Participation of electronic excited states in the positronium formation mechanism in the Gd(III) pentakis (picrate) complexes with imidazolium countercations

2016 ◽  
Vol 170 ◽  
pp. 491-496 ◽  
Author(s):  
F. Fulgêncio ◽  
A.S. Borges ◽  
M.H. Araújo ◽  
H.F. Brito ◽  
F.C. Oliveira ◽  
...  
2012 ◽  
Vol 733 ◽  
pp. 245-248 ◽  
Author(s):  
Welington F. Magalhães ◽  
Fernando Fulgêncio ◽  
Fernando C. de Oliveira ◽  
Dario Windmöller ◽  
José C. Machado ◽  
...  

Positron annihilation lifetime (PALS) and photoluminescence spectroscopies measurements were performed in Tb(III) and Eu(III) dipivaloylmethanates, Tb(dpm)3and Eu(dpm)3, and also on their binary solid solutions of general formula Tb1-xEux(dpm)3. A correlation between the5D4Tb(III) energy level lifetime and the positronium formation probability was observed, indicating that the ligand-to-metal charge transfer LMCT states act in both luminescence quenching and positronium formation inhibition. From these results, a new model is proposed, showing that excited electronic states have a relevant role in the positronium formation mechanism.


2019 ◽  
Author(s):  
Fernando Fulgêncio ◽  
Rafael Sábio ◽  
Sidney. J. Ribeiro ◽  
Fernando C. Oliveira ◽  
Alex S. Borges ◽  
...  

2018 ◽  
Author(s):  
Juan Sanz García ◽  
Martial Boggio-Pasqua ◽  
Ilaria Ciofini ◽  
Marco Campetella

<div>The ability to locate minima on electronic excited states (ESs) potential energy surfaces (PESs) both in the case of bright and dark states is crucial for a full understanding of photochemical reactions. This task has become a standard practice for small- to medium-sized organic chromophores thanks to the constant developments in the field of computational photochemistry. However, this remains a very challenging effort when it comes to the optimization of ESs of transition metal complexes (TMCs), not only due to the presence of several electronic excited states close in energy, but also due to the complex nature of the excited states involved. In this article, we present a simple yet powerful method to follow an excited state of interest during a structural optimization in the case of TMC, based on the use of a compact hole-particle representation of the electronic transition, namely the natural transition orbitals (NTOs). State tracking using NTOs is unambiguously accomplished by computing the mono-electronic wavefunction overlap between consecutive steps of the optimization. Here, we demonstrate that this simple but robust procedure works not only in the case of the cytosine but also in the case of the ES optimization of a ruthenium-nitrosyl complex which is very problematic with standard approaches.</div>


2014 ◽  
Vol 43 (9-10) ◽  
pp. 1644-1644
Author(s):  
Hitoshi Ozawa ◽  
Kazunori Yashiro ◽  
Takuma Yamamoto ◽  
Satoshi Yabushita

ChemPhysChem ◽  
2005 ◽  
Vol 6 (3) ◽  
pp. 503-510 ◽  
Author(s):  
Begoña Milián ◽  
Rosendo Pou-Amérigo ◽  
Manuela Merchán ◽  
Enrique Ortí

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