单晶C60压力诱导相变

在２９０Ｋ温度下和０－０．６００ＧＰａ流体静压国和范围内,通过对块体Ｃ６０单晶的直流电导测量,观察到在０．１７６ＧＰａ的压力下Ｃ６０单昌的电导发生一个大的跳跃,该跳跃对应于Ｃ６０单晶分子自旋取向从有序琶无序可逆相变。     

Ir（110）表面原子结构、氧原子吸附和STM图像的第一性原理研究

用密度泛函理论（DFT）的总能计算研究了金属Ir（110）表面结构以及氧原子的吸附状态.计算得到Ir（110）-（1×1）的外层表面间的弛豫分别是-13.3%（△d12/d0）和＋6.1%（△d23/d0）,表面能σ=175meV-2,功函数Φ=5.22eV;相应的Ir（110）-（1×2）缺列再构表面的△d12/d0=-9.7%,△d23/d0=-2.4%,表面能为169meV/2,Φ=5.33eV.研究Ir（110）-（1×1）和（1×2）再构表面氧吸附,发现各吸附位置的吸附能值均为正值,表明吸附为放热反应,且氧原子最有可能吸附在短桥位（shortbridgesite,SB）.同时我们还模拟计算Ir（110）-（1×2））缺列再构表面和氧吸附再构表面的扫描隧道显微镜（STM）图像并记录STM针尖的起伏变化,结果显示表面吸附氧的位置远高于{001}方向的铱原子列,但是在STM形貌图上氧原子基本上没有凸起.     

Electronic structure and magnetism of RMn6Sn6 （R=Tb, Dy）

This article reports first-principles band structure calculations for RMn6Sn6 (R= Tb, Dy). The calculation uses the linear muffin-tin orbitals (LMTO) method in the atomic-sphere-approximation (ASA),and yields results showing that both TbMn6Sn6 and DyMn6Sn6 are ferrimagnetic compounds with antiparallel aligned moments of R and Mn atoms. In this research the 4f states of R atoms are treated as localized states,i. e., the hybridization of 4f states with other valence electrons is neglected. The moments of Mn in both compounds were determined to be 2.43μB and 2.38μB, respectively. The considerably small additional moments for Mn from the spin-orbit coupling indicates that the spin-orbital coupling is not dominated for Mn atoms. The total moments of Tb and Dy atoms are 10.28μB and 11.20μB. All the calculation findings accorded well with experimental results.