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Two-band superconductivity in LaFeAsO_(0.89)F_(0.11) at very high magnetic fields

机译:LaFeAsO_(0.89)F_(0.11)在非常高的磁场中的两波段超导性

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The recent synthesis of the superconductor LaFeAsO_(0.89)F_(0.11) with transition temperature T_c ≈ 26 K (refs 1-4) has been quickly followed by reports of even higher transition temperatures in related compounds: 41K in CeFeAsO_(0.84)F_(0.16)(ref. 5), 43K in SmFeAsO_(0.9)F_(0.1)(ref. 6), and 52 K in NdFeAsO_(0.89)F_(0.11) and PrFeAsO_(0.89)F_(0.11)(refs 7, 8). These discoveries have generated much interest in the mechanisms and manifestations of unconventional superconductivity in the family of doped quaternary layered oxypnictides LnOTMPn (Ln: La, Pr, Ce, Sm; TM: Mn, Fe, Co, Ni; Pn: P, As), because many features of these materials set them apart from other known superconductors. Here we report resistance measurements of LaFeAsO_(0.89)F_(0.11) at high magnetic fields, up to 45 T, that show a remarkable enhancement of the upper critical field B_(c2) compared to values expected from the slopes dB_(c2)/dT ≈ 2 T K~(-1) near T_c, particularly at low temperatures where the deduced B_(c2)(0) ≈ 63-65 T exceeds the paramagnetic limit. We argue that oxypnictides represent a new class of high-field superconductors with B_(c2) values surpassing those of Nb_3Sn, MgB_2 and the Chevrel phases, and perhaps exceeding the 100 T magnetic field benchmark of the high-T_c copper oxides.
机译:最近合成了转变温度T_c≈26 K(参考1-4)的超导体LaFeAsO_(0.89)F_(0.11),随后报道了相关化合物的转变温度更高:CeFeAsO_(0.84)F_( 0.16)(参考5),SmFeAsO_(0.9)F_(0.1)(参考6)中的43K和NdFeAsO_(0.89)F_(0.11)和PrFeAsO_(0.89)F_(0.11)中52K(参考7,8 )。这些发现引起了人们对掺杂四元层状氧化氧LnOTMPn(Ln:La,Pr,Ce,Sm; TM:Mn,Fe,Co,Ni; Pn:P,As)系列中超常规超导电性的机制和表现形式的浓厚兴趣。 ,因为这些材料的许多特性使它们与其他已知的超导体区分开来。在这里,我们报告了LaFeAsO_(0.89)F_(0.11)在高达45 T的高磁场下的电阻测量结果,与从斜率dB_(c2)/得出的期望值相比,显示了上临界场B_(c2)的显着提高。 dT≈2 TK〜(-1)在T_c附近,特别是在推定的B_(c2)(0)≈63-65 T超过顺磁极限的低温下。我们认为,氧素代表了一类新的高场超导体,其B_(c2)值超过了Nb_3Sn,MgB_2和Chevrel相的值,并且可能超过了高T_c铜氧化物的100 T磁场基准。

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