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首页> 外文期刊>Journal of Physics. Condensed Matter >Universal doping evolution of the superconducting gap anisotropy in single crystals of electron-doped Ba(Fe1-xRhx)(2)As-2 from London penetration depth measurements
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Universal doping evolution of the superconducting gap anisotropy in single crystals of electron-doped Ba(Fe1-xRhx)(2)As-2 from London penetration depth measurements

机译:来自伦敦渗透深度测量的电子掺杂Ba(Fe1-XRHX)(2)AS-2单晶超导间隙各向异性的通用掺杂演化

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Doping evolution of the superconducting gap anisotropy was studied in single crystals of 4d-electron doped Ba(Fe1-xRhx)(2)As-2 using tunnel diode resonator measurements of the temperature variation of the London penetration depth Delta lambda(T). Single crystals with doping levels representative of an underdoped regime x = 0.039 (T-c = 15.5 K), close to optimal doping x = 0.057 (T-c = 24.4 K) and overdoped x = 0.079 (T-c = 21.5 K) and x = 0.131 (T-c = 4.9 K) were studied. Superconducting energy gap anisotropy was characterized by the exponent, n, by fitting the data to the power-law, Delta lambda = AT(n). The exponent n varies non-monotonically with x, increasing to a maximum n = 2.5 for x = 0.079 and rapidly decreasing towards overdoped compositions to 1.6 for x = 0.131. This behavior is qualitatively similar to the doping evolution of the superconducting gap anisotropy in other iron pnictides, including hole-doped (Ba,K) Fe2As2 and 3d-electron-doped Ba(Fe,Co)(2)As-2 superconductors, finding a full gap near optimal doping and strong anisotropy toward the ends of the superconducting dome in the T-x phase diagram. The normalized superfluid density in an optimally Rh-doped sample is almost identical to the temperature-dependence in the optimally doped Ba(Fe,Co)(2)As-2 samples. Our study supports the universal superconducting gap variation with doping and s(+/-) pairing at least in iron based superconductors of the BaFe2As2 family.
机译:使用隧道二极管谐振器测量的伦敦渗透深度Delta Lambda(T)的温度变化的隧道二极管谐振器测量,研究了超导间隙各向异性的超导间隙各向异性的掺杂演变。具有掺杂水平的单晶,代表欠型状态x = 0.039(Tc = 15.5 k),接近最佳掺杂X = 0.057(Tc = 24.4k),过掺杂x = 0.079(Tc = 21.5 k)和x = 0.131(Tc研究了= 4.9 k)。超导能隙各向异性的特征在于,通过将数据拟合到电力法,Delta Lambda = AT(n)。指数n与X无单调地变化,x = 0.079增加到最大n = 2.5,并且朝向X = 0.131的X = 0.131的覆盖组合物快速降低至1.6。这种行为与其他铁突出的超导间隙各向异性的掺杂演变具有定性类似的,包括空穴掺杂(Ba,K)Fe2as2和3D电子掺杂的Ba(Fe,Co)(2)SuS-2超导体,发现在TX相图中,在超导圆顶的末端靠近最佳掺杂和强四个各向异性的完全间隙。最佳Rh掺杂样品中的归一化的超流密度与最佳掺杂的Ba(Fe,Co)(2)AS-2样品中的温度依赖性几乎相同。我们的研究支持至少在Bafe2As2家族的铁基超导体中对掺杂和S(+/-)配对的通用超导间隙变化。

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