Graduate Quantum Ising model correlation function query

Click For Summary
The discussion centers on the quantum Ising model and its correlation function, specifically examining the implications of the Hamiltonian and time evolution operator on the operators involved. The query highlights a statement regarding the well-defined value of the operator ##\hat{\sigma}^{z}_{j}## when the operator ##\hat{\sigma}^{a=\pm}_{j}## appears in the correlation function ##\mathcal{G}##. It is suggested that after the first occurrence of ##\hat{\sigma}^{a=\pm}_{j}##, the state becomes an eigenstate of ##\hat{\sigma}_{j}^{z}##, allowing it to commute with the Hamiltonian. However, the poster seeks clarification on how this well-defined nature holds true before the time ##t_1##. The discussion emphasizes the nuances of operator behavior in quantum dynamics.
Danny Boy
Messages
48
Reaction score
3
In this paper, on quantum Ising model dynamics, they consider the Hamiltonian
$$\mathcal{H} = \sum_{j < k} J_{jk} \hat{\sigma}_{j}^{z}\hat{\sigma}_{k}^{z}$$
and the correlation function
$$\mathcal{G} = \langle \mathcal{T}_C(\hat{\sigma}^{a_n}_{j_n}(t_n^*)\cdot\cdot\cdot \hat{\sigma}^{a_1}_{j_1}(t_1^*)\hat{\sigma}^{b_m}_{k_m}(t_m) \cdot\cdot\cdot \hat{\sigma}^{b_1}_{k_1}(t_1)) \rangle$$
where ##a,b= \pm## and the time dependence of the Heisenberg picture
$$\hat{\sigma}_{j}^{a}(t) = e^{it\mathcal{H}}\hat{\sigma}_{j}^{a}e^{-it\mathcal{H}}$$
where the time ordering operator ##\mathcal{T_C}## orders operators along a closed path ##\mathcal{C}##.

Question: Can anyone see the reasoning behind the following statement on page 6:
If an operator ##\hat{\sigma}^{a=\pm}_{j}## occurs in ##\mathcal{G}## one or more times, the operator ##\hat{\sigma}^{z}_{j}## (appearing in the time evolution operator) is forced to take on a well defined value ##\sigma_{j}^{z}(t)## at all points in time.

Thanks for any assistance.
 
Physics news on Phys.org
I think the idea is after ##t_1## (denoting the first occurrence of the operator ##\hat{\sigma}^{a=\pm}_{j}##) since this results in the state on site ##j## being an eigenstate of ##\hat{\sigma}_{j}^{z}##, hence it commutes with the Ising Hamiltonian above. It is still not clear how it it well defined before time ##t_1##?
 
Last edited:
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 1 ·
Replies
1
Views
1K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 16 ·
Replies
16
Views
3K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 87 ·
3
Replies
87
Views
8K
Replies
7
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K