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Optimized polar-azimuthal orientations for polarized light illumination of different superconducting nanowire single-photon detector designs

机译:针对不同超导纳米线单光子探测器设计的偏振光照明,优化了极性-方位角方向

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摘要

The optimum orientations were determined for polarized light illumination of three superconducting nanowire single-photon detector (SNSPD) designs consisting of niobium-nitride (NbN) stripes with dimensions according to conventional devices in 200 nm periodic pattern: (1) standing in air (bare-SNSPD), (2) below ~quarter-wavelength hydrogen-silsesquiox-ane (HSQ) filled nano-cavity (DC-SNSPD), and (3) below HSQ-filled nano-cavity closed by a thin gold reflector (OC-SNSPD). Computations showed that the optical response and near-field distribution vary significantly with polar angle φ, and these variations are analogous across all azimuthal angles γ, but are fundamentally different in different device designs. Larger absorptance is attainable due to p-polarized illumination of NbN patterns in P-orientation, while s-polarized illumination results in higher absorptance in S-orientation. As a result of p-polarized illumination, a global NbN absorptance maximum appears in bare-SNSPD at polar angle corresponding to attenuated total internal reflection (ATIR); in DC-SNSPD exactly at total internal reflection (TIR); and at perpendicular incidence in OC-SNSPD. S-polarized illumination results in a global NbN absorptance maximum in bare-SNSPD at TIR; in DC-SNSPD at polar angle corresponding to ATIR phenomenon; while large and almost polar angle independent absorptance is attainable in OC-SNSPD at small tilting.
机译:确定了三种超导纳米线单光子探测器(SNSPD)设计的偏振光的最佳取向,这些设计由氮化铌(NbN)条纹组成,其尺寸根据常规设备以200 nm周期性模式显示:(1)站在空气中(裸露) -SNSPD),(2)低于四分之一波长的氢硅倍半氧烷(HSQ)填充的纳米腔(DC-SNSPD),以及(3)低于HSQ填充的纳米腔且由薄金反射器(OC- SNSPD)。计算表明,光学响应和近场分布随极角φ发生很大变化,并且这些变化在所有方位角γ上都是相似的,但是在不同的器件设计中根本不同。由于P取向的NbN图案的p偏振照明可获得较大的吸收率,而s偏振照明的S取向吸收率较高。 P偏振照明的结果是,在裸SNSPD中,在与衰减的全内反射(ATIR)相对应的极角处,出现了一个整体的NbN吸收最大值。在DC-SNSPD中精确地处于全内反射(TIR);在OC-SNSPD中垂直入射。 S偏振照明会在TIR的裸SNSPD中导致全局NbN吸收率最大值;在DC-SNSPD中处于与ATIR现象相对应的极角;而在OC-SNSPD中,小倾斜时可获得大且几乎与极角无关的吸收率。

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