- #1
chaksome
- 17
- 6
I am reading a paper about quantum many-body scar based on the spin-1 XY model. I noticed that he write down the Hamiltonian as follows
$$
H=J \sum_{\langle i j\rangle}\left(S_{i}^{x} S_{j}^{x}+S_{i}^{y} S_{j}^{y}\right)+h \sum_{i} S_{i}^{z}+D \sum_{i}\left(S_{i}^{z}\right)^{2}
$$
which is a little bit different from what I've learned as
$$
H=J \sum_{\langle i j\rangle}\left(\left(1+\gamma_i\right)S_{i}^{x} S_{j}^{x}+\left(1-\gamma_i\right)S_{i}^{y} S_{j}^{y}\right)+h \sum_{i} S_{i}^{z}
$$
I think the ##\gamma## is a parameter characterizing the degree of anisotropy in the XY plane, so ##\gamma = 0## when we assume that the energy gap of the system is always closed. Besides, ##h## is a parameter characterizing the degree of the external field.
How about D, what does it represent? Why should we consider the term of the square of ##S^z_i##(identity matrix)? Please help me out~Thanks a lot!
$$
H=J \sum_{\langle i j\rangle}\left(S_{i}^{x} S_{j}^{x}+S_{i}^{y} S_{j}^{y}\right)+h \sum_{i} S_{i}^{z}+D \sum_{i}\left(S_{i}^{z}\right)^{2}
$$
which is a little bit different from what I've learned as
$$
H=J \sum_{\langle i j\rangle}\left(\left(1+\gamma_i\right)S_{i}^{x} S_{j}^{x}+\left(1-\gamma_i\right)S_{i}^{y} S_{j}^{y}\right)+h \sum_{i} S_{i}^{z}
$$
I think the ##\gamma## is a parameter characterizing the degree of anisotropy in the XY plane, so ##\gamma = 0## when we assume that the energy gap of the system is always closed. Besides, ##h## is a parameter characterizing the degree of the external field.
How about D, what does it represent? Why should we consider the term of the square of ##S^z_i##(identity matrix)? Please help me out~Thanks a lot!
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