Increase in the asymmetry on increasing excitation laser power density is due to Fano interaction between electronic Raman scattering involving photo-excited electrons within electronic states and usual optical phonon Raman scattering [10].
The energies of the hybridized modes are easily understood by the electrostatic interaction between electronic charge densities.
The presence of the Si-ncs in the polymer increases the transport and assures an interaction between electronic states of the Si-ncs and P3HT polymer.
In their analysis, they categorised interventions by the types of electronic or non-electronic interventions the interventions included and then tested interaction between electronic and non-electronic components, additive effects between electronic and non-electronic components, and whether electronic components could be considered equivalent in their effectiveness.
This singular behaviour of the polaron concentration has a direct impact on the uranium sublattice partial molar heat capacity and an indirect effect on the energy interactions between the electronic and ionic structure of the target mediated by these polarons.
Interactions between the electronic excited states of these dye molecules lead to the transfer of excitation energy in a nonradiative process from the donor molecule to the acceptor molecule.
On the contrary, a positive Laplacian indicates the local depletion of electron density, typical of closed-shell interactions, i.e. interaction between two electronic systems with the outermost electronic shell filled, as it occurs in ionic bonds, or any other interaction between molecules (van der Waals, medium-weak hydrogen bonding etc).
The hyperfine interaction between the electronic spin and the 14N nuclear spin term (AIcdotsigma) can be separated into the diagonal term (AI^{x}sigma^{x}) and the flip-flop term (A(I^{y}sigma ^{y}+I^{z}sigma^{z})).
The strong coupling regime is observed in heterostructures due to the efficient radiative scattering without any loss of energy, which would lead to interactions between quantum-confined electronic states in semiconductor nanostructures and dielectric-confined electromagnetic modes in the metal counterparts.
