The quantum clock model is a quantum lattice model. It is a generalisation of the transverse-field Ising model . It is defined on a lattice with N {\displaystyle N} states on each site. The Hamiltonian of this model is
H = − J ( ∑ ⟨ i , j ⟩ ( Z i † Z j + Z i Z j † ) + g ∑ j ( X j + X j † ) ) {\displaystyle H=-J\left(\sum _{\langle i,j\rangle }(Z_{i}^{\dagger }Z_{j}+Z_{i}Z_{j}^{\dagger })+g\sum _{j}(X_{j}+X_{j}^{\dagger })\right)}
Here, the subscripts refer to lattice sites, and the sum ∑ ⟨ i , j ⟩ {\displaystyle \sum _{\langle i,j\rangle }} is done over pairs of nearest neighbour sites i {\displaystyle i} and j {\displaystyle j} . The clock matrices X j {\displaystyle X_{j}} and Z j {\displaystyle Z_{j}} are N × N {\displaystyle N\times N} generalisations of the Pauli matrices satisfying
Z j X k = e 2 π i N δ j , k X k Z j {\displaystyle Z_{j}X_{k}=e^{{\frac {2\pi i}{N}}\delta _{j,k}}X_{k}Z_{j}} and X j N = Z j N = 1 {\displaystyle X_{j}^{N}=Z_{j}^{N}=1}
where δ j , k {\displaystyle \delta _{j,k}} is 1 if j {\displaystyle j} and k {\displaystyle k} are the same site and zero otherwise. J {\displaystyle J} is a prefactor with dimensions of energy, and g {\displaystyle g} is another coupling coefficient that determines the relative strength of the external field compared to the nearest neighbor interaction. The model obeys a global Z N {\displaystyle \mathbb {Z} _{N}} symmetry, which is generated by the unitary operator U X = ∏ j X j {\displaystyle U_{X}=\prod _{j}X_{j}} where the product is over every site of the lattice. In other words, U X {\displaystyle U_{X}} commutes with the Hamiltonian. When N = 2 {\displaystyle N=2} the quantum clock model is identical to the transverse-field Ising model. When N = 3 {\displaystyle N=3} the quantum clock model is equivalent to the quantum three-state Potts model. When N = 4 {\displaystyle N=4} , the model is again equivalent to the Ising model. When N > 4 {\displaystyle N>4} , strong evidences have been found that the phase transitions exhibited in these models should be certain generalizations of Kosterlitz–Thouless transition, whose physical nature is still largely unknown.
One-dimensional model There are various analytical methods that can be used to study the quantum clock model specifically in one dimension.
Kramers–Wannier duality A nonlocal mapping of clock matrices known as the Kramers–Wannier duality transformation can be done as follows:
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