首页> 外文OA文献 >Upper critical field measurements up to 60 T in arsenic-deficient LaO_(0.9)F_(0.1)FeAs_(1-delta): Pauli limiting behaviour at high fields vs improved superconductivity at low fields
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Upper critical field measurements up to 60 T in arsenic-deficient LaO_(0.9)F_(0.1)FeAs_(1-delta): Pauli limiting behaviour at high fields vs improved superconductivity at low fields

机译:在砷缺乏的情况下,上临界场测量高达60 T.   LaO_(0.9)F_(0.1)Feas_(1-delta):pauli限制高场的行为vs   在低场改善超导性

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摘要

We report resistivity and upper critical field B_c2(T) data for As deficientLaO_(0.9)F_(0.1)FeAs_(1-delta) in a wide temperature and high field range up to60 T. These disordered samples exhibit a slightly enhanced superconductingtransition at T_c = 29 K and a significantly enlarged slope dB_(c2))/dT = -5.4T/K near T_c which contrasts with a flattening of B_(c2)(T) starting near 23 Kabove 30 T. This flattening is interpreted as Pauli limiting behaviour (PLB)with B_(c2)(0) approx 63 T. We compare our results with B_(c2)(T)-data reportedin the literature for clean and disordered samples. Whereas clean samples showno PLB for fields below 60 to 70 T, the hitherto unexplained flattening ofB_(c2)(T) for applied fields H || ab observed for several disordered closelyrelated systems is interpreted also as a manifestation of PLB. Consequences ofour results are discussed in terms of disorder effects within the frame ofconventional and unconventional superconductivity.
机译:我们报道了在高达60 T的宽温度和高磁场范围内As缺陷LaO_(0.9)F_(0.1)FeAs_(1-δ)的电阻率和上临界场B_c2(T)数据。这些无序样品在T_c处显示出稍微增强的超导转变= 29 K,并且在T_c附近显着增大的斜率dB_(c2))/ dT = -5.4T / K,这与B_(c2)(T)在23 K高于30 T附近开始展平形成对比。这种展平被解释为Pauli限制B_(c2)(0)约63 T时的行为(PLB)。我们将我们的结果与文献中报道的干净和无序样品的B_(c2)(T)数据进行比较。低于60 T到70 T的磁场显示为PLB的干净样品,而对于施加的磁场H ||则迄今无法解释的B_(c2)(T)展平。在几个无序的密切相关的系统中观察到的ab也被解释为PLB的一种表现。我们在常规和非常规超导性框架内的无序效应方面讨论了结果的后果。

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