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arXiv 1306.6128nlin.CDmath-phmath.MPquant-ph
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Kicked-Harper模型与共振双Kicked转子模型:从谱差异到拓扑等价

Kicked-Harper model vs On-Resonance Double Kicked Rotor Model: From Spectral Difference to Topological Equivalence

Hailong Wang, Derek Y. H. Ho, Wayne Lawton, Jiao Wang, Jiangbin Gong

摘要:

最近的研究已经确定,除了众所周知的踢哈珀模型(KHM),共振双踢转子模型(ORDKR)也有霍夫施塔特的蝴蝶Floquet频谱,与标准的霍夫施塔特的频谱,这是一个范例,在整数量子霍尔效应的研究非常相似。前面已经指出,这两个动力学模型的准能谱(i)如果有效的普朗克常量取2*pi的无理倍数,则可以精确地相互重叠;(ii)如果相同的参数取2*pi的有理倍数,则会不同。本文对这两个模型进行了详细的比较,其中有效的普朗克常量为2*pi M/N,其中M和N是互质的奇整数。研究发现,在两个周期性踢踹序列具有相同踢踹强度的情况下,该谱具有一个平坦带和$N-1$非平坦带,其最大宽度随K的N+2次方幂律衰减,其中K为踢踹强度参数。一个平坦的频带的存在被严格证明和幂律缩放,数值检查的情况下,也被证明为三波段的情况下分析。相比之下,KHM没有任何平坦带,其带宽与K成线性比例。这表明,导致在动态行为,如瞬态(但非常长)的动态本地化的ORDKR,这是不存在的KHM的显着差异。最后,我们表明,尽管有这些差异,存在简单的扩展KHM和ordKR(在引入一个额外的周期相位参数),使得由此产生的扩展KHM和ordKR实际上是拓扑等价的,即,它们产生完全相同的Floquet-band Chern数,并在相同的反冲强度下显示拓扑相变。这种拓扑等价的理论推导。

英文摘要:

Recent studies have established that, in addition to the well-known kicked Harper model (KHM), an on-resonance double kicked rotor model (ORDKR) also has Hofstadter's butterfly Floquet spectrum, with strong resemblance to the standard Hofstadter's spectrum that is a paradigm in studies of the integer quantum Hall effect. Earlier it was shown that the quasi-energy spectra of these two dynamical models (i) can exactly overlap with each other if an effective Planck constant takes irrational multiples of 2*pi and (ii) will be different if the same parameter takes rational multiples of 2*pi. This work makes some detailed comparisons between these two models, with an effective Planck constant given by 2*pi M/N, where M and N are coprime and odd integers. It is found that the ORDKR spectrum (with two periodic kicking sequences having the same kick strength) has one flat band and $N-1$ non-flat bands whose largest width decays in power law as K to the power of N+2, where K is a kicking strength parameter. The existence of a flat band is strictly proven and the power law scaling, numerically checked for a number of cases, is also analytically proven for a three-band case. By contrast, the KHM does not have any flat band and its band width scales linearly with K. This is shown to result in dramatic differences in dynamical behavior, such as transient (but extremely long) dynamical localization in ORDKR, which is absent in KHM. Finally, we show that despite these differences, there exist simple extensions of KHM and ORDKR (upon introducing an additional periodic phase parameter) such that the resulting extended KHM and ORDKR are actually topologically equivalent, i.e., they yield exactly the same Floquet-band Chern numbers and display topological phase transitions at the same kick strengths. A theoretical derivation of this topological equivalence is provided.

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