...
首页> 外文期刊>Physical review >Charge transfer and structure of K/Si(111)-2~(1/2)3 x 2~(1/2)3-B surface studied by reflection high-energy positron diffraction
【24h】

Charge transfer and structure of K/Si(111)-2~(1/2)3 x 2~(1/2)3-B surface studied by reflection high-energy positron diffraction

机译:反射高能正电子衍射研究K / Si(111)-2〜(1/2)3 x 2〜(1/2)3-B表面的电荷转移和结构

获取原文
获取原文并翻译 | 示例
   

获取外文期刊封面封底 >>

       

摘要

The atomic coordinates and charge transfer of the K/Si(l11)-2~(1/2)3 × 2~(1/2)5-B surface were investigated using reflection high-energy positron diffraction (RHEPD). Upon the adsorption of K onto the Si( 111 )-~(1/2)3 × ~(1/2)3-B surface, the position of the 111 Bragg reflection is shifted to a lower angle, thus suggesting that a change in the inner potential arises from the charge transfer of 1.Oe~- per K atom to the surface. From RHEPD rocking curves recorded at 113 K, we determined that the top K atoms and the Si adatoms are adsorbed 2.96 and 2.51 A from the first Si layer, respectively. The Si adatoms are significantly displaced upward compared to that found for the Si(l 11)-~(1/2)3 x ~(1/2)3-B surface. Furthermore, we found that the K atoms are adsorbed between the H_3 and T_4' sites. These are consistent with the recent theoretical prediction that the Si adatoms are upwardly displaced and the K atoms form a trimer structure in the 2-~(1/2)3 x 2~(1/2)3 unit cell at low temperature [Phys. Rev. Lett. 107, 187603 (2011)], although the flat model where all the Si adatoms have the same height is also acceptable in the rocking curve analyses. However, at room temperature, which is above the surface phase-transition temperature for 2~(1/2)3 x 2 ~(1/2)3 to~(1/2)3 x~(1/2)3, the K atoms are randomly located in the 2~(1/2)3 x 2~(1/2)5 unit cell. This phase transition is accompanied by the disordering of K atoms.
机译:利用反射高能正电子衍射(RHEPD)研究了K / Si(11)-2〜(1/2)3×2〜(1/2)5-B表面的原子坐标和电荷转移。当K吸附到Si(111)-〜(1/2)3×〜(1/2)3-B表面上时,111 Bragg反射的位置移动到一个较小的角度,从而表明发生了变化内部电势是由每K原子1.Oe〜-向表面的电荷转移产生的。根据在113 K处记录的RHEPD摇摆曲线,我们确定顶部K原子和Si原子分别从第一Si层吸附了2.96和2.51A。与对于Si(11)-〜(1/2)3 x〜(1/2)3-B表面发现的硅原子相比,硅原子显着向上移位。此外,我们发现K原子吸附在H_3和T_4'位之间。这些与最近的理论预测一致,即硅吸附原子在低温下会在2-〜(1/2)3 x 2〜(1/2)3晶胞中向上移位并且K原子形成三聚体结构[Phys] 。牧师107,187603(2011)],尽管在摇摆曲线分析中所有硅原子都具有相同高度的平面模型也是可以接受的。但是,在室温下,在2〜(1/2)3 x 2〜(1/2)3至〜(1/2)3 x〜(1/2)3的表面相变温度以上, K原子随机位于2〜(1/2)3 x 2〜(1/2)5晶胞中。该相变伴随有K原子的无序化。

著录项

  • 来源
    《Physical review》 |2012年第3期|p.035423.1-035423.5|共5页
  • 作者单位

    Advanced Science Research Center, Japan Atomic Energy Agency, 1233 Watanuki, Takasaki, Gunma 370-1292, Japan;

    Advanced Science Research Center, Japan Atomic Energy Agency, 1233 Watanuki, Takasaki, Gunma 370-1292, Japan;

    Advanced Science Research Center, Japan Atomic Energy Agency, 1233 Watanuki, Takasaki, Gunma 370-1292, Japan;

  • 收录信息
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    phase transitions and critical phenomena;

    机译:相变和临界现象;

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号