Query about an article on quantum synchronization

Click For Summary
SUMMARY

The discussion focuses on quantum synchronization as outlined in a specific paper. It highlights the implications of the ##U(1)## symmetry, which leads to the conclusion that the expectation values of the raising and lowering operators, ##\langle \hat{\sigma}^{\pm}_{(A,B)j} \rangle##, are zero. Consequently, all nonzero observables can be expressed solely in terms of the operators ##\langle \hat{\sigma}^{z}_{(A,B)j} \rangle##, ##\langle \hat{\sigma}^{+}_{(A,B)i}\hat{\sigma}^{-}_{(A,B)j} \rangle##, and ##\langle \hat{\sigma}^{z}_{(A,B)i}\hat{\sigma}^{z}_{(A,B)j} \rangle##, as these do not involve raising or lowering operators.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly quantum synchronization.
  • Familiarity with operator notation in quantum mechanics, including raising and lowering operators.
  • Knowledge of symmetry principles in quantum systems, specifically ##U(1)## symmetry.
  • Basic comprehension of expectation values in quantum mechanics.
NEXT STEPS
  • Study the implications of ##U(1)## symmetry in quantum mechanics.
  • Explore the role of expectation values in quantum observables.
  • Review the mathematical framework of quantum operators, focusing on raising and lowering operators.
  • Investigate applications of quantum synchronization in quantum information theory.
USEFUL FOR

Researchers, physicists, and students in quantum mechanics, particularly those interested in quantum synchronization and the mathematical foundations of quantum theory.

Danny Boy
Messages
48
Reaction score
3
TL;DR
Query in attached paper on quantum synchronization.
I am currently studying this paper on quantum synchronization. The first page gives an introduction to synchronization and the basic setup of the ensembles in the cavity. My query is on the second page where the following statements are made.

Because of the ##U(1)## symmetry, ##\langle \hat{\sigma}^{\pm}_{(A,B)j} \rangle = 0##. Therefore, all nonzero observables can be expressed in terms of ##\langle \hat{\sigma}^{z}_{(A,B)j} \rangle, \langle \hat{\sigma}^{+}_{(A,B)i}\hat{\sigma}^{-}_{(A,B)j} \rangle## and ##\langle \hat{\sigma}^{z}_{(A,B)i}\hat{\sigma}^{z}_{(A,B)j} \rangle.##

Can anyone see why the implication is that all observables can be expressed by these terms?

Thanks for any assistance.
 

Attachments

Last edited by a moderator:
Physics news on Phys.org
The statement is referring to the fact that, due to the ##U(1)## symmetry, the expectation values of the raising and lowering operators are zero. This means that any observables that can be expressed in terms of these operators will also have zero expectation values. As such, the only nonzero observables are those that can be expressed in terms of the ##\langle \hat{\sigma}^{z}_{(A,B)j} \rangle, \langle \hat{\sigma}^{+}_{(A,B)i}\hat{\sigma}^{-}_{(A,B)j} \rangle## and ##\langle \hat{\sigma}^{z}_{(A,B)i}\hat{\sigma}^{z}_{(A,B)j} \rangle## operators, as these are the only ones which do not contain raising or lowering operators.
 

Similar threads

  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 15 ·
Replies
15
Views
3K
  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 1 ·
Replies
1
Views
2K
Replies
4
Views
2K
  • · Replies 11 ·
Replies
11
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 16 ·
Replies
16
Views
4K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K