Rabbit ears concepts of water lone pairs: a reply to comments of Hiberty, Danovich, and Shaik

2015 ◽  
Vol 16 (3) ◽  
pp. 694-696 ◽  
Author(s):  
A. D. Clauss ◽  
M. Ayoub ◽  
J. W. Moore ◽  
C. R. Landis ◽  
F. Weinhold
Keyword(s):  

We respond to recent comments (Hibertyet al., 2015) on our earlier article (Clausset al., 2014) concerning “rabbit ears” depictions of lone pair orbitals in water and other species.

2019 ◽  
Author(s):  
Yu Liu ◽  
Terry J. Frankcombe ◽  
Timothy Schmidt

<div>The electronic structure of water is typically thought of exhibiting lone-pairs of electrons, described by some as "rabbit-ears'". This is not the universal view, and does not mesh with an interpretation based on the one-electron wavefunctions which emerge from molecular orbital theory. Here we show, by analysing the antisymmetrized wavefunction (Slater determinant) rather than the Hartree product, that the water wavefunction indeed exhibits equivalent lone pairs. The observed photoelectron spectrum is reconciled with this view in terms of a relaxation of this structure upon the loss of an electron. It is therefore shown that the lone-pair viewpoint is completely consistent with both the experimental results and the calculated wavefunction.<br></div>


2019 ◽  
Author(s):  
Yu Liu ◽  
Terry J. Frankcombe ◽  
Timothy Schmidt

<div>The electronic structure of water is typically thought of exhibiting lone-pairs of electrons, described by some as "rabbit-ears'". This is not the universal view, and does not mesh with an interpretation based on the one-electron wavefunctions which emerge from molecular orbital theory. Here we show, by analysing the antisymmetrized wavefunction (Slater determinant) rather than the Hartree product, that the water wavefunction indeed exhibits equivalent lone pairs. The observed photoelectron spectrum is reconciled with this view in terms of a relaxation of this structure upon the loss of an electron. It is therefore shown that the lone-pair viewpoint is completely consistent with both the experimental results and the calculated wavefunction.<br></div>


RSC Advances ◽  
2015 ◽  
Vol 5 (97) ◽  
pp. 79882-79887 ◽  
Author(s):  
Danni Li ◽  
Qun Jing ◽  
Chen Lei ◽  
Shilie Pan ◽  
Bingbing Zhang ◽  
...  

Metal lone pairs play an important role in determining the SHG enhancement and bandgap red shift.


1993 ◽  
Vol 71 (8) ◽  
pp. 1123-1127 ◽  
Author(s):  
Peter Politzer ◽  
M. Edward Grice ◽  
Jane S. Murray ◽  
Jorge M. Seminario

Ab initio computational studies have been carried out for three molecules that are commonly classed as antiaromatic: cyclobutadiene (1), 1,3-diazacyclobutadiene (7), and 1,4-dihydropyrazine (6). Their dinitro and diamino derivatives were also investigated. Stabilizing or destabilizing energetic effects were quantified by means of the isodesmic reaction procedure at the MP2/6-31G*//HF/3-21G level, and calculated molecular electrostatic potentials (HF/STO-5G//HF/3-21G) were used as a probe of electron delocalization. Our results do not show extensive delocalization in the π systems of any one of the three parent molecules. The destabilization found for 1 and 7 is attributed primarily to strain and to repulsion between the localized π electrons in the C=C and C=N bonds, respectively. However, 6 is significantly stabilized, presumably due to limited delocalization of the nitrogen lone pairs. NH2 groups are highly stabilizing, apparently because of lone pair delocalization. NO2 is neither uniformly stabilizing nor destabilizing.


IUCrJ ◽  
2020 ◽  
Vol 7 (3) ◽  
pp. 480-489 ◽  
Author(s):  
Kasper Tolborg ◽  
Carlo Gatti ◽  
Bo B. Iversen

In chemistry, stereochemically active lone pairs are typically described as an important non-bonding effect, and recent interest has centred on understanding the derived effect of lone pair expression on physical properties such as thermal conductivity. To manipulate such properties, it is essential to understand the conditions that lead to lone pair expression and provide a quantitative chemical description of their identity to allow comparison between systems. Here, density functional theory calculations are used first to establish the presence of stereochemically active lone pairs on antimony in the archetypical chalcogenide MnSb2O4. The lone pairs are formed through a similar mechanism to those in binary post-transition metal compounds in an oxidation state of two less than their main group number [e.g. Pb(II) and Sb(III)], where the degree of orbital interaction (covalency) determines the expression of the lone pair. In MnSb2O4 the Sb lone pairs interact through a void space in the crystal structure, and their their mutual repulsion is minimized by introducing a deflection angle. This angle increases significantly with decreasing Sb—Sb distance introduced by simulating high pressure, thus showing the highly destabilizing nature of the lone pair interactions. Analysis of the chemical bonding in MnSb2O4 shows that it is dominated by polar covalent interactions with significant contributions both from charge accumulation in the bonding regions and from charge transfer. A database search of related ternary chalcogenide structures shows that, for structures with a lone pair (SbX 3 units), the degree of lone pair expression is largely determined by whether the antimony–chalcogen units are connected or not, suggesting a cooperative effect. Isolated SbX 3 units have larger X—Sb—X bond angles and therefore weaker lone pair expression than connected units. Since increased lone pair expression is equivalent to an increased orbital interaction (covalent bonding), which typically leads to increased heat conduction, this can explain the previously established correlation between larger bond angles and lower thermal conductivity. Thus, it appears that for these chalcogenides, lone pair expression and thermal conductivity may be related through the degree of covalency of the system.


2019 ◽  
Vol 7 (35) ◽  
pp. 20223-20228 ◽  
Author(s):  
Dandan Wu ◽  
Shaonian Hu ◽  
Hongyun Xue ◽  
Xiaojuan Hou ◽  
Haiwei Du ◽  
...  

Graphitic carbon nitride (g-C3N4) with pronounced excitation of lone pairs enhances its photocatalytic hydrogen (H2) generation activity.


1998 ◽  
Vol 547 ◽  
Author(s):  
Thomas F. Fässler

AbstractThe phases K6Sn23Bi2, K6Sn25, NaSn5, BaSn3, BaSn5, and K5Pb24 depict the structural transition from Zintl phases with localized chemical bonds to typical intermetallic compounds which may even have superconducting properties. The question of the nature of the chemical bond in these compounds is studied with the help of quantum mechanical calculations. Tight binding band structure calculations and real space representations using the Electron Localization Function (ELF) show that free electron pairs play a crucial role for the description of the chemical bond in polar intermetallic compounds. Interactions between lone pairs have a dominant influence on the electronic structures. The coincident appearance of quasi-molecular localized states in form of lone pairs and disperse delocalized bands at the Fermi level EF is discussed with respect to a ‘chemical view’ of the superconductivity observed for BaSn3, BaSn5, and K5Pb24.


1965 ◽  
Vol 18 (3) ◽  
pp. 261 ◽  
Author(s):  
MG Krishna ◽  
K Ramaswamy ◽  
R Pichai

An attempt has been made to modify the UBFF for chlorine trifluoride by taking into account the presence of lone pairs of electrons, on the lines suggested by Pariseau, Wu, and Overend. It was found that the lone-pair-bond-pair interaction is less than the lone-pair-lone-pair interaction which is considerably lower than the stretching force constant for the lone pair of electrons. An approximate relation between the above interactions was obtained.


1981 ◽  
Vol 34 (12) ◽  
pp. 2569 ◽  
Author(s):  
LW Deady

The relative rates of N-alkylation of 1,1'-dimethyl-2,2'-biimidazole (6), 5,6-dihydrodiimidazo- [1,2-a:2',1'-c]pyrazine (7) and 6,7-dihydro-5H-diimidazo[l,2-a:2',1'-c][l,4]diazepine (8) with a variety of alkylating agents are reported. Irrespective of the alkylating agent, the order of reactivity was (8) (where the biimidazole has an additional three-carbon bridge) > (7) (two-carbon bridge) > (6) (no bridge), with a maximum of (8)/(6) = 317 for reaction with chloro(methoxy)methane. Since reaction of (8) is most susceptible to steric hindrance, but where the nitrogen lone pairs are in close proximity, these results support the idea of lone-pair cooperativity in the alkylation reactions. Variation in the rate ratios with changes in alkylating agent are discussed.


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