2019
DOI: 10.1016/j.electacta.2018.12.066
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Three-dimensional high-rate electropolymerized thin film with exceptionally high photocurrent based on a triphenylamine-containing ruthenium complex

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Cited by 14 publications
(13 citation statements)
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“…Stable and rapidly responding photocurrents were observed and monotonically increased as the biases became more negative from +0.6 to −0.4 V versus SCE, indicating that interfacial electron transfer occurred from thin-film-modified ITO to electrolyte solution and the photocurrents generated by the films were the cathode photocurrent, which is similar to the behaviors of some Ru­(II)-complex-based electrostatic self-assembled films previously reported. , It was found that the maximum photocurrent (photocurrent densitiy) of 2.66 μA (9.6 μA/cm 2 ) was achieved at −0.4 V for the poly­( L ) 1 film. In comparison to Table , it is worth mentioning that a significant cathode photocurrent density of 2.2 μA/cm 2 at a bias potential of 0 V was observed for the poly­( L ) 1 film, which outperforms or is comparable to those previously reported for some representative molecule-based thin films under similar experimental conditions. ,,,,,,, …”
Section: Resultssupporting
confidence: 70%
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“…Stable and rapidly responding photocurrents were observed and monotonically increased as the biases became more negative from +0.6 to −0.4 V versus SCE, indicating that interfacial electron transfer occurred from thin-film-modified ITO to electrolyte solution and the photocurrents generated by the films were the cathode photocurrent, which is similar to the behaviors of some Ru­(II)-complex-based electrostatic self-assembled films previously reported. , It was found that the maximum photocurrent (photocurrent densitiy) of 2.66 μA (9.6 μA/cm 2 ) was achieved at −0.4 V for the poly­( L ) 1 film. In comparison to Table , it is worth mentioning that a significant cathode photocurrent density of 2.2 μA/cm 2 at a bias potential of 0 V was observed for the poly­( L ) 1 film, which outperforms or is comparable to those previously reported for some representative molecule-based thin films under similar experimental conditions. ,,,,,,, …”
Section: Resultssupporting
confidence: 70%
“…On the basis of the data shown in Figure c and eqs and of Laviron’s theory, the k s value could be calculated where α is the electron transfer coefficient and ν a and ν c are the critical scan rates, which were obtained to be ν a = ν c = 0.1429 V/s by linearly fitting the anodic and cathodic data of Figure c, respectively. An apparent k s value of the poly­( L ) 1 film was determined to be 5.66 s –1 , which is greater or comparable to k s values previously reported for Ru III/II -associated redox reactions in a [(H 2 L 1 )­Ru­(H 2 L 2 )­Ru­(H 2 L 1 ) 2 ]­(ClO 4 ) 4 {H 2 L 1 = 2,6-bis­(2-benzimidazolyl)­pyridine; H 2 L 2 = 2,6-bis­(4-([2,2’:6′,2″-terpyridin]-4′-yl)­phenyl)-1,5-dihydrobenzo­[1,2- d :4,5- d ′]­diimidazole}-based drop-casting film (3.1 s –1 ) and a [Ru­(bpy) 2 (Hdppip)]­(ClO 4 ) 2 {Hdppip = 2-(2,6-di­(pyridin-2-yl)­pyridine-4-yl)-1 H -imidazo­[4,5- f ]­[1,10]­phenanthroline}-based electrostatic film with graphene oxide (5.5 s –1 ) and 17-fold as fast as a value of 0.33 s –1 that we recently reported for a TPA •+1/0 -associated redox reaction in an electropolymerized film poly­[Ru­(ppip) 3 ] 1 {ppip = N -phenyl- N -(4-(1-phenyl-1 H -imidazo­[4,5- f ]­[1,10]­phenanthrolin-2–2-ylphenyl)­benzenamine} . As shown in Figure d, the corrected k s value was calculated to be 5.89 s –1 by replacing E p – E ° with solution ohmic drop E p – E ° – iR s , which was very close to the apparent k s value, where R s is the solution resistance measured by electrochemical impedance spectroscopy (EIS) to be 29.1 Ω.…”
Section: Resultssupporting
confidence: 68%
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