| Literature DB >> 28932672 |
Yameng Ren1,2, Jiao Liu1,2, Aibin Zheng3, Xiandui Dong1, Peng Wang3.
Abstract
Continuous studies on the use of a polycyclic aromatic hydrocarbon as the central block of an organic photosensitizer have brought forth a new opportunity toward efficiency enhancement of dye-sensitized solar cells (DSCs). In this paper, a nonacyclic aromatic hydrocarbon 9,19-dihydrodinaphtho[3,2,1-de:3',2',1'-op]pentacene, tethered with four 4-hexylphenyl solubilizing groups is reported. The novel chromophore 9,9-19-19-tetrakis(4-hexylphenyl)-9,19-dihydrodinaphtho[3,2,1-de:3',2',1'-op]pentacene is further functionalized with diarylamines and 4-(7-ethynylbenzo[c][1,2,5]thiadiazol-4-yl)benzoic acid to produce two donor-acceptor (D-A) organic photosensitizers, achieving good power conversion efficiencies up to 10.2% in DSCs.Entities:
Keywords: charge transfer; dyes; excited states; polycyclic aromatic hydrocarbon; solar cells
Year: 2017 PMID: 28932672 PMCID: PMC5604383 DOI: 10.1002/advs.201700099
Source DB: PubMed Journal: Adv Sci (Weinh) ISSN: 2198-3844 Impact factor: 16.806
Figure 1Molecular structures of R1 and R2 characteristic of a polycyclic aromatic hydrocarbon DNP, which is filled with the color of cyan.
Scheme 1Synthetic routes to R1 and R2. Reagents and conditions: (i) Pd(OAc)2, Sphos, K3PO4, dioxane/H2O (v/v, 5/1), reflux, 12 h; (ii) (4‐hexylphenyl)magnesium bromide, THF, reflux, 6 h; (iii) Amberlyst 15, toluene, reflux, 6 h; (iv) NBS, THF, R.T., 10 min; (v) bis(4‐(hexyloxy)phenyl)amine, Pd2(dba)3, P(t‐Bu)3, NaOtBu, toluene, reflux, 12 h; (vi) bis(2′,4′‐bis(hexyloxy)‐[1,1′‐biphenyl]‐4‐yl)amine, Pd2(dba)3, P(t‐Bu)3, NaOtBu, toluene, reflux, 12 h; (vii) NBS, THF, R.T., 1 h; (viii) butyl 4‐(7‐ethynylbenzo[c][1,2,5]thiadiazol‐4‐yl)benzoate, Pd2(dba)3, P(t‐Bu)3, Cs2CO3, dioxane, reflux, 12 h; (ix) KOH, THF/H2O (v/v, 3/1), reflux, 9 h; then phosphoric acid; (x) NBS, THF, R.T., 1 h; (xi) butyl 4‐(7‐ethynylbenzo[c][1,2,5]thiadiazol‐4‐yl)benzoate, Pd2(dba)3, P(t‐Bu)3, Cs2CO3, dioxane, reflux, 12 h; (xii) KOH, THF/H2O (v/v, 3/1), reflux, 9 h; then phosphoric acid.
Figure 2a) Cyclic voltammograms of R1 and R2 in THF. Scan rate: 5 mV s−1. Decamethylferrocene (DMFc) was added as the internal reference and all potentials were further calibrated with the standard redox couple ferrocene/ferrocenium (Fc/Fc+). b) Stationary UV–vis spectroscopies of R1 and R2 in THF (10 µm).
Energy levels and photophysical data
| Dye |
|
|
|
|
|
|
|
|
|---|---|---|---|---|---|---|---|---|
| THPDNP | −2.80 | −2.48 | −5.21 | −5.19 | 485 | 465 | / | 16.4 |
| DPA‐THPDNP | −2.84 | −2.52 | −4.94 | −4.93 | 520 | 504 | / | 20.9 |
| DBPA‐THPDNP | −2.86 | −2.54 | −5.04 | −5.02 | 514 | 494 | / | 30.3 |
|
| −3.34 | −3.09 | −4.97 | −4.95 | 572 | 580 | 468 | 56.4 |
|
| −3.34 | −3.09 | −5.05 | −5.03 | 568 | 577 | 1296 | 62.6 |
Electrochemically measured frontier orbital energies (and) versus vacuum are calculated via , herein is the onset oxidation and reduction potentials (Figure 2a and Figure S2a, Supporting Information) of a molecule at the ground‐state in THF. H and L stand for HOMO and LUMO, respectively. Energy levels of LUMO and HOMO (and ) are computed at the B3LYP/6‐311G(d,p) level of theory for a dye molecule in THF. Maximum absorption wavelength () and maximum molar absorption coefficient () are derived from electronic absorption spectroscopies of THF solutions. Maximum absorption wavelength () is calculated at the TD‐MPW1K/6‐311G(d,p) level of theory for a dye molecule in THF. The equilibrium excited state lifetimes () are derived from Figure S6 (Supporting Information).
Figure 3a,b) Up‐converted PL traces probed at 850 nm of dye molecules grafted on mesoporous alumina and titania films. The grey fitting lines are also included. Pump wavelength: 490 nm; pulse fluence: 28 µJ cm−2.
Figure 4a,b) Absorption transients of dye‐grafted titania films in combination with an inert electrolyte made from 0.5 m TBP and 0.1 m LiTFSI in acetonitrile and a Co‐bpy electrolyte. Excitation wavelength: 629 nm for R1/inert; 621 nm for R2/inert; 630 nm for R1/Co‐bpy; 626 nm for R2/Co‐bpy. Probe wavelength: 785 nm. Pulse fluence: 20 µJ cm−2. The solid gray lines are multiexponential fittings.
Figure 5a) External quantum efficiencies (EQEs) at a set of wavelengths (λ) of incident monochromatic lights for dyes R1 and R2 self‐organized on the surface of a bilayer film [(4.5+5.0) µm thick] of mesoporous and microporous titania. b) Wavelength‐dependent light‐harvesting yields (φ) for a single layer (8.0 µm thick) of mesoporous titania grafted with dye molecules. c) Current–voltage (J–V) curves recorded under the simulated AM1.5G sunlight (100 mW cm−2). The aperture area of black metal mask: 0.160 cm2. d) Dependence of open‐circuit photovoltage (V) on short‐circuit photocurrent density (J). The solid fitting lines are also included. e) Charge extracted from a dye‐grafted titania film (Q) as a function of open‐circuit photovoltage (V). f) Plots of half‐lifetime () of electrons in the conduction band and traps under the conduction band of titania versus Q.
Photovoltaic parameters of four cells measured under the simulated AM1.5G sunlight (100 mW cm−2)
| Dye |
|
| V | FF [%] | PCE [%] |
|---|---|---|---|---|---|
|
| 14.59 ± 0.08 | 14.47 ± 0.09 | 867 ± 2 | 74.6 ± 0.2 | 9.4 ± 0.2 |
|
| 14.03 ± 0.04 | 14.00 ± 0.03 | 948 ± 3 | 77.2 ± 0.1 | 10.2 ± 0.1 |
was computed via wavelength integration of the product of the EQE curve measured at the short‐circuit and the standard AM1.5G emission spectrum (ASTM G173‐03).