AB-INITIO STUDY OF THE STRUCTURE OF Pd(110)-c(4×2)-BENZENE

1999 ◽  
Vol 06 (05) ◽  
pp. 903-906
Author(s):  
FABIO FAVOT ◽  
ANDREA DAL CORSO ◽  
ALFONSO BALDERESCHI

From first principle calculations we have determined the structure of the Pd(110)-c(4×2)-benzene system for three azimuthally different orientations of the benzene molecule (two with C2v and one with C2 symmetry). For all cases, in the relaxed structure the benzene molecule loses its planar geometry since the C–H bonds appreciably bend upwards, the carbon hexagon loses planar geometry too and exhibits inequivalent C–C bond lengths, and the substrate is slightly buckled. We discuss the calculated geometries in terms of benzene–substrate interactions and predict a C2 symmetry of the adsorbed molecule.

2020 ◽  
Vol 34 (30) ◽  
pp. 2050285
Author(s):  
G. S. Orudzhev ◽  
V. N. Jafarova ◽  
S. S. Huseynova ◽  
E. K. Gasimova

This paper presents the results of first-principle calculations of the magnetic properties of vanadium-doped and a vacancy-defected chalcopyrite semiconductor ZnSnAs2. It was shown that adding a transition element contributes to the magnetization of ZnSnAs2. The calculations for a number of supercells showed that a ferromagnetic spin ordering is favorable when V substitutes Sn. Besides, the Zn, Sn and As vacancies affect the magnetization. While V(Sn) substitution of the vacancies strengthens magnetization, a slight weakening of the magnetization occurs due to the arsenic atoms. Four As atoms chemically bonded to V dopant were found to be most contributive.


RSC Advances ◽  
2015 ◽  
Vol 5 (122) ◽  
pp. 101162-101168 ◽  
Author(s):  
M. C. Righi ◽  
S. Loehlé ◽  
M. I. de Barros Bouchet ◽  
D. Philippon ◽  
J. M. Martin

The reaction of trimethyl-phosphite, TMPi, with a clean Fe(110) surface has been investigated by ab initio calculations.


1993 ◽  
Vol 71 (9) ◽  
pp. 1495-1523 ◽  
Author(s):  
Osvald Knop ◽  
T. Stanley Cameron ◽  
Pradip K. Bakshi ◽  
Witold Kwiatkowski ◽  
S.C. Choi ◽  
...  

Recrystallization of a primary or secondary alkylammonium tetraphenylborate (TB) from approximately 1:1 mixtures of Me2CO (or MeEtCO) and water yields, against expectation, the TB of the corresponding iminium cation and thus provides an easy route to a variety of aliphatic Schiff bases. The crystal structures of five such salts have been determined: A, [Me2C = NHMe]BPh4 (Cmcm, a = 10.747(2) Å, b = 15.641(4) Å, c = 13.453(4) Å, Z = 4); B, [Me2,C = NMe2,]BPh4 (Cmca, a = 13.196(4) Å, b = 14.469(3) Å, c = 25.122(4) Å. Z = 8); C, [Me,C = NHEt]BPh4 (P21/n, a = 12.146(3) Å, b = 14.099(2) Å, c = 14.177(3) Å, β = 96.23(2)°, Z = 4); D, [MeEtC=NHMe]BPh4 (Cmc21, a = 10.967(5) Å, b = 15.642(5) Å, c = 13.430(4) Å, Z = 4); E, [Me2C=NH(β-CH2CH2Ph)]BPh4 H2O (C2/c, a = 30.747 Å, b = 9.845(4) Å, c = 19.741(5) Å, β = 97.12(2)°, Z = 8). The building principles of these and related TBs are discussed in detail, as also is the tendency of the small iminium ions to orientational disorder. The range of the C=N bond length in these and other iminium salts is quite narrow, with 1.283(12) Å as the mean (uncorrected) value. Where a hydrogen atom(s) is attached to the iminium nitrogen, it will form a hydrogen bond (simple or bifurcated) with the aromatic π system of the nearest phenyl ring(s). The narrowness of the C=N bond-length range with respect to substitution on the cation has prompted a detailed 6-31G* ab initio study of the effect, on the geometry of the [H2C=NH2]+ ion, of a partial or complete replacement of the H atoms by one of the following substituents: F, Cl, CN, Li, and Na. The 46 structures optimized in planar geometry were supplemented by a number of optimizations of similarly substituted ethylenes as well as by a few optimizations in perpendicular geometry. Analysis of the numerical results involves the bond lengths and angles, Mulliken εM and (in part) Löwdin εL net charges on the atoms, and electron densities ρc = ρ(rc) at the bond critical points. Only a limited use has been made of comparisons involving the total electronic energies E (substitutional isomerism). Since the above substituents span the entire electronegativity scale, and CN provides for the possibility of conjugation, the effects they produce are expected to bracket the effects that would be produced by any other substituents. The calculations confirm the essential narrowness of the C=N bond-length range in iminium ions. They also show that, at least in the 6-31G* scheme, the nitrogen in [H2C=NH2]+ carries a significant negative net charge (both in terms of εM and εL), which is contrary to the conventional representation of the ion as H2C=N+H2. The trends observed in the parameters are smooth and highly self-consistent except for the tri- and tetrasubstituted ions containing Li or Na, where interligand repulsions may invalidate the assumption of planarity. Many of the parameters can be represented to a high degree of correlation as linear functions α0 + αCnC(X) + αNnN(X) of the numbers n of substituent atoms X on the C and N atoms. This representation makes it possible to estimate the contribution to the parameter value from the substitution at the distant atom of the C=N bond, i.e., the extent of localization of the effect produced by the substituent. The success of the linearization of the parameter variation raises the important question of whether the apparent additivity is genuine and intrinsic or merely a property of the 6-31G* optimization scheme. In other words, will additivity be retained, functionally, for sets of parameters obtained from higher level ab initio calculations, and will it be eventually verified by experiment?


2016 ◽  
Vol 18 (27) ◽  
pp. 18074-18080 ◽  
Author(s):  
Shuli Wei ◽  
Da Li ◽  
Yunzhou Lv ◽  
Zhao Liu ◽  
Chunhong Xu ◽  
...  

Using first-principle methods, ground-state TaB3 with the monoclinic C2/m space group and high-pressure TaB4 with the orthorhombic Amm2 space group have been found.


2019 ◽  
Vol 1163 ◽  
pp. 112508 ◽  
Author(s):  
Tymofii Yu. Nikolaienko ◽  
Valerii S. Chuiko ◽  
Leonid A. Bulavin

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