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首页> 外文期刊>Physica, C. Superconductivity and its applications >Superconducting condensate formation in quasi-2D systems with arbitrary carrier density
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Superconducting condensate formation in quasi-2D systems with arbitrary carrier density

机译:具有任意载流子密度的准二维系统中的超导冷凝物形成

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A phase diagram for a quasi-2D metal with variable carrier density has been derived. The phases present are the normal phase, where the order parameter is zero; the pseudogap phase where the absolute value of the order parameter is non-zero but its phase is random, and a superconducting phase with a crossover quasi-2D Berezinskii-Kosterlitz-Thouless (BKT) region. The crossover region is bounded by the quasi-2D BKT temperature and the temperature for the onset of conventional long-range order (CLRO). The practical observation of these regions, however, critically depends on the carrier density. At high densities both the pseudogap and BKT regions vanish asymptotically. i.e one obtains the standard BCS picture. At intermediate densities the pseudogap phase is large but the BKT region is negligible. Finally, at very low densities both the pseudogap and BKT regions are sizeable. An attempt is made to explain the behaviour observed in underdoped (intermediate densities) and optimally doped high-T sub(c) superconducting compounds above their critical temperature. The transition to the pseudogap phase should also be regarded as a crossover.
机译:推导了具有可变载流子密度的准二维金属的相图。存在的阶段是正常阶段,其中阶数参数为零;否则为零。伪间隙相位,其中阶跃参数的绝对值非零,但其相位是随机的,以及具有交叉准2D Berezinskii-Kosterlitz-Thouless(BKT)区域的超导相位。交越区的边界为准2D BKT温度和常规远程顺序(CLRO)的起始温度。然而,对这些区域的实际观察主要取决于载流子密度。在高密度下,伪间隙和BKT区域都渐近消失。即,获得标准的BCS图片。在中等密度下,伪间隙相很大,但BKT区可忽略不计。最后,在非常低的密度下,伪间隙和BKT区域都相当大。试图解释在临界温度以上在低掺杂(中等密度)和最佳掺杂的高T sub(c)超导化合物中观察到的行为。过渡到伪间隙阶段也应视为交叉。

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