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Exciton states and optical transitions in colloidal CdS quantum dots
Exciton states and optical transitions in colloidal CdS quantum dots

92, 075445 (2015)
92, 075445 (2015)

... electrostatics [40] that the long-range exchange Coulomb interaction indeed corresponds to the electrostatic dipoledipole coupling. Matrix elements (5) can thus be directly represented by using Eqs. (9) and (4) in terms of interacting “transition dipoles” [Eq. (10)]. This physically attractive reals ...
Optical cooling of interacting atoms in a tightly confined trap
Optical cooling of interacting atoms in a tightly confined trap

Detecting a many-body mobility edge with quantum
Detecting a many-body mobility edge with quantum

Controlling Chemical Reactions by Short, Intense Mid
Controlling Chemical Reactions by Short, Intense Mid

... light may not be statistically significant. The results for circularly polarized pulses with a maximum field strength of 0.06 au can be compared to linearly polarized pulses averaged over ϕ = 0−360°. The yield of H and HCl+ is much less for linear polarized light than for circularly polarized light wi ...
THEORETICAL AND COMPUTATIONAL METHODS
THEORETICAL AND COMPUTATIONAL METHODS

... a.u. The only adiabatic state open for dissociation is the ground state, a = 1. However, the components with a = 2 − 4 have small oscillating tails (may not be visible), which are due to the coupling of the corresponding adiabatic states to φ1 (ρ; θ, φ). This is a generic property of the hyperspheri ...
Life beyond quantum physics
Life beyond quantum physics

... bird. In physical systems the final state is determined by the initial conditions plus the physical laws. In biological organisms the case is the opposite: the final state is determined by the living organisms themselves (Bertalanffy, 1950). Action is an ideal tool of choice to describe biological p ...
Deviation from Universality in Collisions of Ultracold 6Li2 Molecules
Deviation from Universality in Collisions of Ultracold 6Li2 Molecules

... and leaving the decay rate dependent on only the longrange van der Waals interaction between collision partners. It has been validated in various experimental settings [1], involving heavier alkali molecules like Rb2 [9], Cs2 [10,11], KRb [2], RbCs [12], and LiCs [13]. These universal collisions hav ...
Synthesis and Characterization of Tetradentate Complexes Type
Synthesis and Characterization of Tetradentate Complexes Type

Quantum coherent biomolecular energy transfer with spatially
Quantum coherent biomolecular energy transfer with spatially

... 2.1. Model The simplest way to model a single chromophore (or pigment) is by describing it as a quantum two-level system consisting of a ground and an excited state, which are separated by the energy gap ǫ. When the electron is in the excited state, it is localized by its attractive interaction with ...
SEMICLASSICAL AND LARGE QUANTUM NUMBER LIMITS
SEMICLASSICAL AND LARGE QUANTUM NUMBER LIMITS

8 Selectivity of the O e
8 Selectivity of the O e

Dynamics and Excited States of Quantum Many
Dynamics and Excited States of Quantum Many

... and effective magnetic fields are engineered using laser fields, and the individual spin states are directly imaged with state-dependent fluorescence. The results in this thesis address several of the ongoing challenges in the development of synthetic quantum matter platforms. One such challenge is ...
Photosynthetic pigment-protein complexes as highly connected
Photosynthetic pigment-protein complexes as highly connected

... The focus of recent work from our group, as well as this article, has been on how one can use simple ideas emerging from the theory of networks (or graphs), along with quantum dynamics simulations of EET, in order to interrogate and, ultimately, rationalize the structural motifs adopted by biologica ...
Gujarat University Ahmedabad B. Sc. (PHYSICS) Semester – V
Gujarat University Ahmedabad B. Sc. (PHYSICS) Semester – V

Presentation453.08
Presentation453.08

Optical control of the spin of a magnetic atom in a semiconductor
Optical control of the spin of a magnetic atom in a semiconductor

Ultrafast Acoustic Phonon Ballistics in Semiconductor Heterostructures
Ultrafast Acoustic Phonon Ballistics in Semiconductor Heterostructures

Non-abelian quantum Hall states and fractional charges in
Non-abelian quantum Hall states and fractional charges in

Non-abelian quantum Hall states and fractional charges in one dimension Emma Wikberg
Non-abelian quantum Hall states and fractional charges in one dimension Emma Wikberg

Some insights on theoretical reaction dynamics: Use
Some insights on theoretical reaction dynamics: Use

... sectors, number of meshpoints in each sectors and the size of the internal basis. In particular, special attention was payed to the pmax convergence and our results confirmed those previously published. Next, convergence conditions were established for the complete integral cross section calculation ...
Reaction of tungsten anion clusters with molecular and atomic
Reaction of tungsten anion clusters with molecular and atomic

... n for n⫽2 – 5 are expected to be weaker than those for n⬎5. TOF mass spectroscopy experiments in Fig. 1 reveal that reactivities of W⫺ n 共for n⫽3 – 8) toward N2 adsorption become lower with decreasing cluster size, which seems to reconcile with the weaker charge transfers for the smaller clusters. I ...
Quantum control of a model qubit based on a multi - FaMAF
Quantum control of a model qubit based on a multi - FaMAF

Ligand field density functional theory calculation of the 4f²→ 4f¹5d¹
Ligand field density functional theory calculation of the 4f²→ 4f¹5d¹

Molecular simulation with variable protonation states at constant pH
Molecular simulation with variable protonation states at constant pH

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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.
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