scholarly journals Designing M-bond (X-M···Y, M = transition metal): σ-hole and radial density distribution

2019 ◽  
Vol 131 (12) ◽  
Author(s):  
Jyothish Joy ◽  
Eluvathingal D Jemmis
1970 ◽  
Vol 29 (5) ◽  
pp. 1397-1397 ◽  
Author(s):  
Takeshi Takashima ◽  
Hiroshi Sato ◽  
Michio Matsumoto ◽  
Yoshiei Nakano

2014 ◽  
Vol 11 (4) ◽  
pp. 1455-1458
Author(s):  
Baghdad Science Journal

Radial density distribution function of one particle D(r1) was calculated for main orbital of carbon atom and carbon like ions (N+ and B- ) by using the Partitioning technique .The results presented for K and L shells for the Carbon atom and negative ion of Boron and positive ion for nitrogen ion . We observed that as atomic number increases the probability of existence of electrons near the nucleus increases and the maximum of the location r1 decreases. In this research the Hartree-fock wavefunctions have been computed using Mathcad computer software .


2015 ◽  
Vol 189 (3) ◽  
pp. 312-317 ◽  
Author(s):  
Akihiro Ishimi ◽  
Kozo Katsuyama ◽  
Hirofumi Nakamura ◽  
Takeo Asaga ◽  
Hirotaka Furuya

2020 ◽  
Vol 492 (3) ◽  
pp. 4112-4119 ◽  
Author(s):  
Xu-Dong Zhang ◽  
Sheng-Bang Qian ◽  
Wen-Ping Liao

ABSTRACT Secondary components of W UMa-type contact binaries (CBs) have many special properties, two of them are excess in radius and luminosity. In order to make these specialties clear, we propose radial density distribution to roughly detect the interior structure of the secondaries in CBs. By comparing the radial density distribution between secondary components of CBs and main-sequence stars, we find the radial density distribution of secondaries in A-subtype CBs are similar to main-sequence stars whose masses higher than 1.8 Msun, which suggests that these two kinds of stars may have some evolutionary relationship. While secondary components of W-subtype CBs are closely connected with stars whose masses lower than 1.8 Msun. Then, we investigate the mass–luminosity relation of secondaries in CBs, the big differences between two subtypes suggests that the overluminosity of secondaries in these two subtypes are caused by two different reasons. Overluminosity in A-subtype is because the secondary components are evolved from initial more massive stars, while in W-subtype is due to energy transfer.


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