I gave in post #2.
 
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I inquired: "what operator is that where it is possible in principle where "I observed the spin to be both up and down"?"
You replied: "There isn't one."

Is the reason there isn't one is because no one has observed superposition or is it because it's not possible mathematically? Or is it possible mathematically? How?
 
Blue Scallop said:
Is the reason there isn't one is because no one has observed superposition or is it because it's not possible mathematically?

Both. We construct mathematical models in order to match what we observe.
 
PeterDonis said:
Both. We construct mathematical models in order to match what we observe.

Let's say there is a workshop at the Perimeter Institute or other physics schools about creating mathematical models just for creative exercise even if it doesn't match what we observe.. and one is tasked to create operators that can produce "I observed the spin to be both up and down".. how do you write such math or just describe how such math can be attempted.. this exercise can also make one get more understanding and familiariry with orthodox QM from looking it from all angles and sides ands point of view.
 
Blue Scallop said:
Let's say there is a workshop at the Perimeter Institute or other physics schools about creating mathematical models just for creative exercise even if it doesn't match what we observe.. and one is tasked to create operators that can produce "I observed the spin to be both up and down".. how do you write such math or just describe how such math can be attempted..

This is all well outside the PF rules. Thread closed.
 

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