Undergrad Physical interpretation of a Hamiltonian with a constraint

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The discussion centers on the physical interpretation of the constraint Tr(Ĥ²) = 2ω² imposed on a Hamiltonian. The trace of the Hamiltonian relates to the sum of its eigenvalues, indicating that the energy eigenvalues must satisfy this condition. Without specific context, it is suggested that this could describe a two-state system where both states have the same energy ω. Various combinations of eigenvalues are proposed, illustrating how they can meet the trace condition. The consensus is that the trace is not a constraint but rather a characteristic of the Hamiltonian's eigenvalues.
Alex Cros
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Dear physics forums,

What is the physical interpretation of imposing the following constrain on a Hamiltonian:
Tr(\hat H^2)=2\omega ^2
where \omega is a given constant. I am not very familiar with why is the trace of the hamiltonian there.

Thanks in advance,
Alex
 
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The physical interpretation requires a physical context, and you didn't explain the physical context. At the very least, you should provide the reference in which this constraint is introduced.
 
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Without the context, I would guess that the Hamiltonian describes a two-state system (hence the factor 2) both of which have the same energy ##\omega##.
 
Demystifier said:
Without the context, I would guess that the Hamiltonian describes a two-state system (hence the factor 2) both of which have the same energy ##\omega##.

In case the OP didn't know this already---for any operator, the trace is equal to the sum of the eigenvalues. So if the trace of H^2 is 2\omega^2, then it means that the energy eigenvalues are such that E_1^2 + E_2^2 + ... = 2\omega^2. Demystifier's example is one of the simplest: E_1 = E_2 = \omega. Or it could be E_1 = \omega, E_2 = -\omega. Or it could be E_1 = \omega, E_2 = \omega/\sqrt{2}, E_3 = \omega/\sqrt{4}, E_4 = \omega/\sqrt{8} ...

The sum of the eigenvalues doesn't seem to me to be a "constraint" on the Hamiltonian, it's just a fact about it.
 
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I am slowly going through the book 'What Is a Quantum Field Theory?' by Michel Talagrand. I came across the following quote: One does not" prove” the basic principles of Quantum Mechanics. The ultimate test for a model is the agreement of its predictions with experiments. Although it may seem trite, it does fit in with my modelling view of QM. The more I think about it, the more I believe it could be saying something quite profound. For example, precisely what is the justification of...

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