原子与分子物理学报
原子與分子物理學報
원자여분자물이학보
Journal of Atomic and Molecular Physics
2015年
5期
896-902
,共7页
郑兴荣%付云%付文羽%李向富%李继弘
鄭興榮%付雲%付文羽%李嚮富%李繼弘
정흥영%부운%부문우%리향부%리계홍
固氩%fcc晶格结构%CCSD( T)%三体势%四体势
固氬%fcc晶格結構%CCSD( T)%三體勢%四體勢
고아%fcc정격결구%CCSD( T)%삼체세%사체세
Solid argon%Face-centered cubic crystal structure%CCSD ( T )%Three-body potential%Four-body potential
X射线衍射实验显示固氩是面心立方( fcc)晶格结构,目前对晶体氩的研究只限于两体,三体以及四体相互作用势。本文利用多体展开方法和超分子单、双(三)重激发耦合簇理论(CCSD(T))对固氩fcc晶格结构的三体和四体的几何构型、几何参数、不同体积下所有三体和四体构型的势能以及各构型所占比例等几个方面进行了准确的量子化学计算。结果表明:所有三体构型中对总的三体势能贡献最大的是构型1、构型6、构型12和构型23;三体势及其交换部分和色散部分的计算结果与现有解析经验势在长程部分符合得非常好,但在短程部分有较小差异。所有的四体构形中对总的四体势能贡献最大的是构型1,构型2,构型4,构型5,构型7和构型8;四体势及其交换势部分和色散部分的计算结果尚无解析经验势可比较。利用这些特殊构型的相关数据并结合其它构型,可拟合出更准确的三体经验势函数及其参数,也为拟合四体经验势函数及其参数提供了重要的参考价值。
X射線衍射實驗顯示固氬是麵心立方( fcc)晶格結構,目前對晶體氬的研究隻限于兩體,三體以及四體相互作用勢。本文利用多體展開方法和超分子單、雙(三)重激髮耦閤簇理論(CCSD(T))對固氬fcc晶格結構的三體和四體的幾何構型、幾何參數、不同體積下所有三體和四體構型的勢能以及各構型所佔比例等幾箇方麵進行瞭準確的量子化學計算。結果錶明:所有三體構型中對總的三體勢能貢獻最大的是構型1、構型6、構型12和構型23;三體勢及其交換部分和色散部分的計算結果與現有解析經驗勢在長程部分符閤得非常好,但在短程部分有較小差異。所有的四體構形中對總的四體勢能貢獻最大的是構型1,構型2,構型4,構型5,構型7和構型8;四體勢及其交換勢部分和色散部分的計算結果尚無解析經驗勢可比較。利用這些特殊構型的相關數據併結閤其它構型,可擬閤齣更準確的三體經驗勢函數及其參數,也為擬閤四體經驗勢函數及其參數提供瞭重要的參攷價值。
X사선연사실험현시고아시면심립방( fcc)정격결구,목전대정체아적연구지한우량체,삼체이급사체상호작용세。본문이용다체전개방법화초분자단、쌍(삼)중격발우합족이론(CCSD(T))대고아fcc정격결구적삼체화사체적궤하구형、궤하삼수、불동체적하소유삼체화사체구형적세능이급각구형소점비례등궤개방면진행료준학적양자화학계산。결과표명:소유삼체구형중대총적삼체세능공헌최대적시구형1、구형6、구형12화구형23;삼체세급기교환부분화색산부분적계산결과여현유해석경험세재장정부분부합득비상호,단재단정부분유교소차이。소유적사체구형중대총적사체세능공헌최대적시구형1,구형2,구형4,구형5,구형7화구형8;사체세급기교환세부분화색산부분적계산결과상무해석경험세가비교。이용저사특수구형적상관수거병결합기타구형,가의합출경준학적삼체경험세함수급기삼수,야위의합사체경험세함수급기삼수제공료중요적삼고개치。
X-ray diffraction experiments shows that solid argon is a face-centered cubic crystal structure ( fcc structure). At present, crystal argon is studied involving two-, three- and four-body potentials. Using the many-body expansion method and the double cluster with full single and double excitations plus perturbative treatment of triples ( CCSD( T) ) , the properties of fcc structure for solid argon which include geometrical config-uration, geometrical parameters, potential energy of three- and four-body potentials and the proportion of all configurations at different volumes were accurately calculated. It is concluded that the configuration 1 , 6 , 12 and 23 play most important role in all three-body potential configurations. The calculation results of three-body po-tential, exchange potential and dispersion potential are in good agreement with the analytic experience potential in long-range part, but have small differences in short-range part. The configuration 1, 2, 4, 5, 7 and 8 play very important role in all four-body potential configurations, and there is not analytic experience potential to compare between the calculated results of four-body potential, exchange potential and dispersion potential. U-sing the data of these special configurations in combination with other configurations can fit a more accurate three-body experience potential function and its parameters, and also provide important reference value about fit four-body experience potential function and its parameters.