Criticality of the magnon-bound-state hierarchy for the quantum Ising chain with the long-range interactions
arXiv:1811.06241 · doi:10.1140/epjb/e2018-90426-8
Abstract
The quantum Ising chain with the interaction decaying as a power law of the distance between spins was investigated numerically. A particular attention was paid to the low-energy spectrum, namely, the single-magnon and two-magnon-bound-state masses, , respectively, in the ordered phase. It is anticipated that for each , the scaled bound-state mass should take a universal constant (critical amplitude ratio) in the vicinity of the critical point. In this paper, we calculated the amplitude ratio with the exact diagonalization method, which yields the spectral information such as directly. As a result, we found that the scaled mass exhibits a non-monotonic dependence on ; that is, the bound state is stabilized by an intermediate value of . Such a feature is accordant with a recent observation based on the non-perturbative-renormalization-group method.
References in corpus (13)
- Observation of a Many-Body Dynamical Phase Transition with a 53-Qubit Quantum Simulator
- Observation of mesoscopic crystalline structures in a two-dimensional Rydberg gas
- Entanglement entropy for the long range Ising chain
- New frontiers with quantum gases of polar molecules
- Anomalous dynamical phase in quantum spin chains with long-range interactions
- Criticality and Phase Diagram of Quantum Long-Range models
- Multi-speed prethermalization in spin models with power-law decaying interactions
- Critical phenomena and quantum phase transition in long range Heisenberg antiferromagnetic chains
- The crossover region between long-range and short-range interactions for the critical exponents
- Fidelity Susceptibility Study of Quantum Long-Range Antiferromagnetic Ising Chain
- Anisotropic Long-Range Spin Systems
- Universal critical behavior of the two-magnon-bound-state mass gap for the (2+1)-dimensional Ising model
- Renormalization group for the -theory with long-range interaction and the critical exponent of the Ising model