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Role of engineered materials in superconducting tunnel-junction x-ray detectors: suppression of quasi-particle recombination losses via a phononic bandgap

机译:工程材料在超导隧道结X射线探测器中的作用:通过声子带隙抑制准粒子复合损失

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Abstract: While much progress has been made towards improvedenergy resolution in STJ detectors recently, resultsare still more than an order of magnitude worse thanthe theoretical limit. Several factors have beenidentified as contributing to degradation of energyresolution in STJ devices: recombination losses,parasitic quasiparticle trapping and quasiparticlediffusion into current leads. In addition, STJdetectors tend to have poor photon capture efficiency.Semiconducting detectors achieve their near theoreticalenergy resolutions and high efficiencies via dopingand/or applying an external field to a pure substance.These methods are ineffective for STJ detectors,therefore engineered materials (consisting of multiplematerials artificially patterned on the microscopiclevel) should be considered. The most common engineeredstructures in use are quasiparticle trappingconfigurations which alleviate lead diffusion anddetection efficiency problems, and we have proposed amultilayered approach which addresses parasitictrapping along with diffusion and efficiency. We nowpropose the possibility of a engineered structure whichwill alleviate quasiparticle recombination losses viathe existence of a phononic band gap which overlaps the2$Delta energy of phonons produced during recombinationof quasiparticles. We will present a 1D Kronig-Pennymodel for phonons normally incident to the layers of amultilayered superconducting tunnel junction as anidealized example.!12s
机译:摘要:尽管最近在提高STJ探测器的能量分辨率方面已取得了很大进展,但结果仍比理论极限差一个数量级。已经发现有几种因素导致STJ器件的能量分辨率降低:复合损失,寄生准粒子捕获和准粒子扩散到电流引线中。此外,STJ检测器往往具有较差的光子捕获效率。半导体检测器通过对纯物质进行掺杂和/或施加外场来达到其接近理论的能量分辨率和高效率。这些方法对STJ检测器无效,因此对工程材料(包括多种材料)应该考虑在微观水平上人工制作图案)。使用中最常见的工程结构是准粒子捕获配置,可缓解铅扩散和检测效率问题,我们提出了一种多层方法,可解决寄生捕获以及扩散和效率问题。现在我们提出一种工程结构的可能性,该结构将通过存在声子带隙而减轻准颗粒的复合损失,该声子带隙与在准颗粒的重组过程中产生的声子的2Δ能量重叠。我们将提出一个声子的一维Kronig-Penny模型,通常将其入射到多层超导隧道结的各层,作为理想的例子。12s

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