TY - JOUR
T1 - Systematic NMR studies of high-Tc and two-leg spin-ladder systems
AU - Kitaoka, Y.
AU - Magishi, K.
AU - Matsumoto, S.
AU - Ishida, K.
AU - Ohsugi, S.
AU - Asayama, K.
AU - Uehara, M.
AU - Nagata, T.
AU - Akimitsu, J.
N1 - Funding Information:
The authors would like to express their thanks to T.M. Rice, H. Fukuyama, M. Imada, N. Nagaosa, M. Ogata, H. Tsunetsugu, M. Takano, S. Uchida, B. Battlog, Z. Hiroi, Y. Koike and Y. Eisaki for stimulating discussions and comments. This work has been supported by CREST (Core Research for Evolutional Science and Technology) of Japan Science and Technology Corporation (JST) and also partly by a Grant-in-Aid from the Ministry of Education, Science and Culture of Japan.
PY - 1998/1
Y1 - 1998/1
N2 - We review systematic NMR studies on underdoped high-Tc, cuprates and two-leg spin-ladder systems, focusing on their spin gap and dynamics. The pressure-induced superconductivity was discovered in Sr14-xCaxCu24O41 comprising the quasi-one-dimensional S = 1/2 two-leg spin-ladder Cu2O3 planes. Remarkably, the new parent cuprate is the Mott insulator with the spin gap in contrast to the antiferromagnetic (AF) insulator for the high-Tc cuprates. From the Cu-NMR results in the ladder Cu2O3 plane on single crystals Sr14-xCaxCu24O41 with x = 9 (hereafter denoted as Ca9) and x = 11.5 (Ca11.5), it is shown that the spin gap, Δ = 510 K in the Sr14 is significantly reduced upon isovalent Ca substitution, but its magnitude remains nearly constant with Δ = 270 and 280 K for the Ca9 and Ca11.5, respectively. In T range of T ≥ Δ, the spin dynamics in carrier-doped two-leg spin-ladder systems are characterized by the behaviour similar to the S = 1/2 1D Heisenberg system. By contrast, the transport property shares a common feature, i.e, due to the spin-gap opening the charge transport is confined in the 2D CuO2 plane for underdoped high-Tc cuprates and in the quasi-1D ladder for spin-ladder compounds.
AB - We review systematic NMR studies on underdoped high-Tc, cuprates and two-leg spin-ladder systems, focusing on their spin gap and dynamics. The pressure-induced superconductivity was discovered in Sr14-xCaxCu24O41 comprising the quasi-one-dimensional S = 1/2 two-leg spin-ladder Cu2O3 planes. Remarkably, the new parent cuprate is the Mott insulator with the spin gap in contrast to the antiferromagnetic (AF) insulator for the high-Tc cuprates. From the Cu-NMR results in the ladder Cu2O3 plane on single crystals Sr14-xCaxCu24O41 with x = 9 (hereafter denoted as Ca9) and x = 11.5 (Ca11.5), it is shown that the spin gap, Δ = 510 K in the Sr14 is significantly reduced upon isovalent Ca substitution, but its magnitude remains nearly constant with Δ = 270 and 280 K for the Ca9 and Ca11.5, respectively. In T range of T ≥ Δ, the spin dynamics in carrier-doped two-leg spin-ladder systems are characterized by the behaviour similar to the S = 1/2 1D Heisenberg system. By contrast, the transport property shares a common feature, i.e, due to the spin-gap opening the charge transport is confined in the 2D CuO2 plane for underdoped high-Tc cuprates and in the quasi-1D ladder for spin-ladder compounds.
KW - High-Tcuprates
KW - NMR
KW - Quantum fluctuation
KW - Spin gap
KW - Spin ladder
KW - Superconductivity
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U2 - 10.1016/S0304-8853(97)00613-6
DO - 10.1016/S0304-8853(97)00613-6
M3 - Article
AN - SCOPUS:0031708509
SN - 0304-8853
VL - 177-181
SP - 487
EP - 492
JO - Journal of Magnetism and Magnetic Materials
JF - Journal of Magnetism and Magnetic Materials
IS - PART 1
ER -