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Artificial gauge field switching using orbital angular momentum modes in optical waveguides

机译:使用轨道角动量模式在光波导中的人工测量仪场切换

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摘要

a Schematic representation of the structure composed of identical cylindrical waveguides arranged in a diamond chain configuration. Each unit cell j hosts three waveguides sj≡Aj,Bj,Cj forming a triangle with central angle θ. The distances between waveguide centres are dAj−Bj=dAj−Cj≡d, dBj−Cj=2dsin(θ/2) and dAj−Aj+1=2dcos(θ/2). The blue arrows indicate the couplings. b Refractive index profile of the waveguides, defined by ncore = 1.548, nclad = 1.540 and waveguide radius R = 1.9 μm. Field intensity of the ℓ=0 (green) and ℓ=1 (red) modes, where βℓ is the propagation constant of mode ℓ, k0 = 2π/λ0 is the vacuum wavenumber and λ0 is the light wavelength in vacuum. c Numerically calculated coupling strengths for separation distances d = 5 μm, 5.5 μm, 6 μm, 6.5 μm, 7 μm and 7.5 μm using λ0 = 700 nm. In particular, c0 (crosses) accounts for the coupling between the ℓ=0 modes, and c1 (circles) and c2 (squares) account for the coupling between the ℓ=1 modes with the same or opposite circulation directions, respectively. The dashed and solid lines correspond to the exponential fittings of c0d≈K0exp(−κ0d), c1(d)≈K1exp(−κ1d) and c2(d)≈K2exp(−κ2d), where K0 = 387 mm−1, κ0 = 1.17 μm−1, K1 = 19.39 mm−1, κ1 = 0.52 μm−1, K2 = 56.25 mm−1 and κ2 = 0.59 μm−1. The inset in c shows c2/c1 with respect to the separation distance d
机译:相同的圆柱形波导构成的结构的示意性表示设置在金刚石链构型。每个单位小区j主机3个波导sj≡Aj,BJ,CJ形成具有中心角θ的三角形。波导中心之间的距离是DAJ-BJ = DAJ-Cj≡d,DBJ-CJ = 2dsin(θ/ 2)和DAJ-AJ + 1 = 2dcos(θ/ 2)。蓝色箭头指示的耦合。 b中的波导的折射率分布,由n芯= 1.548,nclad = 1.540和波导半径R = 1.9微米限定。的ℓ= 0(绿色)场强度和ℓ= 1(红色)模式,其中βℓ是模式ℓ,K0 =2π/λ0的传播常数是真空波数和λ0是真空中的光的波长。 Ç数值计算用于耦合的间隔距离的优势D = 5微米,5.5微米,6微米,6.5微米,7微米,并使用λ0= 700nm的7.5微米。特别地,C0(十字)占C1(圆)和c2(正方形)帐户中的ℓ= 0模式之间的耦合,以及用于ℓ= 1种模式分别与相同或相反的方向循环,之间的耦合。虚线和实线对应于c0d≈K0exp(-κ0d),C1(d)≈K1exp(-κ1d)和c2(d)≈K2exp(-κ2d),其中K0 =387毫米-1,κ0的指数配件= 1.17微米-1,K1 =19.39毫米-1,κ1= 0.52微米-1,K2 =56.25毫米-1和κ2= 0.59微米-1。相对于该间隔距离d在(c)所示的插图C2 / C1

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