2000
DOI: 10.1016/s0301-0104(00)00157-9
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The lowest energy Frenkel and charge-transfer excitons in quasi-one-dimensional structures: application to MePTCDI and PTCDA crystals

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Cited by 234 publications
(297 citation statements)
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“…where ܴሺ‫,ܧ‬ ݀ሻ denotes in our case the reflectivity of the sample stack consisting of the quartz 1 MLE of PTCDA partially potassium-doped providing pronounced new features of PTCDA radical anions at low photon energies (investigated in detail previously 32 ), polycrystalline (pc) PTCDA 33 and the dramatically broadened spectra of 1 MLE of PTCDA on Au(111) and Ag(111) 34,35 are shown in the bottom panel. b) Δ‫ܴܵܦ‬ of PTCDA on quartz glass for nominal thicknesses ranging from submonolayers up to 1 MLE.…”
Section: Resultsmentioning
confidence: 99%
“…where ܴሺ‫,ܧ‬ ݀ሻ denotes in our case the reflectivity of the sample stack consisting of the quartz 1 MLE of PTCDA partially potassium-doped providing pronounced new features of PTCDA radical anions at low photon energies (investigated in detail previously 32 ), polycrystalline (pc) PTCDA 33 and the dramatically broadened spectra of 1 MLE of PTCDA on Au(111) and Ag(111) 34,35 are shown in the bottom panel. b) Δ‫ܴܵܦ‬ of PTCDA on quartz glass for nominal thicknesses ranging from submonolayers up to 1 MLE.…”
Section: Resultsmentioning
confidence: 99%
“…12, 13,20,25,33 When |J k=0 − U| ≫ |t e + t h | (Figure 3a), the diabatic FE and CTE bands are energetically well separated, limiting the FE/ CTE mixing. In this regime, FE/CTE mixing is dominated by the first-order processes described by eq 12; only CT states characterized by p = π/N, 3π/N, ... appreciably mix with the FE, as very little second-order mixing between CT states occurs via indirect coupling through the FE state.…”
Section: Journal Of the American Chemical Societymentioning
confidence: 99%
“…Coupling between the CT states and the optically allowed FE depends on the sum |t e + t h |, in agreement with previous works. 12, 13,[20][21][22][23][24][25]33 Importantly, this sum also determines the coupling between CT states of different electron/hole radii (see eq 7) and thus the k = 0 CT bandwidth (see Figure 6a−c). 33 Hence, the relative phases of the CT integrals determine not only the probability of the excitation existing in a charge-separated state after absorption but also the extent to which the electron and hole are separated in such states.…”
Section: Journal Of the American Chemical Societymentioning
confidence: 99%
“…The E FR is much lower than the E CT in the spin triplet channel (υ = 0), because Ẅ >> Ŵ, therefore the lowest triplet exciton is predominantly FR exciton in molecular crystals. However, whether the lowest singlet exciton is CT or FR depends on the relative strength of υ and Ẅ, e.g., FR for picene 14 but a mixture of CT and FR for pentacene 14,26,27 and PTCDA 26,27,55 . For the PTB7 crystal, the on-site attractive e-h interaction Ẅ may be close to the sum of inter-site attractive matrix elements Ŵ due to the strong inter-chain π-π interaction.…”
Section: Optical Excitationsmentioning
confidence: 99%