Can Periodic Hamiltonian and Translation Operators Share Eigenstates?

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In summary, if a periodic Hamiltonian operator commutes with the translation operator, then it is possible to find simultaneous eigenstates for these two operators. These eigenstates are expressed as |θ>=Σeinθ|n> (n ranging from -[oo] to +[oo]) and have an eigenvalue of e-iθ for the translation operator. This result is based on Sakurai's Modern Quantum Mechanics, specifically pp. 261-263.
  • #1
eNtRopY
Prove that if a periodic Hamiltonian operator commutes with the translation operator then these two operators can have simultaneous eigenstates.


{{ H(x) = H(x+a) }
& { T(a)f(x) = f(x+a) }
& { [T(a),H(x)] = 0 }
}
--> {{[uni][psi] [subset] complex functions, there exists [psi] [subset] complex functions
such that { H(x)[psi](x) = E[psi](x) }
& { T(a)[psi](x) = c(a)[psi](x) }
}

Thanks dudes.

eNtRopY
 
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  • #2
is the periodic hamiltonian a harmonic oscillator function?
 
  • #3
No it's independent of time. I mean that it is periodic in space... like a Bloch function.

V(x+a) = V(x)

Actually, I believe I figured out the answer, but if you guys want to post your answer that's cool too.

eNtRopY
 
  • #4
Originally posted by eNtRopY
Prove that if a periodic Hamiltonian operator commutes with the translation operator then these two operators can have simultaneous eigenstates.

Are you sure that's the problem? I ask because any two operators that commute can have simultaneous eigenstates; the "periodic" condition has nothing to do with it.

Methinks you are supposed to be finding an explicit expression for what exactly those eigenstates are.


In this case, |θ>=Σeinθ|n> (n goes from -[oo] to +[oo]) is an eigenstate of τ(a) with eigenvalue e-iθ.

This is from Sakurai, Modern Quantum Mechanics pp. 261-263.
 

1. What is a Commutation Relation?

A commutation relation is a mathematical rule that describes how two or more operators, which are mathematical functions, interact with each other. It determines the order in which the operators are applied and how their results are combined.

2. Why are Commutation Relations important in physics?

Commutation relations are important in physics because they help us understand the fundamental principles and relationships between physical quantities. They are used to describe the behavior of particles and systems, and are essential in solving complex physical problems.

3. How are Commutation Relations used in quantum mechanics?

In quantum mechanics, commutation relations are used to describe the uncertainty principle, which states that it is impossible to know the exact values of certain physical quantities simultaneously. These relations also play a key role in determining the allowed energy levels and dynamics of quantum systems.

4. Can Commutation Relations change over time?

Yes, commutation relations can change over time depending on the physical system being studied. In quantum mechanics, for example, the commutation relations may differ for different energy states of a particle, thus changing as the particle's energy changes.

5. Are Commutation Relations always commutative?

No, commutation relations are not always commutative. In some cases, the order in which operators are applied can affect the final result, making the relations non-commutative. However, in other cases, commutation relations may be commutative, meaning the order of operators does not affect the final result.

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