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| <math>TT^\dagger = \sum_{m=1}^{N}\sum_{n=1}^{N}(|m+1\rangle\langle m|)(|n\rangle\langle n+1|) = \sum_{m=1}^{N}\sum_{n=1}^{N}delta_{m,n}|m+1\rangle\langle n+1|</math> | | <math>TT^\dagger = \sum_{m=1}^{N}\sum_{n=1}^{N}(|m+1\rangle\langle m|)(|n\rangle\langle n+1|) = \sum_{m=1}^{N}\sum_{n=1}^{N}\delta_{m,n}|m+1\rangle\langle n+1|</math> |
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| <math>TT^\dagger = \sum_{n=1}^{N}|n\rangle\langle n| = \left [ I \right ]_{NXN}</math> | | <math>TT^\dagger = \sum_{n=1}^{N}|n\rangle\langle n| = \left [ I \right ]_{NXN}</math> |
Symmetries(Problem taken from a quantum assignment in the Department of Physics, UF)
Problem
Consider an
state system with the states labeled as
. Let the hamiltonian for this system be
Notice that the Hamiltonian, in this form, is manifestly hermitian. Use periodic boundary condition, i.e,
. You can think of these states as being placed around a circle.
(a) Define the translation operator,
as taking
.Write T in
a form like
in the first equation and show that
is both unitary and commutes with
. It is thus a symmetry of the hamiltonian.
(b) Find the eigenstates of T by using wavefunctions of the form
What are the eigenvalues of these eigenstates? Do all these eigenstates have to be eigenstates of
as well? If not, do any of these eigenstates have to be eigenstates of
? Explain your answer.
(c) Next Consider
which takes
Write F in a form like
in the first equation and show that
both is unitary and commutes with
. It is thus a symmetry of the hamiltonian.
(d) Find a complete set of eigenstates of
and their eigenvalues. Do all these eigenstates have to be eigenstates of
as well? If not, do any of these eigenstates have to be eigenstates of
? Explain your answer.
Solution
So
with
So
So
is unitary.
as