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Quantum criticality in photorefractive optics: vortices in laser beams and antiferromagnets

机译:光折变光学中的量子临界性:激光束中的涡旋   和反铁磁体

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摘要

We study vortex patterns in a prototype nonlinear optical system:counterpropagating laser beams in a photorefractive crystal, with or withoutthe background photonic lattice. The vortices are effectively planar anddescribed by the winding number and the "flavor" index, stemming from the factthat we have two parallel beams propagating in opposite directions. The problemis amenable to the methods of statistical field theory and generalizes theBerezinsky-Kosterlitz-Thouless transition of the XY model to the "two-flavor"case. In addition to the familiar conductor and insulator phases, we also havethe perfect conductor (vortex proliferation in both beams/"flavors") and thefrustrated insulator (energy costs of vortex proliferation and vortexannihilation balance each other). In the presence of disorder in the backgroundlattice, a novel phase appears which shows long-range correlations and absenceof long-range order, thus being analogous to spin glasses. An important benefitof this approach is that qualitative behavior of patterns can be known withoutintensive numerical work over large areas of the parameter space. Moregenerally, we would like to draw attention to connections between the(classical) pattern-forming systems in photorefractive optics and the methodsof (quantum) condensed matter and field theory: on one hand, we use thefield-theoretical methods (renormalization group, replica formalism) to analyzethe patterns; on the other hand, the observed phases are analogous to thoseseen in magnetic systems, and make photorefractive optics a fruitful testingground for condensed matter systems. As an example, we map our system to adoped $O(3)$ antiferromagnet with $\mathbb{Z}_2$ defects, which has the samestructure of the phase diagram.
机译:我们研究了原型非线性光学系统中的涡旋图案:在具有或不具有背景光子晶格的光折射晶体中反向传播激光束。涡流实际上是平面的,并且由绕线数和“风味”指数来描述,这是由于我们有两个在相反方向传播的平行光束。该问题适合于统计场论的方法,并且将XY模型的Berezinsky-Kosterlitz-Thouless过渡推广到“两味”情况。除了熟悉的导体和绝缘体相,我们还拥有理想的导体(两束/“风味”中的涡旋扩散)和受挫的绝缘体(涡旋扩散和涡旋an灭的能量成本相互平衡)。在背景晶格中存在紊乱的情况下,出现了一个新的相,该相显示出远距离的相关性而没有远距离的有序性,因此类似于自旋玻璃。这种方法的一个重要好处是,无需在参数空间的大面积上进行大量的数值工作,就可以知道模式的定性行为。通常,我们希望引起人们注意光折光光学系统中的(经典)图案形成系统与(量子)凝聚态和场论方法之间的联系:一方面,我们使用场论方法(重归一化组,复制品形式主义) )分析模式;另一方面,观察到的相类似于磁性系统中观察到的相,并使光折光光学器件成为凝聚态系统的卓有成效的试验场。例如,我们将我们的系统映射到具有$ \ mathbb {Z} _2 $缺陷的,反光的$ O(3)$反铁磁体,其相位图的结构相同。

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