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1 tronic transition is 'dark' with a vanishing oscillator strength.
2 actors responsible for the modulation of the oscillator strength.
3 ity from the former to achieve an observable oscillator strength.
4 nm] and the decrease in the lambda(max) band oscillator strength (0.069 +/- 0.004) of E181Q relative
5 2* orbitals agrees with the calculated TDDFT oscillator strengths [0.10 and 0.21, (C5H5)2TiCl2; 0.21
6 of J-aggregates that due to their high peak oscillator strength and high luminescence efficiency hav
10 parameters, electronic transition energies, oscillator strengths, and transition polarizations for N
11 orin 12, red-shifted Q(x) band with enhanced oscillator strengths) are detailed and rationalized on t
12 measured their first and second exciton peak oscillator strengths as a function of size and chemical
13 d near 693 nm and characterized by very weak oscillator strength) as well as emission peaks near 691
14 which allow for exceptional control over the oscillator strengths at the exciton and trion resonances
15 e in character and exhibits not only a large oscillator strength but an unusually large doubly excite
16 ucture arises because of a redistribution of oscillator strength, but the through-space couplings do
18 relative to pure CsPbBr3 indicates enhanced oscillator strength consistent with earlier published at
19 ate direct band gap character based on their oscillator strengths, different from previously reported
21 ty of a material in relation to light is its oscillator strength distribution, i.e., how strongly it
23 bdamax approximately 455 nm) with a very low oscillator strength (f approximately 0.6, epsilon approx
24 osine, base stacking was found to reduce the oscillator strength for the fluorescence transition, but
25 mitting characteristics and enormous exciton oscillator strength, however, their low charge carrier m
27 50 and B875 due to partial redistribution of oscillator strength into a higher energetic exciton tran
28 ystems with low exchange energy, substantial oscillator strength is sustained at the singlet-triplet
30 ular architecture (M-(PM')n-M), wherein high-oscillator-strength NIR absorptivity up to 850 nm, near-
31 ime, together with the combination of modest oscillator strength of atoms and low collection efficien
32 AP in the trimers suffers a reduction in the oscillator strength of its low-lying pi-pi* 2AP-like all
33 ture is not identified probably due to lower oscillator strength of plasmon compared to the coronene.
35 with a concomitant blue shift and decreased oscillator strength of the lambdamax absorption band.
36 as been attributed to the strongly modulated oscillator strength of the ligand field transitions rath
37 of the monomers, which are due to the small oscillator strength of the lowest optical transition, ar
39 ions, conformational distribution, and large oscillator strength of the V (pipi*) transition in sinap
40 ligand field state and strong modulation of oscillator strengths of ligand field transitions by cohe
41 ole formation is due to large differences in oscillator strengths of the S(0) <--> S(1) transitions i
43 bits approximately 8-fold greater absorptive oscillator strength over the 380-700 nm range relative t
44 and demonstrate for the first time that high oscillator strength porphyrinic chromophores, convention
45 ll as the initial linear rise of the 0-0/1-0 oscillator strength ratio with increasing |J(0)|, are in
46 The plasmon resonances have remarkably large oscillator strengths, resulting in prominent room-temper
47 the L(a) transition, which has a much higher oscillator strength than the S(1)L(b)-transition of pyre
48 tly the corresponding S(1)-->S(0) transition oscillator strength; these data show that these effects
49 tantial PCE is attributed to the broad, high oscillator strength visible absorption, the ordered mole
50 ndent DFT calculated transition energies and oscillator strengths, which agree well with the experime
51 ansition energies and polarization-dependent oscillator strengths, which agreed well with the XANES s
52 etype, evince strong mixing of the PZn-based oscillator strength with ruthenium terpyridyl charge res
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