Commutator of the density operator

Click For Summary
SUMMARY

The discussion centers on the commutation properties of the density operator with other operators, specifically unitaries and observables. It is established that the density operator does not generally commute with unitary operators or observables. The participants clarify that while the trace operation allows for certain reordering of matrices, this does not imply that the density operator commutes with those matrices. Furthermore, it is emphasized that states (vectors) and observables (matrices) cannot be commuted, and the properties of Hermitian operators are discussed in relation to expectation values.

PREREQUISITES
  • Understanding of density operators in quantum mechanics
  • Familiarity with unitary and Hermitian operators
  • Knowledge of trace operations and their properties
  • Basic concepts of quantum states and observables
NEXT STEPS
  • Study the properties of density operators in quantum mechanics
  • Learn about the implications of Hermitian operators in quantum mechanics
  • Explore the mathematical framework of trace operations in linear algebra
  • Investigate the relationship between states and observables in quantum theory
USEFUL FOR

Quantum physicists, students of quantum mechanics, and researchers interested in the mathematical foundations of quantum theory will benefit from this discussion.

keen23
Messages
9
Reaction score
0
Hello all!
I hope some of you are more proficient in juggling with bra-kets...
I am wondering if/when the density operator commutes with other operators, especially with unitaries and observables.

1. My guess is, that it commutes with unitaries, but I am not sure if my thinking is correct. It's like this:

\langle x|\rho U^{\dagger}|x\rangle=\langle x|U^{\dagger}\rho U U^{\dagger}|x\rangle=\langle x|U^{\dagger} \rho|x\rangle<br />

Is that ok?

2.How do I determine, if a state commutes with its observable? I don't see a physical meaning in this, I'm not sure what to do...

Thanks
 
Physics news on Phys.org
1. No, you've basically argued that any unitary matrix commutes with any other matrix, which is not true. The problem is that you insert U and U^\dagger in a weird way, you are assuming that \rho = U^\dagger\rho U which is not true. If you want to insert an identity operator by inserting U and its adjoint, you can't split them up around another matrix, unless you assume that U and that other matrix commute.

Now there are rules for computing the trace where this will work, because Tr AB = Tr BA regardless of whether A and B commute. So if you're tracing over the product of the density matrix and some other matrix, then something like this can work (be careful about reordering a product of more than two matrices, however). Expressions involving the trace over the density matrix times an operator are quite common, so you may see reordering like this. But this does not mean that the density matrix commutes with that operator.

2. States don't commute with observables. States are vectors, observables are matrices, and you just can't commute them. You can take the Hermitian conjugate, which usually will leave an operator unchanged and might end up looking like you've commuted the state with the operator, but it's not the same operation.
 
Thank you for your reply!
Did I get it right, it's in general not possible to swap an operater and \rho?

Indeed I want to take the trace, thanks for the hint of swapping "before" :)

I will see later if this works for me (I am afraid, it won't, since U=U_A U_B. I was hoping to get rid of U_B first by letting it act on the ket on the right side... So that won't work...)

Thanks :)
 
It's not hard to show that \langle\alpha|XY|\beta\rangle=\langle\beta|Y^\dagger X^\dagger|\alpha\rangle^*. So if |\alpha\rangle=|\beta\rangle and both operators are hermitian, you can swap them, since the product of two hermitian operators is hermitian, and hermitian operators have real expectation values. In other words, if your U is hermitian instead of unitary, it "commutes" with \rho inside an expectation value, but not in general.
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

Similar threads

Replies
2
Views
1K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 8 ·
Replies
8
Views
2K
Replies
0
Views
792
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 4 ·
Replies
4
Views
1K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 3 ·
Replies
3
Views
1K
  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 6 ·
Replies
6
Views
2K