2 research outputs found
Angular-Shaped 4,10-Dialkylanthradiselenophene and Its Donor–Acceptor Conjugated Polymers: Synthesis, Physical, Transistor, and Photovoltaic Properties
An angular-shaped and isomerically
pure 4,10-diÂ(2-octyl)ÂdodecylÂanthradiselenophene
(aADS) was successfully developed. The expedient synthesis to form
the framework of aADS with two lateral side chains regioselectively
at its 4,10-positions is via a base-induced propargyl–allenyl
isomerization/6Ď€-electrocyclization/aromatization protocol.
This pentacyclic distannylated aADS unit was then copolymerized with
dithienylÂdiketopyrrolopyrrole (DPP) and dithienyl-5,6-difluoro-2,1,3-benzothiadiazole
(DTFBT) acceptors with different alkyl side chains to afford four
donor–acceptor copolymers: PaADSDPP, PaADSDTFBT-C<sub>4</sub>, PaADSDTFBT-C<sub>8</sub>, and PaADSDTFBT-C<sub>8</sub>C<sub>12</sub>. UV–vis spectroscopy and cyclic voltammetry revealed that
PaADSDPP has the narrowest energy band gap, and PaADSDTFBT-C<sub>8</sub>C<sub>12</sub> has larger band gap than PaADSDTFBT-C<sub>4</sub> and
PaADSDTFBT-C<sub>8</sub>. Two layer ONIOM (our own <i>n</i>-layered integrated molecular orbital and molecular mechanics) calculations
were implemented to investigate the disparity in optical, electrochemical,
and device properties between these polymers. Both experimental and
theoretical data suggest that the aliphatic side chains play a significant
role in determining the physical, transistor, and photovoltaic properties
of the polymers. PaADSDTFBT-C<sub>4</sub> and PaADSDTFBT-C<sub>8</sub> exhibited organic-field-effect-transistor hole mobilities of 2.7
× 10<sup>–2</sup> and 1.0 × 10<sup>–2</sup> cm<sup>2</sup> V<sup>–1</sup> s<sup>–1</sup>, greatly
outperforming that of PaADSDTFBT-C<sub>8</sub>C<sub>12</sub> with
a mobility of 5.4 × 10<sup>–6</sup> cm<sup>2</sup> V<sup>–1</sup> s<sup>–1</sup>. Polymer solar cells were fabricated
on the basis of ITO/PEDOT:PSS/polymer:PC<sub>71</sub>BM/Ca/Al configuration.
The efficiency decreased as the increase of bulkiness of the aliphatic
side chains installed on DTFBT units (4.4% for PaADSDTFBT-C<sub>4</sub>, 3.5% for PaADSDTFBT-C<sub>8</sub>, 0.3% for PaADSDTFBT-C<sub>8</sub>C<sub>12</sub>). Atomic force microscopy images reveal that the degree
of aggregation for the polymer:fullerene blends is influenced significantly
by the bulkiness of aliphatic side chain installed on DTFBT. Noticeable
aggregation was found for the PaADSDTFBT-C<sub>8</sub>C<sub>12</sub>:PC<sub>71</sub>BM blend. These results are in good agreement with
the computational results elucidating that the intermolecular interactions
between the polymers and PC<sub>71</sub>BM are sterically hindered
by the bulky 2-octyldodecyl groups. This work not only presents a
promising selenophene-based aADS building block but also provides
insights into the side-chain engineering for donor–acceptor
conjugated copolymers
A New Ladder-Type Germanium-Bridged Dithienocarbazole Arene and Its Donor–Acceptor Conjugated Copolymers: Synthesis, Molecular Properties, and Photovoltaic Applications
We
have developed a new germanium-bridged heptacyclic arene, dithienogermolocarbazole
(DTGC), in which two outer thiophene subunits are covalently fastened
to the central 2,7-carbazole core by two dibutylgermanium bridges.
The germole moieties embedded in the DTGC structure were successfully
constructed by one-pot nucleophilic cyclization in a high yield of
88%. Because of the relatively lower polarity of carbon–germanium
bonds, the DTGC unit is chemically stable under basic conditions,
rendering its more versatile functionalization. Comparison of germanium-bridged
DTGC with the carbon-bridged DTCC (dithienocyclopentacarbazole) and
silicon-bridged DTSC (dithienosilolocarbazole) analogues reveals that
the HOMO energy level of DTGC lies between those of DTCC and DTSC
and so does the LUMO energy level of DTGC. Density functional theory
(DFT) calculations suggest that DTSC and DTGC have more bent structures
than DTCC, which plays an important role in determining their frontier
orbital energies. The structural disparity could be amplified in their
corresponding polymers. The DTGC unit was copolymerized with four
different comonomers, including benzothiadiazole (BT), dithienylbenzothiadiazole
(DTBT), difluorobenzothiadiazole (FBT), and dithienyldifluorobenzothiadiazole
(DTFBT) to yield a series of new alternating donor–acceptor
copolymers, polyÂ(dithienogermolo-carbazole-<i>alt</i>-benzothiadiazole)
(PDTGCBT), polyÂ(dithienogermolocarbazole-<i>alt</i>-dithienylbenzothiadiazole)
(PDTGCDTBT), polyÂ(dithienogermolocarbazole-<i>alt</i>-difluorobenzothiadiazole)
(PDTGCFBT), and polyÂ(dithienogermolocarbazole-alt-dithienyldifluorobenzothiadiazole)
(PDTGCDTFBT). Because of the two additional thiophene rings in the
repeating units on the backbone to facilitate π-electron delocalization,
PDTGCFDTBT showed a lower optical band gap than PDTGCFBT. Furthermore,
PDTGCDTFBT also showed the lower-lying LUMO and HOMO energy levels
than PDTGCDTBT as a result of the electron-withdrawing fluorine atoms.
Consequently, the bulk heterojunction solar cell incorporating PDTGCDTFBT
delivered the highest performance with <i>V</i><sub>oc</sub> of 0.84 V, <i>J</i><sub>sc</sub> of 9.87 mA/cm<sup>2</sup>, FF of 48.8%, and PCE of 4.05%. By adding 3 vol % 1-chloronaphthalene
to tailor the morphology, the solar cell using PDTGCDTFBT with higher
molecular weight exhibited the improved efficiency of 4.50% with a <i>V</i><sub>oc</sub> of 0.84 V, a <i>J</i><sub>sc</sub> of 11.19 mA/cm<sup>2</sup>, and an FF of 47.7%