首页> 外文OA文献 >Doping Dependencies of Onset Temperatures for the Pseudogap and Superconductive Fluctuation in Bi$_{2}$Sr$_{2}$CaCu$_{2}$O$_{8+\delta}$, Studied from both In-Plane and Out-of-Plane Magnetoresistance Measurements
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Doping Dependencies of Onset Temperatures for the Pseudogap and Superconductive Fluctuation in Bi$_{2}$Sr$_{2}$CaCu$_{2}$O$_{8+\delta}$, Studied from both In-Plane and Out-of-Plane Magnetoresistance Measurements

机译:pseudogap和pseudogap的起始温度的掺杂依赖性   Bi $ _ {2} $ sr $ _ {2} $ CaCu $ _ {2} $ O $ _ {8+ \ delta} $中的超导波动,   研究了平面内和平面外的磁电阻测量

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摘要

To investigate the relationship between the pseudogap and superconductivity,we measured both the in-plane ($\rho_{ab}$) and out-of-plane ($\rho_c$)resistivity for oxygen-controlled Bi$_{2}$Sr$_{2}$CaCu$_{2}$O$_{8+\delta}$single crystals subject to magnetic fields (parallel to the $c$ axis) of up to17.5 T. The onset temperature for the superconductive fluctuation, $T_{scf}$,is determined by the large positive in-plane magnetoresistance (MR) andnegative out-of-plane MR observed near $T_c$, whereas the pseudogap openingtemperature $T^*$ is determined by the semiconductive upturn of the zero-field$\rho_c$. $T_{scf}$ was found to scale roughly as $T_c$, with a decreasingtemperature interval between them upon doping. On the other hand, $T^*$ startsout much higher than $T_{scf}$ but decreases monotonically upon doping;finally, at a heavily overdoped state, it is not observed above $T_{scf}$.These results imply that the pseudogap is not a simple precursor ofsuperconductivity, but that further study is needed to determine whether or not$T^*$ exists below $T_{scf}$ in the heavily overdoped state.
机译:为了研究伪间隙与超导性之间的关系,我们测量了氧气控制的Bi $ _ {2} $的面内($ \ rho_ {ab} $)和面外($ \ rho_c $)电阻率。 Sr $ _ {2} $ CaCu $ _ {2} $ O $ _ {8+ \ delta} $单晶受磁场(平行于$ c $轴)的最大作用为17.5T。超导波动$ T_ {scf} $是由在$ T_c $附近观察到的大的正面内磁阻(MR)和负面外MR决定的,而伪间隙开口温度$ T ^ * $是由零场$ \ rho_c $的半导体上升。发现$ T_ {scf} $的缩放比例大致为$ T_c $,掺杂时它们之间的温度间隔减小。另一方面,$ T ^ * $开始时比$ T_ {scf} $高得多,但在掺杂时单调减少;最后,在重度过量的状态下,在$ T_ {scf} $以上未观察到它。这些结果表明:伪间隙不是超导的简单先兆,但是还需要进一步研究以确定在重掺杂状态下$ T ^ * $是否低于$ T_ {scf} $。

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