Study of electronic structure of certain phenazasilines by quantum chemistry and UV spectroscopy methods

1985 ◽  
Vol 21 (2) ◽  
pp. 219-222
Author(s):  
S. G. Semenov ◽  
I. P. Yakovlev ◽  
Yu. S. Finogenov
2005 ◽  
Vol 123 (8) ◽  
pp. 084301 ◽  
Author(s):  
Wutharath Chin ◽  
François Piuzzi ◽  
Jean-Pierre Dognon ◽  
Iliana Dimicoli ◽  
Michel Mons

2015 ◽  
Vol 17 (39) ◽  
pp. 25809-25821 ◽  
Author(s):  
Aude Bouchet ◽  
Johanna Klyne ◽  
Giovanni Piani ◽  
Otto Dopfer ◽  
Anne Zehnacker

The effects of ionisation and protonation on the geometric and electronic structure of a prototypical aromatic amino-alcohol with two chiral centres are revealed by IR and UV spectroscopy.


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 ◽  
...  

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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