reactive flux
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2021 ◽  
Vol 201 ◽  
pp. 113978
Author(s):  
C.W. Reese ◽  
A. Gladstein ◽  
P. Shevchenko ◽  
X. Xiao ◽  
A.J. Shahani ◽  
...  

2021 ◽  
Vol 60 (6) ◽  
pp. 3502-3513
Author(s):  
Daniel G. Chica ◽  
Abishek K. Iyer ◽  
Matthew Cheng ◽  
Kevin M. Ryan ◽  
Patrick Krantz ◽  
...  

2020 ◽  
Vol 22 (31) ◽  
pp. 17532-17539 ◽  
Author(s):  
Oihana Galparsoro ◽  
Sven Kaufmann ◽  
Daniel J. Auerbach ◽  
Alexander Kandratsenka ◽  
Alec M. Wodtke

We present first principles calculations of the reactive flux for thermal recombinative desorption of hydrogen from Cu(111).


2019 ◽  
Vol 19 (10) ◽  
pp. 5720-5728
Author(s):  
Tetsuya Yamada ◽  
Yuto Kamiya ◽  
Noriyuki Naruse ◽  
Nobuyuki Zettsu ◽  
Katsuya Teshima

2019 ◽  
Vol 75 (7) ◽  
pp. 1041-1045
Author(s):  
Lotfi Rghioui ◽  
Lahcen El Ammari ◽  
Abderrazzak Assani ◽  
Mohamed Saadi

The crystal structures of dirubidium potassium dysprosium bis(vanadate), Rb2KDy(VO4)2, and caesium potassium gadolinium bis(vanadate), Cs1.52K1.48Gd(VO4)2, were solved from single-crystal X-ray diffraction data. Both compounds, synthesized by the reactive flux method, crystallize in the space group P\overline{3}m1 with the glaserite structure type. VO4 tetrahedra are linked to DyO6 or GdO6 octahedra by common vertices to form sheets stacking along the c axis. The large twelve-coordinate Cs+ or Rb+ cations are sandwiched between these layers in tunnels along the a and b axes, while the K+ cations, surrounded by ten oxygen atoms, are localized in cavities.


2019 ◽  
Vol 21 (45) ◽  
pp. 25389-25396
Author(s):  
P. G. Jambrina ◽  
A. Zanchet ◽  
M. Menéndez ◽  
V. J. Herrero ◽  
F. J. Aoiz

The present calculations for the O(3P) + H2 reaction show that the A′′ is more reactive than the A′ PES. However, at energies close to the vibrationally adiabatic barrier for H2 in j = 0, the reactive flux is larger on A′ PES due to a reorienting effect that promotes collinear approaches at the transition state.


Author(s):  
Niels Engholm Henriksen ◽  
Flemming Yssing Hansen

This chapter discusses a direct approach to the calculation of the rate constant k(T) that bypasses the detailed state-to-state reaction cross-sections. The method is based on the calculation of the reactive flux across a dividing surface on the potential energy surface. Versions based on classical as well as quantum mechanics are described. The classical version and its relation to Wigner’s variational theorem and recrossings of the dividing surface is discussed. Neglecting recrossings, an approximate result based on the calculation of the classical one-way flux from reactants to products is considered. Recrossings can subsequently be included via a transmission coefficient. An alternative exact expression is formulated based on a canonical average of the flux time-correlation function. It concludes with the quantum mechanical definition of the flux operator and the derivation of a relation between the rate constant and a flux correlation function.


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