How to Prove the Unitarity of Matrix U_{pq}?

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SUMMARY

The discussion centers on proving the unitarity of the matrix U_{pq} in the context of fermionic annihilation operators. The Hamiltonian given is H = ∑_{k}(ε_k - μ)c_k^{†}c_k + γ∑_{kp}c_k^{†}c_p, with the relation c_p = ∑_{q} U_{pq} b_q. The key conclusion is that U being unitary is equivalent to the anticommutation relations {b_q, b_p} = 0 and {b_q, b_p^{†}} = δ_{pq} being satisfied. The participants emphasize the need for additional information about the operators b to derive an explicit equation for U.

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Threepwood
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Homework Statement


I have been given the Hamiltonian
H = \sum_{k}\left(\epsilon_k - \mu\right) c_k^{\dag} c_k + \gamma \sum_{kp}c_k^{\dag} c_p
and also that
c_p = \sum_{q} U_{pq} b_q
I have to prove that this matrix U_{pq} is unitary, and find an equation for U_{pq}.

Homework Equations


This is equivalent to proving that
\{b_q, b_p\} = 0
and
\{b_q , b_p^{\dag}\} = \delta_{pq}
where b and c are creation and annihiliation operators.

The Attempt at a Solution


Knowing that
c_p = \sum_{q} U_{pq} b_q
then
c_q = \sum_{p} U_{pq} b_p
and
\{b_q , b_p\} = b_q b_p + b_p b_q
c_p b_p = \left(\sum_{q} U_{pq} b_q\right) b_p
b_q c_q = b_q \left(\sum_{p} U_{pq} b_p\right)
So that
c_p b_p + b_q c_q = \left(\sum_{q} U_{pq} b_q\right) b_p + b_q \left(\sum_{p} U_{pq} b_p\right)

Hmm, now what?
 
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You should use that the c operators satisfy the same anticommutation relations that the b's also satisfy. On the other hand, c_p and b_q do not, in general, satisfy such relations.
 
Isn't that precisely what I'm supposed to be proving?
 
No, you have to prove U is unitary.

Edit: you already seem to know that U being unitary is equivalent to the b's satisfying the same anticommutation relations as the c's. But that's all there is to it...
 
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I need to prove those relations. How do I prove that
\{b_q , b_p\} = 0 and \{b_q , b_p^{\dag} \} = \delta_{pq}?

And also, beyond that, how do I find an equation for U? I don't need to solve the equation for U, just find it.
 
You need more information to prove any of those relations. You must have been given some info about what the b's are supposed to be, for instance. I assumed that you had been told that the b's are fermionic annihilation operators.
 
Yes, they are. At the moment I'm more interested in finding this equation for U, but I have no idea where to even start. I've just been playing around with the relations, like taking
c_p c_q^{\dag} + c_q^{\dag} c_p = \delta_{pq}
applying c_q to the left
c_q c_p c_q^{\dag} + c_q c_q^{\dag} c_p = c_q \delta_{pq}
because c_p c_q = - c_q c_p, then
-c_p c_q c_q^{\dag} + c_q c_q^{\dag} c_p = c_q \delta_{pq}
and c_q c_q^{\dag} = 0, so
c_q \delta_{pq} = 0
Hmm! Is this useful relation? Probably not..
 
If the b's are fermionic annihilation operators, then that *means* they satisfy the anticommutation relations that, as you figured out, are equivalent to U being unitary. Done.
 
Ok, but what about finding an equation for U?
 
  • #10
You clearly did not state the full problem so I have to keep guessing: were you supposed to diagonalize the Hamiltonian and find U such that H=\sum_k E(k) b^+_kb_k [/itex]?
 
  • #11
That was never stated in the question, but maybe it was implied somehow. It would make sense. How would I go about doing that?
 

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