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arXiv:0907.0085 · Physical Review E

Many-body reduced fidelity susceptibility in Lipkin-Meshkov-Glick model

Jian Ma, Xiaoguang Wang, Shi-Jian Gu

Published Aug 27, 2009• 18 citations
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Abstract

We study the reduced fidelity susceptibility ${\ensuremath{\chi}}_{r}$ for an $M$-body subsystem of an $N$-body Lipkin-Meshkov-Glick model with $\ensuremath{\tau}=M/N$ fixed. The reduced fidelity susceptibility can be viewed as the response of subsystem to a certain parameter. In noncritical region, the inner correlation of the system is weak, and ${\ensuremath{\chi}}_{r}$ behaves similar with the global fidelity susceptibility ${\ensuremath{\chi}}_{g}$, the ratio $\ensuremath{\eta}={\ensuremath{\chi}}_{r}/{\ensuremath{\chi}}_{g}$ depends on $\ensuremath{\tau}$ but not on $N$. However, at the critical point, the inner correlation tends to be divergent, and we find ${\ensuremath{\chi}}_{r}$ approaches ${\ensuremath{\chi}}_{g}$ with increasing the $N$. It is interesting to note that, $\ensuremath{\eta}=1$ in the thermodynamic limit, which means the susceptibilities of the local and global system are the same. Finally, we make numerical computations, and they are in perfect agreement with the analytical predictions.

DOI
10.1103/physreve.80.021124

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We study the reduced fidelity susceptibility \ensuremathχr{\ensuremath{\chi}}_{r}\ensuremathχr​ for an MMM-body subsystem of an NNN-body Lipkin-Meshkov-Glick model with \ensuremathτ=M/N\ensuremath{\tau}=M/N\ensuremathτ=M/N fixed. The reduced fidelity susceptibility can be viewed as the response of subsystem to a certain parameter. In noncritical region, the inner correlation of the system is weak, and \ensuremathχr{\ensuremath{\chi}}_{r}\ensuremathχr​ behaves similar with the global fidelity susceptibility \ensuremathχg{\ensuremath{\chi}}_{g}\ensuremathχg​, the ratio \ensuremathη=\ensuremathχr/\ensuremathχg\ensuremath{\eta}={\ensuremath{\chi}}_{r}/{\ensuremath{\chi}}_{g}\ensuremathη=\ensuremathχr​/\ensuremathχg​ depends on \ensuremathτ\ensuremath{\tau}\ensuremathτ but not on NNN. However, at the critical point, the inner correlation tends to be divergent, and we find \ensuremathχr{\ensuremath{\chi}}_{r}\ensuremathχr​ approaches \ensuremathχg{\ensuremath{\chi}}_{g}\ensuremathχg​ with increasing the NNN. It is interesting to note that, \ensuremathη=1\ensuremath{\eta}=1\ensuremathη=1 in the thermodynamic limit, which means the susceptibilities of the local and global system are the same. Finally, we make numerical computations, and they are in perfect agreement with the analytical predictions.
We derive a general formula for the reduced fidelity susceptibility when the reduced density matrix is 2x2 block diagonal. By using this result and a continuous unitary transformation, we study finite-size scaling of the reduced fidelity susceptibility in the Lipkin-Meshkov-Glick model. It is found that it can well characterize quantum phase transitions, that is, we can extract information about quantum phase transitions from only the fidelity of a subsystem, which is of practical use in experiments.
We study the critical properties of the Lipkin-Meshkov-Glick model in terms of the fidelity susceptibility. By using the Holstein-Primakoff transformation, we obtain explicitly the critical exponent of the fidelity susceptibility around the second-order quantum phase transition point. Our results provide a rare analytic case for the fidelity susceptibility in describing the universality class in quantum critical behavior. The different critical exponents in two phases are nontrivial results, indicating that the fidelity susceptibility is not always extensive.
In quantum phase transitions induced by continuous level crossing, global-state fidelity drops to zero at every level crossing point, making finite-size scaling not applicable to study the criticality. In this paper, we calculate the partial-state fidelity in two models, i.e., the Lipkin-Meshkov-Glick (LMG) model and one-dimensional Heisenberg model. We show that it can spot the second-order phase transition point in the thermodynamic limit, where continuous level crossing occurs. The finite-size scaling shows the partial-state fidelity susceptibility diverges as NNN for the isotropic LMG model and N3{N}^{3}N3 for the Heisenberg model.
In this paper, we study the scaling behavior of the ground-state logarithmic fidelity in the Lipkin–Meshkov–Glick (LMG) model. We find that the logarithmic fidelity shows a different scaling behavior in different phases of the model. It is an extensive quantity in the model's symmetry-broken phase while it behaves intensively in the polarized phase. Moreover, we also find that the logarithmic fidelity shows a singular behavior around the vicinity of the critical point and the critical exponent of the correlation length is also obtained numerically.
Berry phases and quantum fidelities for interacting spins have attracted considerable attention, in particular in relation to entanglement properties of spin systems and quantum phase transitions. These efforts mainly focus either on spin pairs or the thermodynamic infinite spin limit, while studies of the multipartite case of a finite number of spins are rare. Here, we analyze Berry phases and quantum fidelities of the energetic ground state of a Lipkin-Meshkov-Glick (LMG) model consisting of three spin-1/2 particles (qubits). We find explicit expressions for the Berry phase and fidelity susceptibility of the full system as well as the mixed state Berry phase and partial-state fidelity susceptibility of its one- and two-qubit subsystems. We demonstrate a realization of a nontrivial magnetic monopole structure associated with local, coordinated rotations of the three-qubit system around the external magnetic field.
Lipkin-Meshkov-Glick (LMG) models describe a set of NNN qubits which are located at the corners of an NNN-dimensional simplex and embedded in an external magnetic field. Because of its high coordinate number, quantum correlations in the models are quite nontrivial. For instance, in the large-NNN limit, two-site entanglement concurrence vanishes for any magnetic field. Multisite global entanglement and generalized global entanglement also tend to vanish in some quantum regions. We characterize the quantum correlations in the LMG model with multipartite nonlocality. In LMG models with anisotropy in the $x\ensuremath{-}y$ plane, for any fixed magnetic field, the ground-state nonlocality (denoted by S\mathcal{S}S) is found to scale as ${log}_{10}\mathcal{S}\ensuremath{\sim}aN+b$, with aaa and bbb the fitting parameters. For LMG models which are isotropic in the $x\ensuremath{-}y$ plane, nevertheless, the nonlocality for each Dicke state scales as ${log}_{10}\mathcal{S}\ensuremath{\sim}a\frac{1}{N}+b$, with b>0b>0b>0. Signals for the quantum phase transitions of the models will also be discussed. These results indicate that multipartite nonlocality captures some key ingredient of the ground-state quantum correlations in the models. In addition to the ground states, we also study multipartite nonlocality in the LMG models at finite temperatures. In the anisotropic models, the thermal stability of the nonlocality at low temperatures is determined by the energy gap. For the isotropic models, nevertheless, as the temperature increases, the nonlocality presents a sharp valley which is followed by a round peak. The behavior is far beyond the above-mentioned ``thermal stability vs energy gap'' picture. The underlying mechanics is the ``contribution inversion'' of low-lying energy states in the thermal-state nonlocality $\mathcal{S}({\stackrel{\ifmmode \hat{}\else \^{}\fi{}}{\ensuremath{\rho}}}_{T})$; that is, in a low-temperature region, the first-excited state ``defeats'' the ground state and plays a dominant role in thermal-state nonlocality.