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Strong exciton-phonon coupling incoherent excitons

4 Strong exciton phonon coupling incoherent excitons [Pg.418]

If we assume that the variation of the function P(m,f) over distances of the order of the lattice constant is small, then eqn (14.27) reduces to the diffusion equation. Indeed, assuming that the vector m varies continuously, we obtain [Pg.419]

If W(n, m) = W(m, n) (which holds if there is no static disorder in the crystal), substitution of the above expression into eqn (14.27) yields [Pg.419]

For crystals with several molecules (labeled by s) per unit cell, which have symmetry operations exchanging molecules with different s values, as holds for anthracene crystals, a similar procedure yields [Pg.419]

under the given conditions, the calculation of the diffusion tensor reduces to the determination of the hopping rates F(ns, ms ). [Pg.419]


STRONG EXCITON-PHONON COUPLING INCOHERENT EXCITONS 419... [Pg.419]


See other pages where Strong exciton-phonon coupling incoherent excitons is mentioned: [Pg.75]    [Pg.418]    [Pg.430]    [Pg.113]   


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