arXiv subjects

Ichiro Terasaki

Publications and source records attributed to Ichiro Terasaki.

40 records · Page 3Linked to original sources

arXiv2002

Block-Layer Concept for the Layered Co Oxide: A Design for Thermoelectric Oxides

High-Tc Cu oxides consist of the alternating stack of the superconductive CuO2 layer and the block layer, such as Bi2Sr2O4 or La2-xSrxO2. By changing the block layer, we can change their physical properties, such as transition temperature Tc. The thermoelectric Co oxides have a similar layered structure composed of the conductive CoO2 layer and the blocking layer. Thus, we propose that their thremoelectric properties can be finely tuned by modifying the block layer.

cond-mat.str-el↗

arXiv2002

Doping Dependence of Anisotropic Resistivities in Trilayered Superconductor Bi2Sr2Ca2Cu3O10+delta (Bi-2223)

The doping dependence of the themopower, in-plane resistivity rho_ab(T), out-of-plane resistivity rho_c(T), and susceptibility has been systematically measured for high-quality single crystal Bi2Sr2Ca2Cu3O10+delta. We found that the transition temperature Tc and pseudogap formation temperature T_rho_c*, below which rho_c shows a typical upturn, do not change from their optimum values in the "overdoped" region, even though doping actually proceeds. This suggests that, in overdoped region, the bulk $T_c$ is determined by the always underdoped inner plane, which have a large superconducting gap, while the carriers are mostly doped in the outer planes, which have a large phase stiffness.

cond-mat.supr-con↗

arXiv2002

In-plane Anisotropy on Resistivity and Thermopower in The Misfit Layered Oxide Bi2-xPbxSr2Co2Oy

We investigated the in-plane anisotropy on the resistivity and thermopower of Bi2-xPbxSr2Co2Oy single crystals, which have a misfit structure between the hexagonal CoO2 layer and the rock salt Bi2Sr2O4 layer. The resistivity and thermopower show significantly large anisotropy, which exceeds two at maximum. This anisotropy would come from the anisotropic pseudogap formation enhanced by the misfit structure. The thermopower changes with Pb doping to take a maximum at x=0.4. The misfit structure improves the thermoelectric properties through chemical pressure. The power factor is as large as 9 muW/cmK2 at 100 K for x=0.6, which is the highest value for thermoelectric oxides at 100 K.

cond-mat.str-el↗

arXiv1994

Kosterlitz-Thouless Transition in Bi${}_2$Sr${}_2$CaCu${}_2$O${}_8+δ$ Thin Films

Current-voltage ($I-V$) characteristics and the increase of superconducting transition temperature $T_c$ as a function of the number of half-unit-cell layers $n$ are studied on Bi${}_2$Sr${}_2$CaCu${}_2$O${}_{8+δ}$ thin films grown by molecular beam epitaxy. These observations are interpreted in terms of Kosterlitz-Thouless (KT) transition associated with vortex string threading the film. Considering the change in the types of the lowest free-energy excitations as a function of the size of vortex pair, we have formulated KT renormalization-group (RG) equations. Using experimental data obtained with Bi${}_2$Sr${}_2$CaCu${}_2$O${}_{8+δ}$ thin films, we have solved the RG equations. It is shown that the KT transition occurs in the vortex-string region with interstring $\ln r$ interaction only. Our calculation successfully explains KT scaling in $I-V$ characteristics and the relation between $T_c$ and $n$. These results indicate that the interlayer interaction plays an important role in Bi${}_2$Sr${}_2$CaCu${}_2$O${}_{8+δ}$ thin films.

cond-mat↗