hybrid orbital
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2020 ◽  
Vol 16 (9) ◽  
pp. 5601-5620
Author(s):  
Florian Buchholz ◽  
Iris Theophilou ◽  
Klaas J. H. Giesbertz ◽  
Michael Ruggenthaler ◽  
Angel Rubio

2020 ◽  
Vol 14 (01) ◽  
pp. 1 ◽  
Author(s):  
Bereneice Sephton ◽  
Yao-Wei Huang ◽  
Antonio Ambrosio ◽  
Cheng-Wei Qiu ◽  
Adam Vallés ◽  
...  

2019 ◽  
Vol 122 (6) ◽  
pp. 568-572 ◽  
Author(s):  
Radhika A. Jain ◽  
Mahesh Verma ◽  
Rekha Gupta ◽  
Shubhra Gill ◽  
Modhupa Ghosh

2019 ◽  
Vol 15 ◽  
pp. 102790 ◽  
Author(s):  
Zebin Huang ◽  
Peipei Wang ◽  
Junmin Liu ◽  
Wenjie Xiong ◽  
Yanliang He ◽  
...  

2019 ◽  
Vol 33 (10) ◽  
pp. 1950090
Author(s):  
Hai-Long Li ◽  
Liang Bian ◽  
Fa-Qin Dong ◽  
Wei-Min Li ◽  
Hao Zou ◽  
...  

To observe the effect of halogen-substitution on the Mn-O electron transfer of NiMn2O4, we calculated Mn-mixed-valence configuration (charge-disproportionation) and oxygen vacancy by the density functional theory (DFT). The results indicate that the halogen-p5 state induces the O-2p orbital splitting to create an oxygen vacancy in the VB (valence band: about −5 eV). The oxygen vacancy can capture an electron from Mn[Formula: see text]-3d5 orbital that makes the Mn[Formula: see text]-3d5 change to Mn[Formula: see text]-3d4 states (Mn-charge disproportionate), and providing many effective-hole (40.14 [Formula: see text] 96.72 × 10[Formula: see text] kg). The halogen-p5-O-2p4 hybrid orbitals enhance the O-2p4-Mn-3d5 p-d hybrid orbital (about 19.18 electron). That increases the surface potential in Mn-O octahedron (for Cl-substituted: about 60 meV), the corresponding electron–electron interactions change from complex t[Formula: see text] (O-2p4-Mn[Formula: see text]-3d[Formula: see text] to complete [Formula: see text] (O-2p4-Mn[Formula: see text]-3d[Formula: see text]-e[Formula: see text](O-2p4-halogen-p5) orbital. This study effectively analyzes the microscopic changes of the electron transfer caused by the small amount of doping, provides a theoretical basis for the design of NMO-based semiconductor material.


2018 ◽  
Vol 149 (8) ◽  
pp. 084107 ◽  
Author(s):  
Ye Luo ◽  
Kenneth P. Esler ◽  
Paul R. C. Kent ◽  
Luke Shulenburger

2017 ◽  
Vol 95 (12) ◽  
pp. 1314-1322 ◽  
Author(s):  
C.E. Brion ◽  
Saul Wolfe ◽  
Zheng Shi ◽  
Glyn Cooper ◽  
Yenyou Jeff Zheng

Observations of the physical behaviour (motions) of the valence (frontier) electrons in the iconic benchmark hydride molecules CH4, NH3, and H2O are used to provide a direct experimental evaluation of hybridization and of the localized and delocalized orbital models of molecular electronic structure, after more than 80 years since the initial proposals of these theoretical concepts. Our previously published experimental measurements of valence (frontier) electron momentum probability distributions, made by electron momentum spectroscopy (EMS), are compared with those calculated using the localized molecular orbital (LMO) model and a range of hybrid orbital models, as well as with the delocalized canonical molecular orbital (CMO) and density functional theory Kohn–Sham orbital (KSO) models. In all cases, the electron momentum probability distributions calculated with LMOs and localized hybrid orbital type models are inconsistent with the experimental observations. In contrast, those calculated with the delocalized CMOs and KSOs are in very good agreement with the experimental measurements. These findings are of importance in those research applications such as reactivity, drug and novel material design, and also in molecular electronics, where the shapes and orientations of particular valence (frontier) orbital electron density probability distributions (and not the total electron densities) are considered to be key determining factors. These findings and their implications are also of pedagogical significance in chemistry and molecular physics.


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