
The role of electronic symmetry in charge-transfer-to
... SH兲 algorithm of Prezhdo and Rossky23 for these calculations. This method is essentially an amalgam of mean-field dynamics24 and the Tully fewest-switches surface-hopping method.25 Although the MF/SH methodology has not been as widely used as the molecular dynamics with electronic transitions 共MDET兲 ...
... SH兲 algorithm of Prezhdo and Rossky23 for these calculations. This method is essentially an amalgam of mean-field dynamics24 and the Tully fewest-switches surface-hopping method.25 Although the MF/SH methodology has not been as widely used as the molecular dynamics with electronic transitions 共MDET兲 ...
Electronic Supplementary Material (ESI) for Journal of Materials Chemistry C.
... the charge transfer integral in the (100) direction. As a result TIPS-pentacene shows two-dimensional charge transport, whereas TES-pentacene is limited to one-dimensional transport. One-dimensional transport is obviously more affected by lattice defects as these irregularities represent a trap or b ...
... the charge transfer integral in the (100) direction. As a result TIPS-pentacene shows two-dimensional charge transport, whereas TES-pentacene is limited to one-dimensional transport. One-dimensional transport is obviously more affected by lattice defects as these irregularities represent a trap or b ...
Effect of electric field on the electronic spectrum and
... found that the one- and two-electron rings are similarly affected by the field. For example, the field would lower the eigenenergies and mix different partial waves. It would also cause severe localization and thus spoil the ABO, i.e. the amplitudes of oscillation of energy and persistent current wo ...
... found that the one- and two-electron rings are similarly affected by the field. For example, the field would lower the eigenenergies and mix different partial waves. It would also cause severe localization and thus spoil the ABO, i.e. the amplitudes of oscillation of energy and persistent current wo ...
down - Display Materials Lab.
... Ch 11. Quantum States for Many-Electron Atoms and Atomic Spectroscopy (A.S.) • States of many - e- atoms are grouped into terms and levels • A.S. is useful for obtaining information on the levels of atoms and ...
... Ch 11. Quantum States for Many-Electron Atoms and Atomic Spectroscopy (A.S.) • States of many - e- atoms are grouped into terms and levels • A.S. is useful for obtaining information on the levels of atoms and ...
Electron energy level statistics in graphene quantum dots
... The geometrical shape “cuts out” a piece of the hexagonal lattice such that armchair and zigzag parts of the boundary appear (for a general discussion of boundary conditions for the tight-binding model of graphene, see [14]). Furthermore, we study the effect of disorder that results from removing he ...
... The geometrical shape “cuts out” a piece of the hexagonal lattice such that armchair and zigzag parts of the boundary appear (for a general discussion of boundary conditions for the tight-binding model of graphene, see [14]). Furthermore, we study the effect of disorder that results from removing he ...
Atom-Light Interactions - Durham University Community
... causes the atom to oscillate between the ground and excited states. If we think in terms of energy transfer, then the conservation of energy implies that energy must be transferred to and from the monochromatic external light field. The processes that exchange energy with the driving field are known ...
... causes the atom to oscillate between the ground and excited states. If we think in terms of energy transfer, then the conservation of energy implies that energy must be transferred to and from the monochromatic external light field. The processes that exchange energy with the driving field are known ...
Fabre de la Ripelle M. A Mathematical Structure for Nuclei
... for −1 z 1 vanishing at z = 1, where Ṽ (ε) is the residual potential and P0 a projection operator which projects functions in the space of rk onto the space of the reference pair 1, 2. The zk and ωk refer to the variable z and ω for the pair k, = 1, 2. Another contribution can be introd ...
... for −1 z 1 vanishing at z = 1, where Ṽ (ε) is the residual potential and P0 a projection operator which projects functions in the space of rk onto the space of the reference pair 1, 2. The zk and ωk refer to the variable z and ω for the pair k, = 1, 2. Another contribution can be introd ...
The Rotation-vibration Hamiltonian
... position of the electrons are not involved). Because of this, it is common to say that the (ξ, η,ζ ) axes are “space-fixed”, while the ( x, y, z ) axes are “molecule-fixed”. That is, the new axes rotate with the molecule while the former axes do not. Although the origin of this new set of coordinate ...
... position of the electrons are not involved). Because of this, it is common to say that the (ξ, η,ζ ) axes are “space-fixed”, while the ( x, y, z ) axes are “molecule-fixed”. That is, the new axes rotate with the molecule while the former axes do not. Although the origin of this new set of coordinate ...
Raman Spectroscopy: Introductory Tutorial
... Organic: The Handbook of Infrared and Raman Characteristic Frequencies of Organic Molecules by Daimay Lin-Vien, et al ...
... Organic: The Handbook of Infrared and Raman Characteristic Frequencies of Organic Molecules by Daimay Lin-Vien, et al ...
Alkali D Line Data
... of the electron wave function. In the absence of external magnetic fields, these sublevels are degenerate. However, when an external magnetic field is applied, their degeneracy is broken. The Hamiltonian describing the atomic interaction with the magnetic field is µB (gS S + gL L + gI I) · B ...
... of the electron wave function. In the absence of external magnetic fields, these sublevels are degenerate. However, when an external magnetic field is applied, their degeneracy is broken. The Hamiltonian describing the atomic interaction with the magnetic field is µB (gS S + gL L + gI I) · B ...
24 Interferometry with Macromolecules: Quantum Paradigms Tested
... relation [3]. The passage through the hole in the wall improves the knowledge of the position state of the ball. Given the complementarity between position and momentum we conclude that the momentum uncertainty after the wall must be larger than before. In the plane of the goal this translates into ...
... relation [3]. The passage through the hole in the wall improves the knowledge of the position state of the ball. Given the complementarity between position and momentum we conclude that the momentum uncertainty after the wall must be larger than before. In the plane of the goal this translates into ...
TITLE: Molecules star in quantum movie STANDFIRST: The
... no less bizarre, is wave-particle duality: under some experimental conditions particles such as electrons and atoms behave as waves, whereas light – perhaps the mostly widely studied wave phenomenon in physics – often behaves as a stream of particles called photons. For decades the interference patt ...
... no less bizarre, is wave-particle duality: under some experimental conditions particles such as electrons and atoms behave as waves, whereas light – perhaps the mostly widely studied wave phenomenon in physics – often behaves as a stream of particles called photons. For decades the interference patt ...
Martin Quack
... century and is understood within the standard model of particle physics, SMPP. For molecular stereochemistry it leads to the surprising prediction of a small energy difference D of the ground state energies of the enantiomers of chiral molecules, corresponding to a small reaction enthalpy for the st ...
... century and is understood within the standard model of particle physics, SMPP. For molecular stereochemistry it leads to the surprising prediction of a small energy difference D of the ground state energies of the enantiomers of chiral molecules, corresponding to a small reaction enthalpy for the st ...
Franck–Condon principle
The Franck–Condon principle is a rule in spectroscopy and quantum chemistry that explains the intensity of vibronic transitions. Vibronic transitions are the simultaneous changes in electronic and vibrational energy levels of a molecule due to the absorption or emission of a photon of the appropriate energy. The principle states that during an electronic transition, a change from one vibrational energy level to another will be more likely to happen if the two vibrational wave functions overlap more significantly.