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NbN nanowire superconducting single photon detectors fabricated on MgO substrates

机译:NBN纳米线超导单光子探测器,在MgO基板上制造

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High sensitivity ultrafast nanowire superconducting single photon detectors (SSPD) in the near infrared wavelength range have been fabricated with ultrathin (3.5nm) NbN films grown on R-plane sapphire substrates by dc reactive magnetron sputtering in Ar+N{sub}2 mixture [1]. The main drawback of this approach is that in order to obtain the superconducting δ cubic fcc phase of NbN the substrate must be heated up to 900°C during deposition, which makes it difficult to integrate the detector with waveguides and microcavities, typically realized on other substrates (such as GaAs and Si) and not compatible with these temperatures. In an effort to develop an exportable technology, NbN films ranging from 3.5 to 150nm in thickness have been deposited by current controlled dc magnetron sputtering in a mixture of Ar and N{sub}2 on single crystal MgO and GaAs substrates. Substrate temperature T{sub}S during deposition was as low as 500°C. In order to maximize the critical temperature T{sub}C, effects of the reactive gas total pressure P{sub}(tot) and composition on film crystal structure and electrical properties have been studied. For 150nm thick films, T{sub}C reaches a maximum of 16.1K on MgO and 14.8K on GaAs, which are state of the art values. In 5nm thick films, T{sub}Cs as high as 10K and 11K have been obtained on GaAs and MgO, respectively (Fig. 1).
机译:通过在ar + n {sab} 2混合物中的DC反应磁控溅射在R平面蓝宝石衬底上生长的超薄(3.5nm)NBN膜,在近红外波长范围内制造高灵敏度超速纳米线超导单光子探测器(SSPD)。 1]。该方法的主要缺点是为了获得NBN的超导δ立方FCC阶段,在沉积期间必须将基板加热至900℃,这使得难以将检测器与波导和微覆盖集成,通常在其他方面实现基板(如GaAs和Si),与这些温度不兼容。在开发出可出口技术的努力中,通过在单晶MgO和GaAs基板上的AR和N {Sub} 2的混合物中,通过电流控制的DC磁控管溅射沉积从3.5至150nm的NBN膜沉积。沉积期间的衬底温度T {亚} S低至500℃。为了最大化临界温度T {Sub} C,研究了反应气体总压力P {SUB}(TOT)和组合物对薄膜晶体结构和电性能的影响。对于150nm厚的薄膜,T {Sub} C最多达到16.1K的MgO和14.8K在GaAs上,这是最先进的值。在5nm厚的薄膜中,在GaAs和MgO上分别获得高达10k和11k的T {Sub} Cs(图1)。

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