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首页> 外文期刊>Low temperature physics: Simultaneous Russian - English publication >ab-plane tunneling and Andreev spectroscopy of the superconducting gap and pseudogap in (Bi,Pb){sub}2Sr{sub}2Ca{sub}2Cu{sub}3O{sub}(10+δ) and Bi{sub}2Sr{sub}2CaCu{sub}2O{sub](8+δ)
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ab-plane tunneling and Andreev spectroscopy of the superconducting gap and pseudogap in (Bi,Pb){sub}2Sr{sub}2Ca{sub}2Cu{sub}3O{sub}(10+δ) and Bi{sub}2Sr{sub}2CaCu{sub}2O{sub](8+δ)

机译:(Bi,Pb){sub} 2Sr {sub} 2Ca {sub} 2Cu {sub} 3O {sub}(10 +δ)和Bi {sub} 2Sr { sub} 2CaCu {sub} 2O {sub](8 +δ)

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摘要

We have measured the temperature dependence of gap features revealed by Andreev reflection (Δ{sub}s) and by tunneling (Δ) in the ah plane of optimally and slightly overdoped microcrystals of (BiPb){sub}2Sr{sub}2Ca{sub}2Cu{sub}3O{sub}(10+δ) (Bi2223) with critical temperature T{sub}c = 110-115 K, and Bi{sub}2Sr{sub}2CaCu{sub}2O{sub}(8+δ) (Bi2212) with T{sub}c= 80-84 K. The tunneling conductance of a Bi2223-insulator-Bi2223 junction shows peaks at the 2Δ gap voltage, as well as dips and broad humps at other voltages. In Bi2223, similarly to the well-known Bi2212 spectra, the energies corresponding to 2Δ, to the dip, and to the hump structure are in the ratio 2:3:4. This confirms that the dip and hump features are generic to the high-temperature superconductors, irrespective of the number of CuO{sub}2 layers or the BiO superstructure. On the other hand, in both compounds the Δ(T) and Δ{sub}s(T) dependences are completely different, and we conclude that the two entities are of different natures.
机译:我们已经测量了由安德列夫反射(Δ{sub} s)和在(BiPb){sub} 2Sr {sub} 2Ca {sub } 2Cu {sub} 3O {sub}(10 +δ)(Bi2223),其临界温度为T {sub} c = 110-115 K,并且Bi {sub} 2Sr {sub} 2CaCu {sub} 2O {sub}(8 +δ)(Bi2212),T {sub} c = 80-84K。Bi2223-绝缘体-Bi2223结的隧穿电导在2Δ间隙电压处显示峰值,在其他电压处出现骤降和宽峰。在Bi2223中,类似于众所周知的Bi2212光谱,对应于2Δ,下陷和峰状结构的能量之比为2:3:4。这证实了浸入和驼峰特征是高温超导体所通用的,而与CuO {sub} 2层数或BiO上层结构无关。另一方面,在这两种化合物中,Δ(T)和Δ{sub} s(T)的依赖性完全不同,因此我们得出结论,这两个实体具有不同的性质。

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