...
首页> 外文期刊>Journal of the Korean Physical Society >Superfluidity in D_2(H_2)_NClusters
【24h】

Superfluidity in D_2(H_2)_NClusters

机译:D_2(H_2)_NClusters中的超流

获取原文
获取原文并翻译 | 示例
           

摘要

The low-temperature properties of small para-112 clusters doped by a single ortho-D_2 moleculeare computed using the path-integral Monte Carlo method. The clusters of D_2(H_2)_NwithN =13and 18 are found to show significant superfluid fractions below 2 K, and the effects due to thepresence of a D_2impurity molecule are quite different between these two cluster sizes. TheN=13cluster has superfluid fractions virtually identical to those of the impurity-free (H_2)_(13)cluster atall temperatures considered here, but the superfluidity for N = 18 is shown to be considerablysuppressed by addition of the impurity molecule. The heavier D_2molecule is also shown to belocated around the cluster center with negligible thermal effects on its density distribution below2 K, which can be understood with the occurrence of Bose condensation manifested by largesuperfluid fractions. While the density distribution of D_2for the case ofN=13 is found to bepeaked at the cluster center, the D_2density peak forN=18 is located slightly off the centerbelow the onset temperature of superfluidity. We conclude that the difference in the effects of theimpurity molecule on the superfluidity between the N 13 and the N = 18 clusters results fromthe recently-discovered magic number behavior of hydrogen clusters
机译:利用路径积分蒙特卡罗方法计算了单个邻位D_2分子掺杂的对位112小簇的低温性质。发现D_2(H_2)_NwithN = 13和18的簇显示出低于2 K的显着超流体分数,并且由于D_2杂质分子的存在所引起的影响在这两个簇大小之间完全不同。在此处考虑的所有温度下,N = 13团簇的超流体分数实际上与无杂质(H_2)_(13)团的超流体分数相同,但是N = 18的超流体表现出通过添加杂质分子而被显着抑制。还显示出较重的D_2分子位于簇中心附近,对其在2 K以下的密度分布可忽略不计的热效应,这可以通过大超流体级分所显示的Bose缩合来理解。虽然发现N = 13的情况下D_2的密度分布处于簇中心,但N = 18的D_2密度峰位于中心点稍稍低于超流的起始温度。我们得出的结论是,杂质分子对N 13和N = 18团簇之间的超流动性影响的差异是由于最近发现的氢团簇的幻数行为造成的

著录项

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