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Quantum mechanics states that hopping integral between local orbitals makes the energy band dispersive.
The ratio of the specific heat integral between selected temperatures gives only a rough indication of the fragility behaviour.
Here 〈1E|nH〉 is the overlap integral between the first electron and the n th heavy-hole states.
The hopping integral between two neighboring atoms in the benzene molecule is quantitatively estimated using fully self-consistence DFT based calculations as implemented in SIESTA package.
Thus, for graphene, a large tension is needed to reduce the hopping integral between C p z orbitals for the antiferromagnetism [56].
Comparing the opto-geometrical parameters of these two fibers and hence the overlap integral between the guided mode and the doped region, it could be concluded that the guiding properties of the two fibers are the same.
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Here 〈1E|nH〉 and 〈nH|1E〉 (〈SO|1E〉) are the overlap integrals between the discussed electron and hole (SO) states.
Similarly, the integrals between Pb and Te are assumed to be like in PbTe.
The relevant integrals between the Te and Cd states are simply taken equal to those in CdTe.
where the elements S ij AB are the overlap integrals between the one-electron basis functions, i.e., S ij AB = ∫ d r ϕ i A * r ϕ j B r. (12).
Using the tight-binding approximation developed for such systems by Bouchard and Luban[25], the amplitude of the electron wave function can be expressed by the transfer integrals between the nearest quantum wells V1: | n 〉 = ∑ l = − ∞ ∞ J l − n 2 V 1 eFd u l ( z ), (3).
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