Renner–Teller coupled-channel dynamics of the N(D2)+H2 reaction and the role of the NH2 Ã A21 electronic state

2008 ◽  
Vol 129 (24) ◽  
pp. 244307 ◽  
Author(s):  
Pablo Gamallo ◽  
Paolo Defazio ◽  
Miguel González ◽  
Carlo Petrongolo
Symmetry ◽  
2021 ◽  
Vol 13 (7) ◽  
pp. 1171
Author(s):  
Humberto Garcilazo ◽  
Alfredo Valcarce

We present a comprehensive study of the decay width of multiquark states containing different color singlet components in a coupled-channel approach. We show how the decay width can provide in-depth information about the nature of a coupled-channel resonance. An unexpected behavior of the decay width of a multiquark state could be pointing to a relevant role of the coupled-channel dynamics, aiming at the channel responsible for the formation of the resonance. The symmetrical situation between meson- and baryon-like multiquarks is highlighted. Our study accounts for the existence of narrow resonances with large phase spaces. In the case of resonances far from their detection channel, it is the mass difference with the formation channel that determines their decay width. The larger the binding, the larger the decay width, even though the phase space to the detection channel gets reduced. The trends noticed cast doubts on the molecular assignment of some multiquark candidates. Finally, we wonder about the existence and properties of multiquark partners in other flavor sectors.


2017 ◽  
Vol 19 (36) ◽  
pp. 25105-25114 ◽  
Author(s):  
Akira Oda ◽  
Takahiro Ohkubo ◽  
Takashi Yumura ◽  
Hisayoshi Kobayashi ◽  
Yasushige Kuroda

Understanding the exact position and the detailed role of the Al array in zeolites is essential for elucidating the origin of unique properties and for designing zeolite materials with high efficiency in catalytic and adsorption processes. In this work, we advanced pivotal roles of Lewis base–metal ion bifunctionality caused by Al atoms arrayed circumferentially in the MFI-zeolite pores.


1993 ◽  
Vol 47 (5) ◽  
pp. 2356-2364 ◽  
Author(s):  
L. S. Celenza ◽  
A. Pantziris ◽  
C. M. Shakin ◽  
J. Szweda

2017 ◽  
Vol 137 ◽  
pp. 13014
Author(s):  
Enrique Ruiz Arriola ◽  
Lorenzo Luis Salcedo ◽  
Eugenio Megías

2005 ◽  
Vol 755 ◽  
pp. 29-39 ◽  
Author(s):  
M.F.M. Lutz ◽  
E.E. Kolomeitsev

2005 ◽  
Vol 72 (1) ◽  
Author(s):  
Sourav Sarkar ◽  
E. Oset ◽  
M. J. Vicente Vacas

1988 ◽  
Vol 207 (2) ◽  
pp. 115-120 ◽  
Author(s):  
F. Cannata ◽  
J.P. Dedonder ◽  
L. Leśniak

2015 ◽  
Vol 93 (11) ◽  
pp. 1343-1351 ◽  
Author(s):  
Manjeet Singh Gautam

This article analyzes the validity of static Woods–Saxon potential and the energy-dependent Woods–Saxon potential (EDWSP) to explore the specific features of fusion dynamics of [Formula: see text] and [Formula: see text] systems. The intrinsic degrees of freedom, such as inelastic surface excitations, play a crucial role in the enhancement of sub-barrier fusion excitation functions over the expectations of the one-dimensional barrier penetration model. Role of dominant intrinsic degrees of freedom of collision partners are entertained within the context of coupled channel calculations. Furthermore, the one-dimensional Wong formula using static Woods–Saxon potential fails miserably to describe the fusion enhancement of [Formula: see text] and [Formula: see text] systems. However, the Wong formula along with the EDWSP model accurately explains the observed fusion enhancement of [Formula: see text] reactions. In the fusion of [Formula: see text] reaction, the above-barrier fusion data are suppressed by a factor of 0.66 with reference to the EDWSP model calculations while the below-barrier fusion data are adequately addressed by the EDWSP model and the coupled channel calculations. Therefore, the coupled channel calculations and the EDWSP model calculations reasonably describe the observed fusion mechanism of [Formula: see text] and [Formula: see text] reactions. This suggests that the energy dependence in the Woods–Saxon potential model introduces similar kinds of barrier modification effects (barrier height, barrier position, and barrier curvature) as reflected from the coupled channel calculations. In the EDWSP model calculations, significantly larger values of diffuseness ranging from a = 0.86 to 0.94 fm, which is much larger than a value extracted from the elastic scattering analysis, are needed to address the sub-barrier fusion data.


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