Quantum chemistry investigation of electronic structure and NMR spectral characteristics for fluorides of dialkylamidosulfoxylic acids and related compounds

2009 ◽  
Vol 47 (9) ◽  
pp. 791-800
Author(s):  
A. B. Rozhenko ◽  
W. W. Schoeller ◽  
V. N. Kozel ◽  
V. E. Pashinnik ◽  
Yu. G. Shermolovich
1972 ◽  
Vol 56 (2) ◽  
pp. 1017-1017
Author(s):  
D. C. Grenoble ◽  
C. W. Frank ◽  
C. B. Bargeron ◽  
H. G. Drickamer

1993 ◽  
Vol 59 (1) ◽  
pp. 29-35 ◽  
Author(s):  
Yoichi Yamaguchi ◽  
Jun Shioya

2017 ◽  
Vol 8 (9) ◽  
pp. 6141-6148 ◽  
Author(s):  
Reece Beekmeyer ◽  
Michael A. Parkes ◽  
Luke Ridgwell ◽  
Jamie W. Riley ◽  
Jiawen Chen ◽  
...  

Anion photoelectron spectroscopy and quantum chemistry calculations are employed to probe the electronic structure and dynamics of a unidirectional molecular rotary motor anion in the gas-phase.


2010 ◽  
Vol 12 (42) ◽  
pp. 14253 ◽  
Author(s):  
Clara Fillaux ◽  
Dominique Guillaumont ◽  
Jean-Claude Berthet ◽  
Roy Copping ◽  
David K. Shuh ◽  
...  

2003 ◽  
Vol 58 (4) ◽  
pp. 217-219
Author(s):  
Igor Novak ◽  
Branka Kovač

The electronic structure of 2,7-dimethyl-5-silaspiro[4,4]nona-2,7-diene has been investigated by UV photoelectron spectroscopy (UPS). The analysis of the spectra has been performed by DFT and ROVGF calculations and comparison with the UPS spectra of related compounds. An unusual π-orbital degeneracy in this molecule of C2-symmetry was observed. The spiroconjugation is quenched, and the reasons are discussed.


2019 ◽  
Vol 5 (1) ◽  
Author(s):  
Ryan Babbush ◽  
Dominic W. Berry ◽  
Jarrod R. McClean ◽  
Hartmut Neven

Abstract We present a quantum algorithm for simulating quantum chemistry with gate complexity $$\tilde {\cal{O}}(N^{1/3}\eta ^{8/3})$$ O ̃ ( N 1 ∕ 3 η 8 ∕ 3 ) where η is the number of electrons and N is the number of plane wave orbitals. In comparison, the most efficient prior algorithms for simulating electronic structure using plane waves (which are at least as efficient as algorithms using any other basis) have complexity $$\tilde {\cal{O}}(N^{8/3}{\mathrm{/}}\eta ^{2/3})$$ O ̃ ( N 8 ∕ 3 ∕ η 2 ∕ 3 ) . We achieve our scaling in first quantization by performing simulation in the rotating frame of the kinetic operator using interaction picture techniques. Our algorithm is far more efficient than all prior approaches when N ≫ η, as is needed to suppress discretization error when representing molecules in the plane wave basis, or when simulating without the Born-Oppenheimer approximation.


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