scholarly journals A Frontier orbital energy approach to redox potentials

2015 ◽  
Vol 633 ◽  
pp. 012045 ◽  
Author(s):  
Jeanet Conradie
2013 ◽  
Vol 49 (85) ◽  
pp. 9938 ◽  
Author(s):  
Elena Zaborova ◽  
Patricia Chávez ◽  
Rony Bechara ◽  
Patrick Lévêque ◽  
Thomas Heiser ◽  
...  

2019 ◽  
Vol 31 (17) ◽  
pp. 6808-6817 ◽  
Author(s):  
Saeed-Uz-Zaman Khan ◽  
Giacomo Londi ◽  
Xiao Liu ◽  
Michael A. Fusella ◽  
Gabriele D’Avino ◽  
...  

Polymer ◽  
2014 ◽  
Vol 55 (9) ◽  
pp. 2139-2145 ◽  
Author(s):  
Tomoyuki Ikai ◽  
Tomoya Kudo ◽  
Masahiro Nagaki ◽  
Tomoyuki Yamamoto ◽  
Katsuhiro Maeda ◽  
...  

2015 ◽  
Vol 3 (34) ◽  
pp. 17738-17746 ◽  
Author(s):  
Christopher Steck ◽  
Marius Franckevičius ◽  
Shaik Mohammed Zakeeruddin ◽  
Amaresh Mishra ◽  
Peter Bäuerle ◽  
...  

Heteropentacene-based A–D–A type hole transport materials with suitable frontier orbital energy levels were synthesized and used in perovskite solar cells showing power conversion efficiencies up to 11.4%.


2020 ◽  
Vol 12 (46) ◽  
pp. 51374-51386
Author(s):  
Xintong Li ◽  
Xiaoqi Han ◽  
Huanrui Zhang ◽  
Rongxiang Hu ◽  
Xiaofan Du ◽  
...  

2020 ◽  
Author(s):  
Ekadashi Pradhan ◽  
Tao Zeng

<p>We used quantum chemistry methods at the levels of mixed-reference spin-flipping time-dependent density functional theory and multireference perturbation theory to study diboron- and diaza-doped anthracenes and phenanthrenes. This class of structures recently surged as potential singlet fission chromophores. We studied electronic structures of their excited states and clarify the reasons why they satisfy or fail to satisfy the energy criteria for singlet fission chromophores. Many studied structures have their S<sub>1</sub> states not dominated by HOMO->LUMO excitation, so that they cannot be described using the conventional two sites model. This is attributed to frontier orbital energy shifts induced by the doping and different charge transfer energies in different one-electron singlet excitations, or in other words different polarizations of hole and/or particle orbitals in their S<sub>1</sub> and T<sub>1</sub> states. There is a mirror relation between the orbital energy shifts induced by diboron- and diaza-dopings, which, together with alternant hydrocarbon pairings of occupied and unoccupied orbitals, leads to more mirror relations between the excited states' electronic structures of the two types of doped structures. </p>


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