2022
DOI: 10.1039/d1mh00846c
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Excited states engineering enables efficient near-infrared lasing in nanographenes

Abstract: The spectral overlap between stimulated emission (SE) and absorption from dark states (i.e. charges and triplets) especially in the near-infrared (NIR), represents one of the most effective gain loss channel...

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Cited by 17 publications
(22 citation statements)
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References 67 publications
(64 reference statements)
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“…[ 18 ] Both NGs present similar performances in terms of gain and losses (Figure S5, Supporting Information, and Table 1), with losses being mainly dominated by those of the PS matrix. Moreover, the ASE threshold and gain values of BOTT‐Mes are comparable to those obtained for other NGs [ 5,19 ] and only slightly inferior in performance than those of state of the art organic molecules dispersed in inert matrixes, such as perylenediimides [ 20 ] and carbon‐bridged oligo( p ‐phenylenevinylene)s. [ 21 ] Additionally, the ASE photostability was tested under an uninterrupted ns‐pulsed pump (10 Hz) at four to five times E th‐ASE in ambient conditions. The ASE half‐life parameter (τ 1/2 ) is determined as the number of pulses needed for the initial output intensity to reach half its initial value (Figure S6, Supporting Information).…”
Section: Resultssupporting
confidence: 54%
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“…[ 18 ] Both NGs present similar performances in terms of gain and losses (Figure S5, Supporting Information, and Table 1), with losses being mainly dominated by those of the PS matrix. Moreover, the ASE threshold and gain values of BOTT‐Mes are comparable to those obtained for other NGs [ 5,19 ] and only slightly inferior in performance than those of state of the art organic molecules dispersed in inert matrixes, such as perylenediimides [ 20 ] and carbon‐bridged oligo( p ‐phenylenevinylene)s. [ 21 ] Additionally, the ASE photostability was tested under an uninterrupted ns‐pulsed pump (10 Hz) at four to five times E th‐ASE in ambient conditions. The ASE half‐life parameter (τ 1/2 ) is determined as the number of pulses needed for the initial output intensity to reach half its initial value (Figure S6, Supporting Information).…”
Section: Resultssupporting
confidence: 54%
“…The fabricated device presents similar laser properties to that previously reported for DFB laser based on TT‐Ar ( E th‐DFB = 25 ± 3 µJ cm –2 for TE 0 ) and other NGs such as FZ1 (50 ± 5 µJ cm –2 for TE 0 ), FZ2 (11 ± 1 µJ cm –2 for TE 0 ) or DBOV‐FAI (50 ± 5 µJ cm –2 for TE 0 ). [ 5,19b ] Additionally, the device based on BOTT‐Mes shows a threshold value similar to those found for state‐of‐the‐art organic compounds dispersed in inert matrixes, e.g., PDI‐O (22 ± 2 µJ cm –2 ) or COPV‐6 (7 ± 1 µJ cm –2 ). [ 29 ]…”
Section: Resultsmentioning
confidence: 59%
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“…The fascinating combination of strong and tunable fluorescence [ 72 , 91 , 96 , 97 ] with high chemical and environmental stabilities [ 30 ] makes GQDs also suitable for optical imaging applications. [ 76 ] Moreover, compared to broad PL spectra due to a wide size distribution of NGs produced by top‐down synthesis, [ 77 , 98 , 99 ] atomically‐precise structures of bottom‐up synthesized GQDs with monodispersed sizes enable extremely narrow PL spectra.…”
Section: Nanographenes: From Structure‐dependent Properties To Applic...mentioning
confidence: 99%
“…[34][35][36] Out of organic compounds emissive in this region nanographenes can be heightened, which are characterized by outstanding photostability. [37,38] Low lasing threshold were determined for different structures, such as donor-π-acceptor type molecules based on benzothiadiazole, [39] pyrrolopyrrole aza-BODIPY, [40] or in perovskites. [41] We have utilized simple single dye-doped polymeric thin films for DFB and RL investigations in this work.…”
Section: Introductionmentioning
confidence: 99%