Spin gap and hole pairing in the spin-ladder cuprate Sr(14-x)A(x)Cu(24)O(41) (A=Ca and La) studied by the thermal conductivity

Citation
K. Kudo et al., Spin gap and hole pairing in the spin-ladder cuprate Sr(14-x)A(x)Cu(24)O(41) (A=Ca and La) studied by the thermal conductivity, J PHYS JPN, 70(2), 2001, pp. 437-444
Citations number
47
Categorie Soggetti
Physics
Journal title
JOURNAL OF THE PHYSICAL SOCIETY OF JAPAN
ISSN journal
00319015 → ACNP
Volume
70
Issue
2
Year of publication
2001
Pages
437 - 444
Database
ISI
SICI code
0031-9015(200102)70:2<437:SGAHPI>2.0.ZU;2-D
Abstract
We have systematically measured the thermal conductivity kappa of Sr(14-x)A (x)Cu(24)O(41) (A=Ca, La: 0 less than or equal to x(Ca) less than or equal to 9: 0 less than or equal to x(La) less than or equal to 5) single crystal s, in order to investigate the spin gap and hole pairing. The observed kapp a has been analyzed to he composed of kappa (ph),kappa (spin) and kappa (ho le) due to phonons, spins and holes, respectively. The contribution of kapp a (spin) is observed only along the c-axis except for x(Ca) greater than or equal to 6. The spin gap in the ladder estimated from kappa (spin) is simi lar to 400 K and independent of x. This is regarded as corresponding to the spin excitation from spin-singlet to spin-triplet, as those estimated from the neutron scattering and Raman scattering measurements. The contribution of kappa (hole) is observed at high temperatures for larger x(Ca) values. The activation energy of holes in the ladder estimated from kappa (hole) de creases with increasing x(Ca). This is regarded as corresponding to the dis sociation of hole pairs, as that estimated from the electrical resistivity measurements. These results are consistent with the recent suggestion that most of holes are paired and localized in the ladder at low temperatures.