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Yukihiro Endo

Publications and source records attributed to Yukihiro Endo.

3 recordsLinked to original sources

Non-Centrosymmetric $\gamma$-Phase GaS Nanobelts for On-Chip Nonlinear Photonic Applications

Second-order nonlinear optical processes in van der Waals (vdW) semiconductors offer a compelling route toward compact, integrable photon-conversion platforms. Among III-VI vdW semiconductors, GaS is particularly attractive owing to its wide bandgap suppressing two-photon absorption under near-infrared laser excitation. However, bulk GaS typically crystallizes in the centrosymmetric $\beta$ phase, which eliminates second-order nonlinearity and severely limits its application in nonlinear photonics. Here, we demonstrate that GaS nanobelts synthesized via self-catalyzed vapor-liquid-solid growth predominantly crystallize in non-centrosymmetric $\gamma$-phase stacking. This behavior originates from edge-selective growth kinetics at the Ga catalyst interface, which stabilizes the $\gamma$ phase and enables deterministic in-plane dipole moment alignment. The GaS nanobelts exhibit strong second-harmonic generation (SHG) with intensities comparable to those of GaSe, a widely used nonlinear optical material. Furthermore, we integrate the nanobelts onto SiN waveguides and demonstrate efficient on-chip SHG and sum-frequency generation. These results establish $\gamma$-GaS nanobelts as a transferable one-dimensional nonlinear materials well suited for on-chip photonic integration and indicate their strong potential for nonlinear optical applications.

physics.optics

Two-dimensional superconductivity of the Ca-intercalated graphene on SiC: vital role of the interface between monolayer graphene and the substrate

Ca-intercalation has opened a way for superconductivity in graphene on SiC. However, the atomic and electronic structures being critical for superconductivity are still under discussion. We find the essential role of the interface between monolayer graphene and the SiC substrate for superconductivity. In the Ca-intercalation process, at the interface a carbon layer terminating SiC changes to graphene by Ca-termination of SiC (monolayer graphene becomes bilayer) with inducing more carriers than a free-standing model. Then, Ca is intercalated in-between graphene layers, which shows superconductivity with the updated critical temperature ($T_{C}$) of up to 5.7 K. In addition, the relation between $T_{C}$ and the normal-state conductivity is unusual, "dome-shape". These findings are beyond the simple C6CaC6 model in which s-wave BCS superconductivity is theoretically predicted. This work proposes a general picture of the intercalation-induced superconductivity in graphene on SiC, and shed the light on the potential of superconductivity induced by other intercalants.

cond-mat.mes-hall

Berry phase shift from 2 $π$ to $π$ in Bilayer graphene by Li-intercalation and sequential desorption

We have found that the Berry phase of bilayer graphene becomes from 2$π$ estimated by Shubnikov-de Haas oscillations when the A-B stacked pristine bilayer graphene experiences the Li-intercalation and sequential Li-desorption process in ultrahigh vacuum. Furthermore, the mobility of such processed bilayer graphene increases around four times larger, ~ 8,000 cm2/V$\cdot$s, than that of the pristine bilayer graphene. This is mainly due to increment of the scattering time and decrement of the cyclotron mass, which can be interpreted as a result of the change of the stacking structure of bilayer graphene from A-B to A-A, corresponding to a change from the parabolic to the linear band dispersion.

cond-mat.mes-hall