Photodissociation of CH2. VI. Three-dimensional quantum dynamics of the dissociation through the coupled 2A″ and 3A″ states

1997 ◽  
Vol 107 (15) ◽  
pp. 5757-5770 ◽  
Author(s):  
Geert-Jan Kroes ◽  
Marc C. van Hemert ◽  
G. D. Billing ◽  
Daniel Neuhauser
2019 ◽  
Vol 9 (1) ◽  
Author(s):  
Yue-Min Wan ◽  
Heng-Tien Lin

AbstractStudy on single electron tunnel using current-voltage characteristics in nanopillar transistors at 298 K show that the mapping between the Nth electron excited in the central box ∼8.5 × 8.5 × 3 nm3 and the Nth tunnel peak is not in the one-to-one correspondence to suggest that the total number N of electrons is not the best quantum number for characterizing the quality of single electron tunnel in a three-dimensional quantum box transistor. Instead, we find that the best number is the sub-quantum number nz of the conduction z channel. When the number of electrons in nz is charged to be even and the number of electrons excited in the nx and ny are also even at two, the adding of the third electron into the easy nx/ny channels creates a weak symmetry breaking in the parity conserved x-y plane to assist the indirect tunnel of electrons. A comprehensive model that incorporates the interactions of electron-electron, spin-spin, electron-phonon, and electron-hole is proposed to explain how the excited even electrons can be stabilized in the electric-field driving channel. Quantum selection rules with hierarchy for the ni (i = x, y, z) and N = Σni are tabulated to prove the superiority of nz over N.


2002 ◽  
Vol 65 (22) ◽  
Author(s):  
François Triozon ◽  
Julien Vidal ◽  
Rémy Mosseri ◽  
Didier Mayou

2011 ◽  
Vol 10 (03) ◽  
pp. 297-307
Author(s):  
SINAN AKPINAR ◽  
TUNAY TURMUS ◽  
SEDA SURUCU

In this paper, we report the results of three dimensional time dependent quantum wave packet calculations carried out for He+Li2 inelastic reaction in the collision energy range 0.43–1.18 eV. A three dimensional potential energy surface (PES) computed by Varandas was used for the dynamical calculations.1 The state to state and state to all transition probabilities for total angular momentum J = 0 have been calculated in a broad range of collision energies. Integral cross-sections and rate constants have been calculated from the wave packet transition probabilities by means of J-shifting approximation based on a capture model and a uniform J-shifting method for J > 0.


1996 ◽  
Vol 248 (1-2) ◽  
pp. 37-42 ◽  
Author(s):  
Tong Peng ◽  
Dong H. Zhang ◽  
John Z.H. Zhang ◽  
Reinhard Schinke

2019 ◽  
Vol 10 (1) ◽  
Author(s):  
Stefan Mueller ◽  
Julian Lüttig ◽  
Pavel Malý ◽  
Lei Ji ◽  
Jie Han ◽  
...  

Abstract Coherent two-dimensional spectroscopy is a powerful tool for probing ultrafast quantum dynamics in complex systems. Several variants offer different types of information but typically require distinct beam geometries. Here we introduce population-based three-dimensional (3D) electronic spectroscopy and demonstrate the extraction of all fourth- and multiple sixth-order nonlinear signal contributions by employing 125-fold (1⨯5⨯5⨯5) phase cycling of a four-pulse sequence. Utilizing fluorescence detection and shot-to-shot pulse shaping in single-beam geometry, we obtain various 3D spectra of the dianion of TIPS-tetraazapentacene, a fluorophore with limited stability at ambient conditions. From this, we recover previously unknown characteristics of its electronic two-photon state. Rephasing and nonrephasing sixth-order contributions are measured without additional phasing that hampered previous attempts using noncollinear geometries. We systematically resolve all nonlinear signals from the same dataset that can be acquired in 8 min. The approach is generalizable to other incoherent observables such as external photoelectrons, photocurrents, or photoions.


2000 ◽  
Vol 318 (1-3) ◽  
pp. 256-262 ◽  
Author(s):  
I. Andrianov ◽  
V. Bonačić-Koutecký ◽  
M. Hartmann ◽  
J. Manz ◽  
J. Pittner ◽  
...  

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