Prediction of the Equilibrium Structures and Photomagnetic Properties of the Prussian Blue Analogue RbMn[Fe(CN)6] by Density Functional Theory

2008 ◽  
Vol 112 (25) ◽  
pp. 5742-5748 ◽  
Author(s):  
Javier Luzon ◽  
Miguel Castro ◽  
Esther J. M. Vertelman ◽  
Régis Y. N. Gengler ◽  
Petra J. van Koningsbruggen ◽  
...  
2019 ◽  
Vol 55 (50) ◽  
pp. 7151-7154 ◽  
Author(s):  
Chunxiao Zhao ◽  
Biao Liu ◽  
Xuning Li ◽  
Kaixin Zhu ◽  
Ruisheng Hu ◽  
...  

We, for the first time, demonstrated using experiments and density functional theory (DFT) calculations that high-spin CoII exhibits excellent Fenton-like activity.


2008 ◽  
Vol 2008 ◽  
pp. 1-4 ◽  
Author(s):  
D. Rodríguez ◽  
D. Soto ◽  
E. Ramírez ◽  
A. Cruz ◽  
A. Santana ◽  
...  

Using hybrid density functional theory and a relatively large basis set, the lowest energy equilibrium structure, vibrational spectrum, and natural orbital analysis were obtained for magnesium diboride clusters [(MgB2)x for x=1,2, and 3]. For comparison, boron clusters [Bx for x=2,4, and 6] were also considered. The MgB2 and (MgB2)2 showed equilibrium structures with the boron atoms in arrangements similar to what was obtained for pure boron atoms, whereas, for (MgB2)3 a different arrangement of boron was obtained. From the population analysis, large electron density in the boron atoms forming the clusters was observed.


2016 ◽  
Vol 18 (4) ◽  
pp. 2887-2895 ◽  
Author(s):  
Thomas Dumas ◽  
Dominique Guillaumont ◽  
Clara Fillaux ◽  
Andreas Scheinost ◽  
Philippe Moisy ◽  
...  

Multi-edge soft X-ray absorption spectroscopy is used to probe orbital mixing in actinide and lanthanide Prussian blue analogs.


1998 ◽  
Vol 53 (3) ◽  
pp. 381-385 ◽  
Author(s):  
Arne Haaland ◽  
Dimitry J. Shorokhov ◽  
Hans Vidar Volden ◽  
Hans Joachim Breunig ◽  
Michael Denker ◽  
...  

Density functional theory calculations on E(SbMe2)2, E = S or Te, Me = CH3, indicate that the equilibrium structures are syn-syn or near syn-syn conformers with overall C2v or C2 symmetry. The calculations further indicate the existence of syn-anti conformers about 4 kJ mol-1 (E = S) or 1 kJ m ol-1 (E = Te) above the equilibrium structure. G as electron diffraction data show that both conform ers are present in gaseous S(SbMe2)2, while the presence of the syn-anti conformer in gaseous Te(SbMe2)2 is uncertain. The Sb - S and Sb - Te bond distances are 241.4(4) and 278.1(3) pm, respectively, the valence angles of the synsyn conformers are <SbSSb = 9 8.7(5)° and <SbTeSb = 91(2)°.


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