Abstract:For novel all-metal electride, multicage chain structures [(Ni@ Ge 9 ) Ca 3 ] n (n = 1−4) with all real frequencies are obtained theoretically for the first time. In the structure of n = 1, the Ni@Ge 9 metal cage as the shortest chain skeleton is surrounded by nonbridge Ca atoms. In the structures of n = 2−4, Ni@Ge 9 metal cages are connected by bridge Ca atom pair(s) forming new hybrid multicage chain skeletons surrounded by nonbridge Ca atoms. And interesting pull−push electron relay occurs. The chain skelet… Show more
“…The VIP correlates with the size of the spherical lobe rounding Mg in HOMO, which is associated to the dispersion of excess electron density. The VIP values of these molecules are slightly larger than the reported values of inorganic, organic and other all-metal electride molecules,15,24,30,31,56 but smaller than the very larger value (7.78 eV) of the electride molecule with the excess electron protected inside the C 36 F 36 cage.…”
contrasting
confidence: 60%
“…30 Moreover, we also constructed one-dimensional all-metal electride chains [(Ni@Ge 9 )Ca 3 ] n (1, 2, 3, and 4) and explored their structures and electric properties. 31 In this all-metal electride multicage chain series, increases strongly from 9321 (n = 1, N e = 2) to 54232 au (n = N e = 4),…”
“…The VIP correlates with the size of the spherical lobe rounding Mg in HOMO, which is associated to the dispersion of excess electron density. The VIP values of these molecules are slightly larger than the reported values of inorganic, organic and other all-metal electride molecules,15,24,30,31,56 but smaller than the very larger value (7.78 eV) of the electride molecule with the excess electron protected inside the C 36 F 36 cage.…”
contrasting
confidence: 60%
“…30 Moreover, we also constructed one-dimensional all-metal electride chains [(Ni@Ge 9 )Ca 3 ] n (1, 2, 3, and 4) and explored their structures and electric properties. 31 In this all-metal electride multicage chain series, increases strongly from 9321 (n = 1, N e = 2) to 54232 au (n = N e = 4),…”
“…14 The excess electron system is well-known for triggering second and third-order nonlinearity. 15,16 In the family of excess electron compounds, electride, 17 alkalides, 18 and alkalineearthides 19,20 are well known.…”
Herein, the geometric, electronic, and nonlinear optical properties of excess electron zintl clusters Ge5AM3, Ge9AM5, and Ge10AM3 (AM = Li, Na, and K) are investigated.
“…Other useful strategies have been made to consider different species with varying shapes, sizes, a number of coordination sites, number of excess electrons along with their different spin states to optimize the magnitude of first‐hyperpolarizability. However, first‐hyperpolarizability of diffuse electron compounds has been studied widely than the second‐hyperpolarizability.…”
A number of imido‐, amido‐, and phosphido‐bridged dialkaline earth metal (M = Be, Mg, and Ca) complexes and their alkali metal (Li and Na) derivatives have been considered to study the ground state structure and the second‐hyperpolarizability. The calculated ground state geometries contain four‐membered MN(P)MN(P) ring having either planar or butterfly‐like bent structure. The second‐hyperpolarizability has been calculated at the HF and CCSD(T) levels using Sadlej's pol and aug‐pc‐2 basis sets, respectively. The addition of second hydrogen/alkali metal atom on nitrogen/phosphorus (N/P) atom substantially reduces the charge transfer from the alkaline earth metal atoms as the high negative charge on N/P exerts stronger push effect on the outermost electron pair in the “ns” sub‐shell of M. The excess electron density on the alkaline earth metal atoms plays a crucial role in the enhancement of second‐hyperpolarizability. The sum‐over‐state method calculated two‐photon contribution of second‐hyperpolarizability has been found to be significant. The variation of second‐hyperpolarizability has been explained satisfactorily in terms of the TD‐CAMB3LYP calculated spectroscopic properties in the light of two‐state model. The calculated mean second‐hyperpolarizabilities of alkali substituted amido‐ and phosphido‐bridged complexes are in the order of 107 au.
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