TY - JOUR
T1 - Effects of high magnetic fields on the pseudogap and d-wave superconductivity in the underdoped and overdoped high-Tc superconductors
AU - Zheng, Guo Qing
AU - Ozaki, H.
AU - Clark, W. G.
AU - Sakai, M.
AU - Kitaoka, Y.
AU - Kodama, Y.
AU - Kondo, T.
AU - Shimakawa, Y.
AU - Kubo, Y.
AU - Kuhns, P.
AU - Reyes, A. P.
AU - Moulton, W. G.
PY - 2000
Y1 - 2000
N2 - Based on measurements of the 63Cu Knight shift and the nuclear spin-lattice relaxation rate under magnetic fields up to 28 T, we find that the pseudogap in the slightly overdoped TlSr2CaCu2O6.88 (Tc=68 K) is due to Cooper pair density fluctuations. Such fluctuations are also found in the underdoped YBa2Cu4O8 (Tc=74 K), but are small and only survive up to Tsf ≃ Tc+15K=90 K, which is much lower than the field-independent pseudogap temperature T* ≃ 160 K. The implication on the phase diagram is discussed. At low temperatures in the superconducting state, a field-induced finite density of states was found in both compounds and is interpreted as due to the quasiparticles outside a vortex core in a d-wave superconductor.
AB - Based on measurements of the 63Cu Knight shift and the nuclear spin-lattice relaxation rate under magnetic fields up to 28 T, we find that the pseudogap in the slightly overdoped TlSr2CaCu2O6.88 (Tc=68 K) is due to Cooper pair density fluctuations. Such fluctuations are also found in the underdoped YBa2Cu4O8 (Tc=74 K), but are small and only survive up to Tsf ≃ Tc+15K=90 K, which is much lower than the field-independent pseudogap temperature T* ≃ 160 K. The implication on the phase diagram is discussed. At low temperatures in the superconducting state, a field-induced finite density of states was found in both compounds and is interpreted as due to the quasiparticles outside a vortex core in a d-wave superconductor.
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U2 - 10.1016/S0921-4534(00)00703-6
DO - 10.1016/S0921-4534(00)00703-6
M3 - Article
AN - SCOPUS:0343832821
SN - 0921-4534
VL - 341-348
SP - 819
EP - 822
JO - Physica C: Superconductivity and its Applications
JF - Physica C: Superconductivity and its Applications
IS - PART 3
ER -