Non-Hermitian operator for superposition

In summary: This is not a question.In summary, 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.
  • #1
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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  • #2
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.
 
  • #3
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.
 
  • #4
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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  • #5
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?
 
  • #6
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.
 
  • #7
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.
 
  • #8
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.
 

FAQ: Non-Hermitian operator for superposition

1. What is a Non-Hermitian operator for superposition?

A Non-Hermitian operator for superposition is a mathematical operator used in quantum mechanics to describe the superposition of quantum states. It is non-Hermitian because it does not satisfy the Hermitian symmetry property, meaning that its adjoint is not equal to itself. This allows for a wider range of possible quantum states and behaviors.

2. How is a Non-Hermitian operator different from a Hermitian operator?

A Hermitian operator is a mathematical operator that satisfies the Hermitian symmetry property, meaning that its adjoint is equal to itself. This property ensures that the operator has real eigenvalues and that its eigenvectors are orthogonal. In contrast, a Non-Hermitian operator does not satisfy this property and can have complex eigenvalues and non-orthogonal eigenvectors.

3. Can a Non-Hermitian operator be used in quantum mechanics?

Yes, Non-Hermitian operators are commonly used in quantum mechanics to describe complex quantum systems. They allow for a more complete description of quantum states and behaviors, and have been successfully applied in various areas of quantum physics.

4. What are some applications of Non-Hermitian operators in quantum mechanics?

Non-Hermitian operators have been used in various applications in quantum mechanics, including the study of quantum entanglement, quantum computation, and quantum information processing. They have also been applied in the study of open quantum systems, where energy is exchanged with the environment.

5. Are there any limitations to using Non-Hermitian operators in quantum mechanics?

While Non-Hermitian operators have proven to be useful in describing complex quantum systems, they also have some limitations. These operators do not always have well-defined eigenvalues and eigenvectors, which can make their interpretation and application challenging. Additionally, they can lead to non-unitary evolution of quantum states, which may not accurately reflect physical reality.

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