2013
DOI: 10.1016/j.orgel.2013.06.015
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Improving device efficiencies of solid-state white light-emitting electrochemical cells by adjusting the emissive-layer thickness

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Cited by 52 publications
(21 citation statements)
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“…Although the above discussion was limited to device data recorded at steady-state, we emphasize that microcavity effects most probably are in play also during the dynamic turn-on process depicted in Figs 1 – 3 . However, it should be noted that a corresponding temporal simulation would be more cumbersome to perform, owing to the evolution of the doping structure, with concomitant temporal changes in the refractive indices of the constituent materials and the position of the excitons 24 , 31 , 45 , 46 .…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Although the above discussion was limited to device data recorded at steady-state, we emphasize that microcavity effects most probably are in play also during the dynamic turn-on process depicted in Figs 1 – 3 . However, it should be noted that a corresponding temporal simulation would be more cumbersome to perform, owing to the evolution of the doping structure, with concomitant temporal changes in the refractive indices of the constituent materials and the position of the excitons 24 , 31 , 45 , 46 .…”
Section: Resultsmentioning
confidence: 99%
“…However, although the electrical tolerance of LECs to the active-layer thickness has been well established through, e.g., the successful operation of mm-wide planar devices at a few volts drive voltage 22 , 23 , the corresponding optical dependence is less studied and comparatively poorly understood 24 , 25 . It has been demonstrated that losses due to doping-induced self-absorption become increasingly prominent as the active-layer thickness increases 26 , 27 , while an enhanced emission color or efficiency has been attributed to scattering 28 , 29 , microcavity 30 , 31 , and waveguide-coupling effects 32 .…”
Section: Introductionmentioning
confidence: 99%
“…3c (TPA-DCPP). We observe that the EL spectrum is relatively invariant to the viewing angle for all three optimized TADF-LECs, which implies that emission-shifting cavity effects are essentially non-existent for this specific device architecture and active-material thickness 5860 . This conclusion is supported by the luminous intensity distribution depicted in Supplementary Fig.…”
Section: Resultsmentioning
confidence: 87%
“…Determining the recombination zone position by fitting the measured EL spectra to the simulated EL spectra calculated from the optical mode density within am icrocavity structure has been employedt os tudy the device physics of LECs. [16,18,26,29,[55][56][57][58] The equation expressing the spectral modification by microcavity effect of the device optical structure is shownb elow [Eq. (1)]: [59] jE ext l ðÞ j 2 ¼ where R 1 (l)a nd R 2 (l)a re the reflectances from the cathode (silver electrode) and the anode (ITO/glass), respectively, f 1 (l) and f 2 (l)a re the phase changes on reflection from the cathode and the anode,r espectively, T 2 (l)i st he transmittance from the ITO/glass substrate, L is the total opticalt hickness of the cavity layers, j E int (l) j 2 is the emission spectrum of the molecules without the microcavity effect, j E ext (l) j 2 is the output emission spectrum affected by the microcavity effect, and z i is the optical distance between the emittings ublayer i and the cathode.…”
Section: Electroluminescent Characteristics Of Lecsmentioning
confidence: 99%