コーパス検索結果 (1語後でソート)
通し番号をクリックするとPubMedの該当ページを表示します
1 and stems from an excited complex (i.e., an exciplex).
2 consistent with formation of a quinone-water exciplex.
3 he ion pair occur almost exclusively via the exciplex.
4 ependence, these bands can be assigned to an exciplex.
5 conversion among the encounter pairs and the exciplex.
6 proceeds through spin-mixing in the triplet exciplex.
7 d hyperfine interactions in the spin triplet exciplex.
8 lower energies, indicative of a new emissive exciplex.
9 , the tetracoordinate excited state, and the exciplex.
10 r emission line is assigned to an Irppy.niBr exciplex.
11 ng the ionic polarization to generate SOC in exciplexes.
12 nformations and the participation of triplet exciplexes.
13 (DA) pair leads, in some cases, to emissive exciplexes.
14 ng excited singlets, triplets, excimers, and exciplexes.
15 The charge transfer (CT) character of the exciplexes (88-97%) was calculated from the electronic c
16 conversion among the encounter pairs and the exciplex (A*/D right harpoon over left harpoon exciplex
18 s the dominant pathway for relaxation, since exciplex and niBr triplet states give either weak or no
20 s have very similar energies for the dopant, exciplex, and niBr triplet states, such that relaxation
21 ZnO impurities, amine-donor charge-transfer exciplexes, and framework decomposition in samples of MO
23 idly interconverting encounter pairs with an exciplex as intermediate, A*/D right harpoon over left h
26 quenching, viz., the loose ion pair and the exciplex, based on the time-resolved magnetic field effe
29 e well suited to demonstrating that emissive exciplexes can be formed in water from purely organic co
32 stem crossing (RISC) from triplet to singlet exciplex diminishes, a pronounced isotope effect is obse
33 emission and increases the efficiency of the exciplex emission as the e-h separation reduces, is disc
34 lays a charge transfer band at 450 nm and an exciplex emission at 520 nm, indicating the formation of
37 anic small-molecule, dendrimer, polymer, and exciplex emitters are all discussed within this review,
38 high CT character in a highly polar solvent, exciplex fluorescence quantum yields up to 0.03 and life
40 gnificantly lowers the activation energy for exciplex formation (E(a)) and helps stabilize the highly
41 the reduction of the singlet-triplet gap by exciplex formation and the external heavy atom effect.
44 mation of both static and dynamic complexes (exciplex formation), which is aided by hydrogen bonding.
45 oly(methyl methacrylate) (PMMA), without any exciplex formation, and its OLPL duration reaches more t
46 of host-guest complexes toward fluorescence, exciplex formation, charge separation, room-temperature
51 relative intensity of the anthracene-related exciplex, formed from the encounter complex, was 8 times
56 omophore leads to formation of a fluorescent exciplex in polar solvents but pyrene-like fluorescence
57 rmation of the aforementioned intramolecular exciplex in terms of a radical ion pair stabilized throu
58 ion to recent findings on the involvement of exciplexes in photoinduced electron transfer reactions.
61 al that the triplet-to-singlet conversion in exciplexes involves an artificially generated spin-orbit
64 ne-based pi-pi* fluorescence) a lower-energy exciplex-like emission feature associated with a naphthy
66 the excited-state charge-transfer complexes (exciplexes) of the PPEs with analytes were observed.
71 actions), we reported recently that cationic exciplexes (products of charge shift reactions) can be f
72 ing" aliphatic amine forms an intramolecular exciplex, providing alternative nonradiative deactivatio
73 ciplex (A*/D right harpoon over left harpoon exciplex right harpoon over left harpoon A(*-)/D(*+)).
74 ediate, A*/D right harpoon over left harpoon exciplex right harpoon over left harpoon A(*-)/D(*+).
75 the first time to Au-Au bonded excimers and exciplexes similar to those reported earlier for Ag(I) c
77 designed to study the characteristics of the exciplex state pinned at a donor-acceptor abrupt interfa
79 initial excitations that decay to long-lived exciplex states is approximately equal to the fraction o
80 ons to low-energy states such as triplet and exciplex states that are nonemissive or weakly emissive.
81 s associated with two stacked bases decay to exciplex states, whereas excitations in unstacked bases
85 The results confirm the previously proposed "exciplex" structure of the MLCT state in Lewis basic sol
86 L emitters are mainly based on a bimolecular exciplex system which usually needs an expensive small m
87 th high mobility, combined with an interface exciplex that confines excitons at the emissive layer/el
88 ayed fluorescence (TADF) from donor-acceptor exciplexes that are either protonated (H) or deuterated
90 -pyrimidine (B3PYMPM) (DeltaE(ST) = 130 meV) exciplexes, the SOC generated by the intermolecular char
92 or the reversible formation and decay of the exciplexes were determined using time-correlated single-
93 nd excited-state energies (dopant, niBr, and exciplex) were used to explain the observed spectral pro
94 an unit creates a new route for decay of the exciplex whereby the triplet state of the spiropyran is