Différences entre les versions de « Abstract pool hdr »

De Workshops
Aller à la navigation Aller à la recherche
(Created page with "<<< Miniworkshop main page =Abstracts= ==John Smith== ''University'' '''<big>Title</big>''' Text [1] Popelier, P. L. A.; Brémond, É. A. G. Int.J.Quant.Che...")
 
Ligne 3 : Ligne 3 :
  
 
=Abstracts=
 
=Abstracts=
==John Smith==
+
==Example: John Smith==
 
''University''
 
''University''
  
Ligne 17 : Ligne 17 :
  
 
[http://wiki.lct.jussieu.fr/workshop/index.php/Abstract_pool_hdr ↑ top of this page]
 
[http://wiki.lct.jussieu.fr/workshop/index.php/Abstract_pool_hdr ↑ top of this page]
 +
 +
 +
=Aurélien de la Lande=
 +
 +
''Laboratoire de Chimie Physique, Université Paris Sud, CNRS, Université Paris Saclay. 15, avenue Jean Perrin, 91405 Orsay, Cedex. France""
 +
 +
'''<big>Robust, basis-set independent method for the evaluation of charge-transfer energy in nonconvalent complexes</big>'''
 +
 +
 +
Separation of the energetic contribution of charge transfer to interaction energy in noncovalent complexes would provide important insight into the mechanisms of the interaction. However, the calculation of charge-transfer energy is not an easy task. It is not a physically well-defined term and the results might depend on how it is described in practice. Commonly, the charge transfer is defined in terms of molecular orbitals; in this framework, however, the charge transfer vanishes as the basis set size increases towards the complete basis set limit. This can be avoided by defining the charge transfer in terms of the spatial extent of the electron densities of the interacting molecules, but the schemes used so far do not reflect the actual electronic structure of each particular system and thus are not reliable. We propose a novel approach – spatial partitioning of the system which is based on a charge transfer-free reference state, namely superimposition of electron densities of the non-interacting fragments. We show that this method, employing constrained DFT for the calculation of the charge-transfer energy, yields reliable results and is robust with respect to the strength of the charge transfer, the basis set size and the DFT functional used. Because it is based on DFT, the method is applicable to rather large systems.
 +
 +
[1] Řezáč, J; de la Lande, A. J. Chem. Theor. Comput. 2015, 11, 528-537.

Version du 30 septembre 2015 à 14:03

<<< Miniworkshop main page


Abstracts

Example: John Smith

University


Title

Text


[1] Popelier, P. L. A.; Brémond, É. A. G. Int.J.Quant.Chem. 2009, 109, 2542.


↑ top of this page


Aurélien de la Lande

Laboratoire de Chimie Physique, Université Paris Sud, CNRS, Université Paris Saclay. 15, avenue Jean Perrin, 91405 Orsay, Cedex. France""

Robust, basis-set independent method for the evaluation of charge-transfer energy in nonconvalent complexes


Separation of the energetic contribution of charge transfer to interaction energy in noncovalent complexes would provide important insight into the mechanisms of the interaction. However, the calculation of charge-transfer energy is not an easy task. It is not a physically well-defined term and the results might depend on how it is described in practice. Commonly, the charge transfer is defined in terms of molecular orbitals; in this framework, however, the charge transfer vanishes as the basis set size increases towards the complete basis set limit. This can be avoided by defining the charge transfer in terms of the spatial extent of the electron densities of the interacting molecules, but the schemes used so far do not reflect the actual electronic structure of each particular system and thus are not reliable. We propose a novel approach – spatial partitioning of the system which is based on a charge transfer-free reference state, namely superimposition of electron densities of the non-interacting fragments. We show that this method, employing constrained DFT for the calculation of the charge-transfer energy, yields reliable results and is robust with respect to the strength of the charge transfer, the basis set size and the DFT functional used. Because it is based on DFT, the method is applicable to rather large systems.

[1] Řezáč, J; de la Lande, A. J. Chem. Theor. Comput. 2015, 11, 528-537.