Ab Initio Examination of Anomeric Effects in Tetrahydropyrans, 1,3-Dioxanes, and Glucose

1994 ◽  
Vol 59 (8) ◽  
pp. 2138-2155 ◽  
Author(s):  
Ulrike Salzner ◽  
Paul v. R. Schleyer
Keyword(s):  
2007 ◽  
Vol 93 (1) ◽  
pp. 1-10 ◽  
Author(s):  
H. Lee Woodcock ◽  
Damian Moran ◽  
Richard W. Pastor ◽  
Alexander D. MacKerell ◽  
Bernard R. Brooks

2005 ◽  
Vol 340 (13) ◽  
pp. 2171-2184 ◽  
Author(s):  
Rodrigo S. Bitzer ◽  
André G.H. Barbosa ◽  
Clarissa O. da Silva ◽  
Marco A.C. Nascimento

2015 ◽  
Vol 17 (28) ◽  
pp. 18501-18513 ◽  
Author(s):  
Vladimir Sladek ◽  
Filip Holka ◽  
Igor Tvaroška

Oxygen substitution in 2-methoxytetrahydropyran by sulphur in 2-methoxythiane approximately doubles the anomeric effect, which slows down enzymatic processing of 2-methoxythiane.


Author(s):  
Xudong Weng ◽  
O.F. Sankey ◽  
Peter Rez

Single electron band structure techniques have been applied successfully to the interpretation of the near edge structures of metals and other materials. Among various band theories, the linear combination of atomic orbital (LCAO) method is especially simple and interpretable. The commonly used empirical LCAO method is mainly an interpolation method, where the energies and wave functions of atomic orbitals are adjusted in order to fit experimental or more accurately determined electron states. To achieve better accuracy, the size of calculation has to be expanded, for example, to include excited states and more-distant-neighboring atoms. This tends to sacrifice the simplicity and interpretability of the method.In this paper. we adopt an ab initio scheme which incorporates the conceptual advantage of the LCAO method with the accuracy of ab initio pseudopotential calculations. The so called pscudo-atomic-orbitals (PAO's), computed from a free atom within the local-density approximation and the pseudopotential approximation, are used as the basis of expansion, replacing the usually very large set of plane waves in the conventional pseudopotential method. These PAO's however, do not consist of a rigorously complete set of orthonormal states.


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