A new trap mechanism has been proposed to generate H@C 60 . Buckyball excited by shaped laser pulse could have large Raman-active vibration mode A g （1）, which enlarges and shrinks buckyball alternately, and raises ...A new trap mechanism has been proposed to generate H@C 60 . Buckyball excited by shaped laser pulse could have large Raman-active vibration mode A g （1）, which enlarges and shrinks buckyball alternately, and raises and decreases the energy barrier repeatedly, forming a trap to capture the incoming H atom. In this trap mechanism, the A g （1） vibration mode is excited before the encapsulation process of H atom. Simulations of semiclassical electron-radiation-ion dynamics showed that the kinetic energy threshold for H atom in this mechanism was lowered from 17.51 eV to 10.51 eV, and successful encapsulation happened in the range from 10.51 eV to 15.55 eV.展开更多
The geometric and electronic structures of scandium carbonitride endofullerene Sc3CN@C2n （2n=68, 78, 80, 82, and 84） and Sc（Y）NC@C76 have been systematically investigated to identify the preferred position of inte...The geometric and electronic structures of scandium carbonitride endofullerene Sc3CN@C2n （2n=68, 78, 80, 82, and 84） and Sc（Y）NC@C76 have been systematically investigated to identify the preferred position of internal C and N atoms by density functional theory （DFT） calculations combined with statistical mechanics treatments. The CN bond orientation can generally be inferred from the molecule stability and electronic configuration. It is found that Sc3CN@C2n molecules have the most stable structure with C atom locating at the center of Sc3CN cluster. The CN bond has trivalent form of[CN]3- and connects with adjacent three Sc atoms tightly. However, in Sc（Y）NC@C76 with[NC]-, the N atom always resides in the center of the whole molecule. In addition, the stability of Sc3CN@C2n has been further compared in terms of the organization of the corresponding molecular energy level. The structural differences between Sc3CN@C2n and Sc3NC@C2n are highlighted by their respected infrared spectra.展开更多
基金Supported by the Fundamental Research Funds for National Natural Science Foundation of China(11205117)the Scientific Research Foundation for the Returned Overseas Chinese Scholars,State Education Ministry
文摘A new trap mechanism has been proposed to generate H@C 60 . Buckyball excited by shaped laser pulse could have large Raman-active vibration mode A g （1）, which enlarges and shrinks buckyball alternately, and raises and decreases the energy barrier repeatedly, forming a trap to capture the incoming H atom. In this trap mechanism, the A g （1） vibration mode is excited before the encapsulation process of H atom. Simulations of semiclassical electron-radiation-ion dynamics showed that the kinetic energy threshold for H atom in this mechanism was lowered from 17.51 eV to 10.51 eV, and successful encapsulation happened in the range from 10.51 eV to 15.55 eV.
基金Project supported by the National Natural Science Foundation of China(Grant Nos.21503208,61604104,and 51002102)the Natural Science Foundation of Shanxi Province,China(Grant Nos.2015011034,201601D202034,and 201601D202029)the Natural Science Foundation Project of Chongqing Science and Technology Commission,China(Grant No.cstc2014jcyj A00032)
文摘The geometric and electronic structures of scandium carbonitride endofullerene Sc3CN@C2n （2n=68, 78, 80, 82, and 84） and Sc（Y）NC@C76 have been systematically investigated to identify the preferred position of internal C and N atoms by density functional theory （DFT） calculations combined with statistical mechanics treatments. The CN bond orientation can generally be inferred from the molecule stability and electronic configuration. It is found that Sc3CN@C2n molecules have the most stable structure with C atom locating at the center of Sc3CN cluster. The CN bond has trivalent form of[CN]3- and connects with adjacent three Sc atoms tightly. However, in Sc（Y）NC@C76 with[NC]-, the N atom always resides in the center of the whole molecule. In addition, the stability of Sc3CN@C2n has been further compared in terms of the organization of the corresponding molecular energy level. The structural differences between Sc3CN@C2n and Sc3NC@C2n are highlighted by their respected infrared spectra.
