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Correlation between the Doping Dependences of Superconducting Gap Magnitude<b>2</b><i>Δ<sub><b>0</b></sub></i>and Pseudogap Temperature<i><i>T</i><sup>*</sup></i>in High-<i><i>T</i><sub><b><i>c</i></b></sub></i>Cuprates
142
Citations
13
References
1998
Year
Superconducting MaterialMagnetic PropertiesEngineeringCacu 2Magnetic MaterialsMagnetismSuperconductivityQuantum MaterialsHigh Tc SuperconductorsSuperconducting DevicesLow-temperature SuperconductivityMaterials ScienceSpin-charge-orbit ConversionSr 2High-tc SuperconductivityPhysicsDoping DependencesHigh-temperature SuperconductivityNatural SciencesCondensed Matter PhysicsApplied PhysicsQuantum SuperconductivityO 8+δ
We report that in La 2- x Sr x CuO 4 (La214) and Bi 2 Sr 2 CaCu 2 O 8+δ (Bi2212), the resistivity ρ and magnetic susceptibility χ decrease more sharply below T * , corresponding to the onset temperature of a spin gap (pseudogap) at least for Bi2212. In each system, T * scales with the superconducting gap magnitude 2Δ 0 ( T * ∼2Δ 0 /4.3 k B ), which increases as the doping level is lowered. We also report that 2Δ 0 is almost proportional to T max (> T * ), where T max is the temperature exhibiting a broad peak of χ and k B T max has been considered to give the measure of effective exchange energy J eff ; the α factors in 2Δ 0 ∼α k B T max ∼α J eff are nearly one and two for La214 and Bi2212, respectively.
| Year | Citations | |
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1995 | 2K | |
1996 | 1.3K | |
1996 | 901 | |
1990 | 209 | |
1992 | 181 | |
1994 | 158 | |
1997 | 118 | |
1996 | 82 | |
1994 | 65 | |
1990 | 33 |
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