2015
DOI: 10.1021/acs.chemrev.5b00012
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Light-Driven and Phonon-Assisted Dynamics in Organic and Semiconductor Nanostructures

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Cited by 169 publications
(212 citation statements)
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References 527 publications
(699 reference statements)
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“…[65][66][67] Shown in Figure 7, the FTs indicate that many more modes contribute to dephasing in bare Cd 33 Se 33 compared to that in passivated 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60…”
Section: Phonon Modesmentioning
confidence: 99%
“…[65][66][67] Shown in Figure 7, the FTs indicate that many more modes contribute to dephasing in bare Cd 33 Se 33 compared to that in passivated 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60…”
Section: Phonon Modesmentioning
confidence: 99%
“…Such organic π-conjugated semiconductors have striking and rather complex optical properties. Their optical excitation not only results in the formation of excitons, Coulomb bound electron-hole pairs, but—in contrast to, for example, inorganic semiconductors—also in the creation of a wealth of other quasiparticles, namely polaron pairs, polarons, biexcitons and others91011. Polaron pairs, sometimes also called spatially indirect or charge-transfer excitons, are charge-neutral excitations in which spatially separated electrons and holes weakly interact via their Coulomb attraction and are each coupled to their own lattice distortion.…”
mentioning
confidence: 99%
“…So, additionally one needs to compute exciton relaxation times due to phonon emission, and, then, contributions to R 1 , R 2 from decays of a photon into low-energy excitons. At the atomistic level, this task can be achieved by employing the finite temperature/real time technique of perturbative many-body quantum mechanics [102][103][104], or the reduced density matrix method [76,[105][106][107].…”
Section: Discussionmentioning
confidence: 99%