about
Stimulated emission from distyrylbenzene derivative crystals grown by vapor deposition.Emission behaviors of unsymmetrical 1,3-diaryl-β-diketones: a model perfectly disclosing the effect of molecular conformation on luminescence of organic solids.Multicolor Amplified Spontaneous Emissions Based on Organic Polymorphs That Undergo Excited-State Intramolecular Proton Transfer.Cross dipole stacking in the crystal of distyrylbenzene derivative: the approach toward high solid-state luminescence efficiency.Doublet-Triplet Energy Transfer-Dominated Photon Upconversion.Up to 100% Formation Ratio of Doublet Exciton in Deep-Red Organic Light-Emitting Diodes Based on Neutral π-Radical.Stable Organic Radicals as Hole Injection Dopants for Efficient Optoelectronics.A Stable Room-Temperature Luminescent Biphenylmethyl Radical.Triplet-Polaron-Interaction-Induced Upconversion from Triplet to Singlet: a Possible Way to Obtain Highly Efficient OLEDs.Bipolar AIE-active luminogens comprised of an oxadiazole core and terminal TPE moieties as a new type of host for doped electroluminescence.Two-Dimensional Organic Single Crystals with Scale Regulated, Phase-Switchable, Polymorphism-Dependent, and Amplified Spontaneous Emission Properties.Delayed fluorescence in a solution-processable pure red molecular organic emitter based on dithienylbenzothiadiazole: a joint optical, electroluminescence, and magnetoelectroluminescence study.Charge-transfer-featured materials-promising hosts for fabrication of efficient OLEDs through triplet harvesting via triplet fusion.Radical-Based Organic Light-Emitting Diodes with Maximum External Quantum Efficiency of 10.6Efficient radical-based light-emitting diodes with doublet emissionOrganic Light-Emitting Diodes Using a Neutral π Radical as Emitter: The Emission from a DoubletRelationship between molecular stacking and optical properties of 9,10-bis((4-N,N-dialkylamino)styryl) anthracene crystals: the cooperation of excitonic and dipolar couplingSingle-benzene solid emitters with lasing properties based on aggregation-induced emissionsEffects of substituents on luminescent efficiency of stable triaryl methyl radicalsHighly Efficient Fluorescent Organic Light-Emitting Devices Using a Luminescent Radical as the SensitizerFine Modulation of the Higher-Order Excitonic States toward More Efficient Conversion from Upper-Level Triplet to SingletHigh stability and luminescence efficiency in donor-acceptor neutral radicals not following the Aufbau principleCircularly polarized luminescence of achiral open-shell π-radicalsUnderstanding the luminescent nature of organic radicals for efficient doublet emitters and pure-red light-emitting diodes
P50
Q33288256-7695FD17-5326-4C41-97FA-06519C692C65Q35179318-11BE35F3-23DC-4457-81FD-C40858872611Q35936519-73242526-613F-4635-A4AC-95FCC6EFB66BQ46746858-7E39119B-310A-41DB-BC34-63B068A2196EQ48048800-9065CE26-6E4D-40AB-AFA4-23F40352E7C0Q48172208-C16F387F-E204-40A3-A79D-D56519E27FDEQ48220757-9C151529-85C5-4EBA-A797-09E53DA4B584Q48228106-6172FC27-C4B4-432A-85FC-8309087B7B3AQ50203267-F0F6FED6-2247-46F2-BDCC-CDFAE73FCFAEQ50242646-CA3FB426-32B3-41BA-8505-86756DF27F05Q50243691-CAF0D297-B4A4-4EEC-BF5E-B235B8384FD1Q50453606-7AF788BB-5454-415A-A35C-DA64A1890EE4Q50456801-6BEA55E6-F3CE-4F5D-8F1E-153696A63CA6Q58598394-05736894-A143-4CC5-B66F-616A924E475BQ59068694-33A3C1B1-2C12-4614-A6C3-D11E7E3E2138Q87196538-F9D079E9-6D50-4597-8E95-D112A9EA4263Q87416280-03026F26-EF35-46A9-B603-B539BFF08D0BQ89288235-8DF8E5FF-F001-455F-834F-D62B37F501CDQ89336898-0B6DE58B-CEC9-4C63-86E9-2887BCBA7418Q90421105-99ED7891-0987-4147-B77A-C4E0245E738BQ90710333-FD576018-D83B-49E1-9628-AB129663EFFFQ92093575-F6C11F93-21D7-4D2E-8E96-9F5B767AA509Q92185857-8E887E4D-9230-431E-AA3A-8C4D32291695Q96431789-817FBA8A-5E60-4E53-BE60-A1ED7ABD4031
P50
description
researcher
@en
հետազոտող
@hy
name
Feng Li
@ast
Feng Li
@en
Feng Li
@es
Feng Li
@nl
Feng Li
@sl
type
label
Feng Li
@ast
Feng Li
@en
Feng Li
@es
Feng Li
@nl
Feng Li
@sl
prefLabel
Feng Li
@ast
Feng Li
@en
Feng Li
@es
Feng Li
@nl
Feng Li
@sl
P1053
E-4879-2013
P106
P108
P31
P3829
P496
0000-0001-5236-3709