Divakaran Uma, Sharma Shraddha, Dutta Amit
UM-DAE Center for Excellence in Basic Sciences, Mumbai 400 098, India.
Department of Physics, Indian Institute of Technology, Kanpur 208 016, India.
Phys Rev E. 2016 May;93(5):052133. doi: 10.1103/PhysRevE.93.052133. Epub 2016 May 18.
We study an integrable spin chain with three spin interactions and the staggered field (λ) while the latter is quenched either slowly [in a linear fashion in time (t) as t/τ, where t goes from a large negative value to a large positive value and τ is the inverse rate of quenching] or suddenly. In the process, the system crosses quantum critical points and gapless phases. We address the question whether there exist nonanalyticities [known as dynamical phase transitions (DPTs)] in the subsequent real-time evolution of the state (reached following the quench) governed by the final time-independent Hamiltonian. In the case of sufficiently slow quenching (when τ exceeds a critical value τ_{1}), we show that DPTs, of the form similar to those occurring for quenching across an isolated critical point, can occur even when the system is slowly driven across more than one critical point and gapless phases. More interestingly, in the anisotropic situation we show that DPTs can completely disappear for some values of the anisotropy term (γ) and τ, thereby establishing the existence of boundaries in the (γ-τ) plane between the DPT and no-DPT regions in both isotropic and anisotropic cases. Our study therefore leads to a unique situation when DPTs may not occur even when an integrable model is slowly ramped across a QCP. On the other hand, considering sudden quenches from an initial value λ_{i} to a final value λ_{f}, we show that the condition for the presence of DPTs is governed by relations involving λ_{i},λ_{f}, and γ, and the spin chain must be swept across λ=0 for DPTs to occur.
我们研究了一个具有三种自旋相互作用和交错场(λ)的可积自旋链,其中交错场被缓慢淬灭[以时间(t)的线性方式,即t/τ,t从一个大的负值变化到一个大的正值,τ是淬灭速率的倒数]或突然淬灭。在此过程中,系统会穿过量子临界点和无隙相。我们探讨了在由最终与时间无关的哈密顿量所支配的状态(淬灭后达到)的后续实时演化中是否存在非解析性[称为动力学相变(DPT)]这一问题。在足够缓慢淬灭的情况下(当τ超过临界值τ₁时),我们表明,即使系统被缓慢驱动穿过多个临界点和无隙相,仍会出现与在孤立临界点处淬灭时类似形式的DPT。更有趣的是,在各向异性情况下,我们表明对于某些各向异性项(γ)和τ的值,DPT会完全消失,从而在各向同性和各向异性情况下的(γ - τ)平面中确定了DPT区域和无DPT区域之间的边界。因此,我们的研究导致了一种独特的情况,即即使一个可积模型被缓慢驱动穿过一个量子临界点,DPT也可能不会出现。另一方面,考虑从初始值λᵢ到最终值λբ的突然淬灭,我们表明DPT存在的条件由涉及λᵢ、λբ和γ的关系所支配,并且自旋链必须扫过λ = 0才能发生DPT。