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rsc.li/polymers
Polymer Chemistry
www.rsc.org/polymers
ISSN 1759-9954
PAPERMunju Goh et al.Enhancement of the crosslink density, glass transition temperature, and strength of epoxy resin by using functionalized graphene oxide co-curing agents
Volume 7 Number 1 7 January 2016 Pages 1–246
Polymer Chemistry
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Wang, Y. Lin, C. Tang, J. Dou, H. Tan, Q. Zheng, C. Ma and Z. Cui, Polym. Chem., 2017, DOI:
10.1039/C6PY02161A.
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ARTICLE
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a. Printable Electronics Research Center, Suzhou Institute of Nano-Tech and Nano-
Bionics, Chinese Academy of Sciences, Collaborative Innovation Center of Suzhou
Nano Science and Technology, 398 Ruoshui Road, SEID SIP, Suzhou, Jiangsu
215123, PR China. Email: [email protected] b. College of Chemistry, Beijing Normal University, No. 19, XinJieKouWai St., HaiDian
District, Beijing, 100875, PR China. c. Department of Chemistry, Xi’an Jiaotong Liverpool University, 111 Ren Ai Road,
SEID SIP, Suzhou, 215123, P. R. China. d. State Key Laboratory of Structure Chemistry, Fujian Institute of Research on the
Structure of Matter, Chinese Academy of Sciences, 155 Yangqiao West Road,
Fuzhou, Fujian 350002, P. R. China e. University of Chinese Academy of Sciences, Beijing, 100049, P. R. China.
† Footnotes rela)ng to the )tle and/or authors should appear here.
Electronic Supplementary Information (ESI) available: [details of any
supplementary information available should be included here]. See
DOI: 10.1039/x0xx00000x
Received 00th January 20xx,
Accepted 00th January 20xx
DOI: 10.1039/x0xx00000x
www.rsc.org/
Peripherally Diketopyrrolopyrrole-Functionalized Dendritic
Oligothiophenes – Synthesis, Molecular Structure, Properties and
Applications
Wei Gao,a,e
Qun Luo,a Junkai Wang,
b Yi Lin,
c Changquan Tang,
d Junyan Dou,
a Hongwei Tan,*
b
Qingdong Zheng,d
Chang-Qi Ma,*a
Zheng Cui*a
Three-dimensional π-conjugated dendrimers are a class of structure defined macromolecules for use in organic
electronics. Herein, a new family of dendritic oligothiophenes (DOT-p-DPPs) that functionalized with diketopyrrolopyrrole
group at the periphery were synthesized by a precise stepwise approach. The chemical structure and the monodispersed
nature of these DOT-p-DPPs were confirmed by NMR, MALDI-TOF MS, HR MS, and GPC measurements. UV-vis absorption
and fluorescence spectra, and cyclic voltammetry of these compounds were also measured. Small band gaps (~ 1.8 eV)
and almost identical HOMO/LUMO energy levels (-5.2/-3.5 eV) were measured for these DOT-p-DPPs independent to the
molecular size. However, the molecular molar extinction coefficient (ε) of DOT-p-DPP was found to be linearly correlated
with the number of terminal DPP units, and high ε of 3.6×105 cm
-1·L·mol
-1 was measured for the bigger molecules. These
results in combination with the theoratical calculation results confirm that the frontier molecular orbitals are mostly
localized over the periphery DPP units. Applications of DOT-p-DPPs in organic solar cells as the electron donor are
presented. However, unfavorable nanophase separation and lower DOT-p-DPP content in the blended films led to poor
device performance. Two photon absorption cross section of these DPP decorated dendrimers was measured, and high
cross section values of over 2000 GM were measured for these dendritic molecules, among which, the G1 dendrimer 6T-p-
DPP with a high TPA cross section value close to 7000 GM was achieved.
1. Introduction
Conjugated polymers and small molecules are among the
most widely investigated organic semiconducting materials for
use in organic electronics.1 Among which, conjugated polymers
are considered having advantages of superior film-forming
ability, good processability, and high device performance.
However, polymeric materials possess its inherent drawbacks,
including wide molecular weight distributions, poor
regioregularity control, and undesired end group effects,
which usually affect the optical and electronic properties of
the materials a lot, and consequently lead to a poor batch-to-
batch reproducibility in device application.2 Conjugated small
molecules, on the other hand, possess well-defined and
monodispersed molecular structure, which are considered
having advantages of good reproducibility in device
application.3 In addition, for their controllable and defined
molecular structure, conjugated small molecules are also often
used as model compounds for structure–property-
performance relationship studies.4 However, conjugated small
molecules have also drawbacks of strong crystallization
tendency in solid films, which brings difficulties in thin film
deposition and poor thermal stability in device application.2a, 2c
Conjugated dendrimers that are composed of conjugation
moieties over the molecular skeleton are a new type of
polymers with three-dimensional hyperbranched molecular
structures.5 Unlike conjugated polymers, conjugated
dendrimers have defined and controllable molecular structure
owing to their precise step-by-step synthesis approach.6 In
addition, high-generation conjugated dendrimers could have
molecular weight as high as 10,000 Da.7 Therefore, conjugated
dendrimers are a kind of structure defined macromolecules,
which is expected to have both advantages of good
processibility of polymers and good reproducibility of small
molecules.3a, 8
Till now, conjugated dendrimers based on
benzene,9 thiophene
10 and carbazole unit
11 have been
synthesized and investigated, among which thiophene based
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ones, named also dendritic oligothiophenes (DOTs) are highly
interesting in organic electronics for their unique optical and
electronic properties originating from the extended π-
conjugation chain.12
Not only the all-thiophene dendrons and
dendrimers have been synthesized and characterized,6b, 10c
dendritic oligothiophenes functionalized at the core,13
the
branching π-bridge,14
and at the periphery7, 15
were also
developed. Various functional groups, including porphyrin,13a
dibenzo-4,4-difluoro-4-bora-3a,4a-diaza-s-indacene (dibenzo-
BODIPY),16
pyridine or methylpyridinium,13b
perylenediimide
derivatives (PDI),17
benzothiadiazole (BT),13c
bisthienoimidazoles,18
pyrazino[2,3-g]quinoxaline,19
squaraine
(SQ),20
fluorenyl hexa-peri-hexabenzocoronene (FHBC),21
metal
complex,22
anchoring groups,23
or electron donating and
withdrawing groups24
have been introduced for such
molecular modification. Application of these functionalized
dendritic macromolecules in nonlinear optical devices,25
organic electroluminescence devices,15a
organic field effect
transistors,26
organic solar cells,12b
metal nanoparticle
synthesis,23
and in biosensoring15b
have been reported,
demonstrating versatile properties and application aspects of
these thiophene dendrons and dendrimers.
Especially, the all-thiophene dendrons and dendrimers
exhibit quite promising photovoltaic performance in organic
solar cells (OSCs). A power conversion efficiency (PCE) of 1.7%
was achieved for the 42T:PC61BM based device, which was
further improved to 3.5% when using PC71BM as the electron
acceptor.12b, 27
The organic solar cell using branched
quinquethiophene based dendrimer showed also highest PCE
of 3.1% when blended with PC71BM as the acceptor.15d
Knowing that the maximum absorption wavelength of these
all-thiophene dendrimers is around 420 nm, a moderate PCE
of more than 3% confirms that 3D conjugated dendrimers
could be an excellent molecular skeleton for constructing
conjugated molecules for OSCs application. On the other hand,
Zheng et. al first reported that π-conjugated dendritic
structure is able to enhance the two-photon absorption (TPA)
of organic chromophores, and TPA cross-section of 1412 GM
(1GM = 10−50
cm4
s photon−1
) was achieved for a six branched
dendrimers, which is much larger than the conventional single
branched chromophores.28
Since then, various dendrictic
molecules were developed for TPA application, and high TPA cross
section values over 104 GM were reported in the literature.
29
Inspired by the good photovoltaic performances of low band
gap polymers, in this paper, a new family of thiophene
dendrimers decorated with diketopyrrolopyrrole (DPP) groups
at the periphery was synthesized and characterized. Such a
chemical structure modification greatly reduces the optical
band gap and increases the light harvesting ability of the
thiophene dendrimers. The chemical structures of these
molecules were proved by NMR spectroscopic, MALDI-TOF MS
and HR MS. The monodisperse nature of these molecules was
investigated by MALDI-TOF MS and GPC analysis. Optical and
electrochemical properties will be also discussed. Finally,
photovoltaic as well as two-photon absorption properties of
these novel molecules were investigated in detail to obtain a
better understanding of these materials properties.
2. Experimental
2.1. Materials
Chemicals were purchased and used without further
purification: 2,5-bis(2-octyldodecyl)-3,6-bis(thiophen-2-
yl)pyrrolo[3,4-c]pyrrole-1,4(2H,5H)-dione (DPP-H) (Suna Tech
Inc), n-butyl lithium (n-BuLi, 2.4 M in n-hexane, J&K Scientific
LTD), [Ir(OMe)(COD)]2 (COD=1,5-cyclooctadiene) (Strem
Chemicals), 4,4'-Bis(di-tert-butyl)-2,2'-bipyridine (dtbpy)
(Sigma-Aldrich), Pd2(dba)3·CHCl3 (Sigma-Aldrich), HP(t-Bu)3·BF4
(Sigma-Aldrich), N-bromosuccinimide (NBS, Alfa Aesar), K2CO3
(Enox®), K3PO4 (Enox
®), 4,4,5,5-Tetramethyl-1,3,2-
dioxaborolane (HBpin) (Sigma-Aldrich). Solvents were purified
and dried by usual methods prior to use and typically used
under inert gas atmosphere.30
PC61BM was purchased from
Solarmer Energy, Inc. (Beijing).
2.2. Instruments and measurements
Nuclear magnetic resonance (NMR) spectra were
recorded on a Bruker Avance III 400 spectrometer (1H NMR:
400 MHz, 13
C NMR: 100 MHz). Chemical shifts are denoted in δ
(ppm), and were referenced to tetramethylsilane (TMS) via the
residual non-deuterated solvent peaks (CDCl3: 1H NMR: 7.26
ppm, 13
C NMR: 77.0 ppm; C2D2Cl4: 1H NMR: 6.00 ppm,
13C
NMR: 74.0 ppm) as internal standard. The splitting patterns
are designated as follows: singlet (s), doublet (d), triplet (t),
and multiplet (m). Matrix assisted laser desorption/ionization
time-of-flight mass spectrometry (MALDI-TOF MS) were
performed on a Bruker Autoflex Speed using trans-2-[3-(4-tert-
butylphenyl)-2-methyl-2-propenylidene] malononitrile (DCTB)
as the matrix. High resolution mass spectrometry (HR MS) was
performed on a Bruker ultrafleXtreme MALDI-TOF/TOF
(operation mode: MALDI; matrix: DCTB). Gel permeation
chromatography (GPC) measurement was performed on a
Waters Breeze separations module apparatus with THF as the
eluent (flow rate 1mL min-1
, 35 ºC). Number-average molecular
weight (Mn) and polydispersity index (Mw/Mn) of compounds
were determined by GPC analysis relative to polystyrene
standards. UV-vis spectra of these new materials in chloroform
(CHCl3) solution and thin film were recorded on a Perkin Elmer
Lambda 750 UV-vis Spectrophotometer. For UV-vis absorption
spectrum measurement in solution, three concentrated
solutions (around 10-4
mol·L-1
) were prepared independently,
each of which were further diluted to get three diluted
solutions (with concentration around 10-7
-10-6
mol·L-1
) for UV-
vis absorption measurement. The absorption spectra of the
dilute solutions were recorded, and the data points of the
absorbance at a certain wavelength vs. concentration were
then plotted. A good linear relationship was found for all these
compounds, suggesting no obvious intermolecular interaction
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was found in such a concentration range. The molecular molar
extinction coefficient (ε) was obtained from the slope of the
best-fit line over the above mentioned data points according
to the Beer–Lambert’s Law equation, A = ε·l·c. Thin film
samples for UV-vis spectra measurement were prepared by
spin-casting a chloroform solution on quartz glasses. The
photoluminescence (PL) spectra of the DOT-c-BTs in
chloroform solution were obtained with an F-4600
fluorescence spectrophotometer.
Cyclic voltammetry (CV) experiments were performed
with a RST-3000 Electrochemistry Workstation (Suzhou
Risetech Instrument co., ltd). All CV measurements were
carried out at room temperature with a conventional three-
electrode configuration under nitrogen atmosphere. The
electrochemical cyclic voltammetry was performed in a 0.1 M
tetrabutylammonium hexafluorophosphate (TBAPF6)/dichloro-
methane (DCM) solution with a scan speed of 100mV s−1
. A Pt
disk (ϕ = 1 mm) embedded in Teflon was used as the working
electrode. The surface was polished before use. A Pt sheet (~ 1
cm2) and Ag/AgCl were used as the counter and reference
electrodes, respectively. After the measurement, small
amount of ferrocene was added in the solution and the
ferrocene/ferrocenium (Fc/Fc+) redox couple was measured as
an internal standard. Transmission electron microscopy (TEM)
tests were performed on a Tecnai G2 F20 S-Twin 200 kV field-
emission electron microscope (FEI). Specimens for the TEM
experiments were obtained by transferring the floated blend
films from the water onto the 200 mesh copper grid. Atomic
force microscopy (AFM) measurements were performed by
using a Scanning Probe Microscope-Dimension 3100 in tapping
mode.
For nonlinear optical experiments, the excitation pulse (1
KHz, 240–2600 nm, pulse-width < 120 fs) was generated from
an optical parametric amplifier (TOPAS-F-UV2, Spectra-Physics)
pumped by a regeneratively amplified femtosecond Ti-
sapphire laser system (800 nm, 1 KHz, pulse energy 4 mJ,
pulse-width < 120 fs, Spitfire Pro-F1KXP, Spectra-Physics),
which is seeded by femtosecond Ti-sapphire oscillator (80
MHz, pulse-width < 70 fs, 710–920 nm, Maitai XF-1, Spectra-
Physics). The data were obtained by the two-photon excited
fluorescence method with fluorescein (80 μM in water, pH =
11) as a reference. Two-photon excited fluorescence spectra of
the samples were recorded in THF solution at room
temperature by using an Ocean Optics s2000 spectrometer in
conjunction with a fiber coupler head. The laser beam was
focused by an f = 10 cm lens, and the solution sample in a 1 cm
fluorimeter cuvette (four optically clear windows) was placed
at a fixed distance of ~13.5 cm from the focusing lens.
2.3. Synthesis
3-(5-Bromothiophen-2-yl)-2,5-bis(2-octyldodecyl)-6-
(thiophen-2-yl)pyrrolo[3,4-c]pyrrole-1,4(2H,5H)-dione (DPP-Br):
A solution of N-bromosuccinimide (NBS) (870 mg, 4.89 mmol) in
chloroform (50 mL) was added to DPP-H (4 g, 4.65 mmol) dissolved
in well-degassed chloroform (150 mL) at room temperature under
nitrogen protection. The reaction mixture was protected from light
and stirred at 0 ºC for 4 h, then allowed to warm to room
temperature, and stirred overnight. The reaction mixture was
concentrated to 50 mL, water (100 mL) was added and the mixture
was extracted with chloroform (100 mL x3). The organic layer was
separated and dried over anhydrous sodium sulfate. After the
solvent was removed under reduced pressure, the crude product
was purified by column chromatography on silica gel with
dichloromethane:hexane from 1:9 to 2:3 (v/v). DPP-Br was obtained
as a purple-black solid powder (2.4 g, 55%). 1H NMR (CD2Cl2,
400MHz): δ = 8.85 (d, J = 3.04 Hz; 1H), 8.59 (d, J = 3.64 Hz; 1H), 7.68
(d, J = 4.52 Hz; 1H), 7.28 (dd, J1= 3.96 Hz, J2= 4.96 Hz; 1H), 7.25 (d, J
= 4.2 Hz; 1H), 3.99 (d, J = 7.72 Hz; 2H), 3.92 (d, J = 7.76 Hz; 2H), 1.86
(br; 2H), 1.23-1.29 (m, 64H), 0.84-0.89 ppm (m, 12H).
2-(5-Hexyl-2-thienyl)-4,4,5,5-tetramethyl-1,3,2-dioxaborolane
(B-T): n-BuLi (40 mL, 2.4 M in hexane, 96.0 mmol) was added
dropwise to a solution of 2-hexylthiophene (13.5 g, 80.4 mmol) in
THF (120 mL) at –78 ºC under nitrogen protection, and the reaction
mixture was stirred for 2 h at –78 ºC. 2-isopropyloxy-4,4,5,5-
tetramethyl-1,3,2-dioxaborolane (18 g, 96.8 mmol) was added
dropwise by a syringe and the reaction mixture was allowed to
warm to room temperature slowly and stirred overnight. The
reaction was quenched with saturated aqueous NH4Cl (100 mL) and
the organic layer was separated. The aqueous phase was extracted
with diethyl ether. The combined organic extracts were dried over
Na2SO4. The solvent was removed under reduced pressure to give
the residue, the crude product was purified by column
chromatography on silica gel with hexane to give B-T as yellow oil
(22.5 g, 90%). 1H NMR (CDCl3, 400 MHz): δ = 7.47 (d, J = 3.44 Hz; 1H),
6.86 (d, J = 3.40 Hz; 1H), 2.85 (t, J = 7.48 Hz, 2H), 1.68(quint, J = 7.48
Hz, 2H), 1.33 (s, 12H), 1.27-1.33 (m, 6H), 0.86-0.90 ppm (m, 3H).
3-(5'-Hexyl-(2,2'-bithiophene-5-yl))-2,5-bis(2-
octyldodecyl)-6-(thiophen-2-yl)pyrrolo[3,4-c]pyrrole-
1,4(2H,5H)-dione (DPP-T): Compound DPP-Br (2.0 g, 2.13 mmol),
B-T (1.5 g, 5.10 mmol), [Pd2(dba)3]·CHCl3 (44 mg, 43 μmol), and
HP(tBu)3·BF4 (25 mg, 86 μmol) were dissolved into well-degassed
THF (150 mL). The reaction mixture was bubbled with nitrogen and
a well-degassed aqueous solution of K2CO3 (1M, 12 mL, 12 mmol)
was added dropwise. The reaction mixture was stirred overnight at
room temperature and then poured into water (150 mL) with some
drops of 2 M HCl. The organic layer was separated and the aqueous
layer was extracted with dichloromethane. The combined organic
extracts dried over Na2SO4. The solvent was removed by rotary
evaporation. The residue was filtered through a short column of
silical gel to remove inorganic salts. The filtrate was concentrated
and the resident was purified by SEC column chromatography
eluting with THF to provide DPP-T as purple-dark solid (2.1 g,
94%).1H NMR (CDCl3, 400 MHz): δ = 8.92 (d, J = 4.04 Hz, 1H), 8.84 (d,
J = 3.04 Hz, 1H), 7.60 (d, J = 4.40 Hz, 1H), 7.24-7.27 (dd, 1H), 7.23 (d,
J = 4.12 Hz,1H), 7.14 (d, J = 3.44 Hz, 1H), 6.74(d, J = 3.60 Hz, 1H),
4.03 (d, J = 2.08 Hz, 2H), 4.01 (d, J = 2.00 Hz, 2H), 2.80-2.84 (t,J =
7.40 Hz, 2H), 1.91-1.96 (br, 2H), 1.66-1.74 (quint, J = 7.47 Hz, 2H),
1.21-1.34 (m; 70H), 0.83-0.92 ppm (m,15H); 13
C NMR (CDCl3, 100
MHz): δ = 161.83, 161.56, 147.80, 143.61, 140.30, 139.50, 136.96,
134.91, 133.58, 130.12, 129.97, 128.33, 127.32, 125.32, 124.98,
123.95, 108.20, 107.84, 46.24, 37.90, 37.73, 31.92, 31.88, 31.53,
31.51, 31.32, 31.18, 30.29, 30.05, 30.00, 29.64, 29.55, 29.49, 29.35,
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29.29, 28.74, 26.35, 26.20, 22.68, 22.65, 22.55, 14.10, 14.05 ppm;
MALDI-TOF MS: m/z calcd for C64H102N2O2S3 : 1026.7 ;
found:1026.6.
3-(5-(4,4,5,5-tetramethyl-1,3,2-dioxaborolan-2-yl)thienyl)-2,5-
bis(2-octyldodecyl)-6-(5'-hexyl-[2,2'-bithiophen]-5yl)pyrrolo[3,4-
c]pyrrole-1,4(2H,5H)-dione (B-DPP-T): In glove box, a 5 mL flask was
charged with [Ir(OMe)(COD)]2 (62 mg, 94 μmol, 4%). HBPin (600 mg,
4.68 mmol, 2 eq) was added to the [Ir(OMe)(COD)]2 flask. The
mixture was stirred for 1 min to give a yellow solution. To the
[Ir(OMe)(COD)]2-HBPin mixture was added dtbpy (50 mg, 186 μmol,
8%), and the mixture was stirred for 3 min to give a claret-red
solution. Another 100 mL flask was charged with DPP-T (2.4 g, 2.34
mmol). Dried THF (50 mL) was added to the flask to dissolve the
DPP-T. To the DPP-T solution was added the claret-red catalyst
mixture, and the reaction mixture was stirred at 50 ºC for 30 min.
After the reaction mixture was cooled to room temperature, the
volatile solvent was removed by rotary evaporation. The crude
product was run through a short pad of silica gel column (first
eluting with 3:1 hexane:dichloromethane to remove starting
material, and then eluting with THF to give the pure product B-DPP-
T as deep purple solid (2.3 g, 85%). 1H NMR (CDCl3, 400 MHz): δ =
8.96 (d, J = 4.16 Hz, 1H), 8.85 (d, J = 3.88 Hz, 1H), 7.70 (d, J = 3.84 Hz,
1H), 7.23 (d, J = 4.16 Hz, 1H), 7.14 (d, J = 3.60 Hz, 1H), 6.74 (d, J =
3.60 Hz, 1H), 4.06 (d, J = 7.60 Hz, 2H), 4.02 (d, J = 7.72 Hz, 2H), 2.82
(t, J= 7.56 Hz, 2H), 1.89-1.96 (m, 2H), 1.70 (quint, J= 7.47 Hz, 2H),
1.37 (s, 12H), 1.21-1.34 (m; 70H), 0.83-0.92 ppm (m,15H); 13
CNMR
(CDCl3, 100MHz): δ = 161.84, 161.56, 147.90, 143.88, 140.81,
139.07, 137.62, 137.28, 135.89, 135.60, 133.56, 127.26, 125.34,
125.06, 124.01, 108.84, 108.00, 84.51, 46.28, 46.24, 37.90, 37.76,
31.91, 31.87, 31.52, 31.50, 31.33, 31.26, 30.29, 30.04, 30.02, 30.01,
29.63, 29.58, 29.55, 29.51, 29.35, 29.28, 28.73, 26.36, 26.31, 24.75,
22.68, 22.65, 22.54, 14.10, 14.05 ppm; MALDI-TOF MS: m/z calcd
for C70H113BN2O4S3:1151.8; found: 1151.6.
3T-p-DPP: Compound 3T-I (100 mg, 200 μmol), B-DPP-T (530
mg, 460 μmol), [Pd2(dba)3]·CHCl3 (10 mg, 10 μmol), and
HP(tBu)3·BF4 (8 mg, 27 μmol) were dissolved into well-degassed THF
(10 mL).The reaction mixture was bubbled with nitrogen and a well-
degassed aqueous solution of K2CO3 (1 M, 1.2 mL, 1.2 mmol ) was
added dropwise. The reaction mixture was stirred overnight at
room temperature and then poured into ice water (50 mL) with
some drops of 2 M HCl. The organic layer was separated and the
aqueous layer was extracted with CH2Cl2. The combined organic
extracts were dried over Na2SO4. The solvent was removed by
rotary evaporation to give residue. The residue was purified by
column chromatography on silica gel with chloroform: hexane from
1:4 to 2:3 (v/v). to give the blue solid product (368 mg, 80%). 1H
NMR (CDCl3, 400MHz): δ = 8.94 (d, J = 2.92 Hz, 1H), 8.93 (d, J = 2.96
Hz, 1H), 8.89 (t, J = 4.48 Hz, 2H), 7.34 (d, J = 5.28 Hz, 1H), 7.27 (d, J =
1.04 Hz, 1H), 7.26 (d, 1H), 7.23 (d, J = 3.80 Hz, 1H), 7.21 (d, J = 4.24
Hz, 3H), 7.19 (d, J = 5.28 Hz, 1H), 7.13 (d, J = 3.56 Hz, 2H), 7.11 (d, J =
3.84 Hz, 1H), 7.05 (d, J = 3.84 Hz, 1H), 6.73 (d, J = 3.64 Hz, 2H),
4.02(d, J = 7.00 Hz, 8H), 2.81 (t, J = 7.56 Hz, 4H), 1.96 (br, 4H), 1.70
(quint, J = 7.50 Hz, 4H), 1.21-1.41 (m; 140H), 0.81-0.92 ppm (m,
30H); 13
C NMR (C2D2Cl4, 100MHz): δ = 161.58, 161.48, 148.13,
143.72, 142.24, 141.80, 139.83, 139.68, 138.88, 138.75, 138.16,
137.24, 137.04, 136.98, 136.53, 136.42, 136.03, 135.52, 133.47,
131.59, 131.17, 130.08, 129.10, 128.52, 128.25,127.86, 127.38,
127.36, 125.90, 125.54, 125.24, 124.96, 124.74,123.97, 108.63,
108.51, 108.14, 46.31, 37.96, 32.03, 31.993, 31.987, 31.63, 31.58,
31.47, 30.38, 30.17, 29.78, 29.74, 29.67, 29.49,29.42, 28.89, 26.49,
22.83, 22.80, 22.70, 14.32, 14.28 ppm; MALDI-TOF MS: m/z calcd
for C140H208N4O4S9:2297.4; found: 2297.0; HR MS: m/z calcd for
C140H208N4O4S9: 2297.3682; found: 2297.3665.
B-3T-p-DPP: In glove box, a 5 mL flask was charged with
[Ir(OMe)(COD)]2 (30.0 mg, 45.0 μmol, 4%). HBPin (2.70 g, 2.10 mmol,
2 eq) was added to the [Ir(OMe)(COD)]2 flask. The mixture was
stirred for 1 min to give a yellow solution. To the [Ir(OMe)(COD)]2
and HBPin mixture was added dtbpy (25.0 mg, 93.0 μmol, 8%), the
mixture was stirred for 3 min to give a claret-red solution. In
another 250 mL flask was charged with 3T-DPP (2.48 g, 1.08 mmol),
dried THF (100 mL) was added to the flask in order to dissolve the
3T-p-DPP. To the 3T-p-DPP solution was added the resulting claret-
red catalyst mixture, and the reaction mixture was stirred at 50 ºC
for 30 min. After the reaction mixture was cooled to room
temperature, the volatile solvent was removed by rotary
evaporation. The crude product was run through a short pad of
silica gel column (first eluting with DCM/hexane (1:3) to remove
starting material 3T-p-DPP, and then eluting with THF to give the
product as a blue solid (2.30 g, 88%).1H NMR (CDCl3, 400 MHz): δ =
8.94 (d, J = 2.76 Hz, 1H), 8.93 (d, J = 2.76 Hz, 1H), 8.90 (d, J = 4.16 Hz,
1H), 8.88 (d, J = 4.16 Hz, 1H), 7.68 (s, 1H), 7.28 (d, J = 1.96Hz, 1H),
7.27 (d, J = 1.96 Hz, 1H), 7.21-7.23 (m, 4H), 7.13-7.14 (m, 3H), 7.06
(d, J = 3.80 Hz, 1H), 6.73(d, J = 3.56 Hz, 2H), 4.03 (d, J = 7.16 Hz, 8H),
2.81 (t, J = 7.54 Hz, 4H), 1.96 (br, 4H), 1.66-1.73 (quint, J = 7.45 Hz,
4H), 1.38 (s, 12H), 1.21-1.33 (m; 140H), 0.81-0.92 ppm (m, 30H); 13
C
NMR (CDCl3, 100 MHz): δ = 161.60, 161.52, 161.48, 147.74, 147.71,
143.55, 143.45, 142.14, 141.58, 139.85, 139.68, 138.95, 138.73,
138.01, 137.81, 137.56, 136.97, 136.87, 136.48, 136.32, 135.44,
133.62, 132.47, 128.76, 128.60, 128.24, 127.81, 127.41, 127.37,
125.29, 124.99, 124.92, 124.90, 124.68, 123.94, 108.57, 108.43,
108.09, 108.06, 84.49, 46.28, 37.89, 31.90, 31.87, 31.85, 31.52,
31.48, 31.32, 31.28, 30.27, 30.03, 29.63, 29.54, 29.35, 29.28, 28.73,
26.34, 26.31, 24.74, 22.67, 22.64, 22.54, 14.09, 14.04 ppm; MALDI-
TOF MS: m/z calcd for C146H219BN4O6S9:2422.5; found: 2423.0.
6T-p-DPP: Compound B-DPP-T (630 mg, 546 μmol), 6T-Br (100
mg, 124 μmol), [Pd2(dba)3]·CHCl3 (10 mg, 10 μmol), and
HP(tBu)3·BF4 (8 mg, 27 μmol) were dissolved into well-degassed THF
(25.0 mL).The reaction mixture was bubbled with nitrogen and a
well-degassed aqueous solution of K2CO3 (1 M, 2 mL, 2 mmol ) was
added dropwise. The reaction mixture was stirred overnight at
room temperature and then poured into water (50 mL) with some
drops of 2 M HCl. The organic layer was separated and the aqueous
layer was extracted with CH2Cl2. The combined organic extracts
dried over Na2SO4. The solvent was removed by rotary evaporation.
The residue was filtered through a short column of silical gel to
remove any inorganic salts. The filtrate was concentrated and
purified by SEC column chromatography eluting with THF to give
the product 6T-p-DPP as a deep blue solid (460 mg, 81%).1H NMR
(CDCl3, 400 MHz): δ = 8.93-8.74 (m, 8H), 7.21 (d, J = 3.52 Hz, 2H),
7.13-7.18 (m, 8H), 7.08 (s, 2H), 7.03 (d, J = 3.04 Hz, 6H), 6.96 (br, 4H),
6.69-6.73 (m, 4H), 3.99 (br, 16H), 2.82 (t, J = 7.58 Hz, 8H), 1.92 (br,
8H), 1.67-1.75 (quint, J = 7.49 Hz, 8H), 1.21-1.41 (m; 280H), 0.80-
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0.94 ppm (m, 60H); 1H NMR (C2D2Cl4, 400 MHz): δ =8.90 (d, J = 3.56
Hz, 4H), δ =8.87 (d, J = 4.16 Hz, 2H), δ =8.84 (d, J = 4.24 Hz, 2H),7.24-
7.28 (m, 10H),7.16-7.18 (m, 8H), 7.13 (d, J = 3.12 Hz, 4H), 6.75 (d, J =
3.40 Hz, 4H), 3.99 (br, 16H), 2.82 (t, J = 7.70 Hz, 8H), 1.94 (br, 8H),
1.67-1.74 (quint, J = 7.50 Hz, 8H), 1.21-1.42 (m; 280H), 0.80-0.94
ppm (m, 60H); 13
C NMR (CDCl3, 100 MHz): δ = 161.15, 160.97,
147.29, 147.27, 143.40, 143.34, 141.57, 141.30, 139.60, 139.46,
138.39, 138.18, 137.57, 137.22, 137.15, 136.75, 136.61, 136.58,
136.37, 136.34, 136.32, 135.33, 134.91, 133.96, 131.37, 130.57,
130.54, 128.75, 128.54, 128.32, 127.80, 127.77, 127.46, 127.45,
126.76, 126.68, 125.25, 125.22, 125.14, 124.82, 124.72, 123.74,
108.23, 108.15, 107.64, 107.62, 46.31, 37.86, 31.96, 31.93, 31.91,
31.62, 31.56, 31.51, 31.39, 30.36, 30.15, 29.74, 29.70, 29.64, 29.61,
29.41, 29.38, 28.89, 26.54, 26.43, 22.70, 22.64, 14.14, 14.11 ppm;
MALDI-TOF MS: m/z calcd for C280H414N8O8S18: 4592.7; found:
4592.6; HR MS: m/z calcd for C280H414N8O8S18: 4592.7202; found:
4592.7496.
9T-p-DPP. Compound 9T-I (50 mg, 40 μmol), B-DPP-T (204 mg,
177 μmol), [Pd2(dba)3]·CHCl3 (5 mg, 5 μmol), and HP(tBu)3·BF4 (4 mg,
14 μmol) were dissolved into well-degassed THF (10 mL). The
reaction mixture was bubbled with nitrogen and a well-degassed
aqueous solution of K3PO4 (1 M, 1 mL, 1 mmol) was added dropwise.
The reaction mixture was stirred overnight at room temperature
and then poured into ice water (10 mL) with some drops of 2 M HCl.
The organic layer was separated and the aqueous layer was
extracted with CH2Cl2. The combined organic extracts dried over
Na2SO4. The solvent was removed by rotary evaporation. The
residue was filtered through a short column of silical gel to remove
any inorganic salts. The filtrate was concentrated and purified by
SEC column chromatography eluting with THF to give the product as
a deep blue solid (126 mg, 62%). 1H NMR (CDCl3, 400 MHz): δ =8.92
(d, J = 4.08 Hz, 4H), 8.89 (d, J = 4.12 Hz, 2H), 8.87 (d, J = 4.16 Hz, 2H),
7.33 (d, J = 5.24 Hz, 1H), 7.22 (s, J = 4.08 Hz, 2H), 7.13-7.20 (m, 12H),
7.03-7.12 (m, 13H), 6.70-6.72 (m, 4H), 3.99 (br, 16H), 2.78-2.82 (m,
8H), 1.94 (br, 8H), 1.65-1.73 (m, 8H), 1.20-1.32 (m; 280H), 0.79-0.92
ppm (m, 60H); 13
C NMR (CDCl3, 100 MHz): δ =161.46, 161.34,
147.62, 147.60, 143.46, 143.40, 141.85, 141.83, 141.50, 141.46,
139.67, 139.60, 138.69, 138.57, 137.45, 137.36, 137.28, 137.23,
137.06, 137.02, 136.60, 136.56, 136.48, 136.27, 136.01, 135.11,
135.01, 134.61, 133.74, 131.77, 131.72, 131.71, 131.20, 130.20,
129.94, 129.86, 128.79, 128.62, 128.59, 128.52, 128.42, 128.02,
127.42, 126.36, 126.12, 125.25, 124.84, 124.72, 124.61, 123.89,
108.48, 108.40, 108.00, 46.29, 37.97, 31.95, 31.92, 31.58, 31.51,
31.39, 31.34, 30.32, 30.11, 29.68, 29.60, 29.40, 29.35, 28.82, 26.42,
26.38, 22.71, 22.70, 22.60, 14.14, 14.08 ppm; MALDI-TOF MS: m/z
calcd for C292H420N8O8S21: 4838.7; found: 4838.8, HR MS: m/z calcd.
for C292H420N8O8S21: (100% abundance) 4842.6906; found:
4842.6917.
18T-p-DPP. Compound B-3T-p-DPP (600 mg, 248 μmol), 6T-Br
(45 mg, 56 μmol), [Pd2(dba)3]·CHCl3 (10 mg, 10 μmol), and
HP(tBu)3·BF4 (8 mg, 27 μmol) were dissolved into well-degassed THF
(20 mL).The reaction mixture was bubbled with nitrogen and a well-
degassed aqueous solution of K3PO4 (1 M, 1.5 mL, 1.5 mmol ) was
added dropwise. The reaction mixture was stirred overnight at
room temperature and then poured into water (50 mL) with some
drops of 2 M HCl. The organic layer was separated and the aqueous
layer was extracted with CH2Cl2. The combined organic extracts
dried over Na2SO4. The solvent was removed by rotary evaporation.
The residue was filtered through a short column of silical gel to
remove any inorganic salts. The filtrate was concentrated and
purified by SEC column chromatography eluting with THF to give
the product as a deep blue solid (351 mg, 65%). 1H NMR (C2D2Cl4,
400 MHz): δ = 8.90 (br, 8H), 8.86 (br, 8H), 7.15-7.34 (m, 54H), 6.76
(br, 8H), 3.99 (br, 32H), 2.82 (br, 16H), 1.93 (br, 16H), 1.70 (m, 16H),
1.21-1.32 (m; 560H), 0.82-0.91 ppm (m, 120H); 13
C NMR (CDCl3, 100
MHz): δ = 161.17, 147.27, 143.26, 141.74, 141.40, 139.40, 138.44,
137.36, 137.19, 136.63, 136.07, 135.05, 133.92, 131.52, 128.60,
128.39, 127.47, 125.12, 124.65, 123.76, 108.20, 107.82, 46.32,
37.99, 31.99, 31.96, 31.63, 31.54, 31.51, 31.41, 30.35,30.18, 29.73,
29.67, 29.44, 29.41,28.92, 26.51, 26.43, 22.75, 22.65, 14.17, 14.11
ppm; MALDI-TOF MS: m/z calcd for C584H838N16O16S42: 9685.4; found:
9684.8, HR MS: m/z calcd for C584H838N16O16S42: (100% abundance)
9685.3664; found: 9685.3677.
21T-p-DPP. Compound B-3T-p-DPP (235mg, 248 μmol), 9T-I (25
mg, 20.1 μmol), [Pd2(dba)3]·CHCl3 (5 mg, 5 μmol), and HP(tBu)3·BF4
(4 mg, 13 μmol) were dissolved into well-degassed THF (20 mL). The
reaction mixture was bubbled with nitrogen and a well-degassed
aqueous solution of K3PO4 (1 M, 1.5 mL, 1.5 mmol) was added
dropwise. The reaction mixture was stirred overnight at room
temperature and then poured into water (50 mL) with some drops
of 2 M HCl. The organic layer was separated and the aqueous layer
was extracted with CH2Cl2. The combined organic extracts dried
over Na2SO4. The solvent was removed by rotary evaporation. The
residue was filtered through a short column of silical gel to remove
any inorganic salts. The filtrate was concentrated and purified by
SEC column chromatography eluting with THF to give the product as
a deep blue solid (123 mg, 63%). 1H NMR (C2D2Cl4, 400 MHz): δ =
8.83 (br, 8H), 8.80 (br, 8H), 7.18-7.40 (m, 60H), 6.79 (br, 8H), 4.04
(br, 32H), 2.87 (br, 16H), 2.01 (br, 16H), 1.77 (m, 16H), 1.21-1.32 (m;
560H), 0.82-0.91 ppm (m, 120H); MALDI-TOF MS: m/z calcd for
C596H844N16O16S45: 9931.3; found:9931.7; HR MS: m/z calcd for
C584H838N16O16S42: (100% abundance) 9931.3293; found: 9931.2081.
2.4. Fabrication and characterization of the organic solar cells
Photovoltaic devices were fabricated with the
configuration of ITO/PEDOT:PSS/DOTs:PC61BM/LiF/Al. The
indium tin oxide (ITO) coated glass substrates were cleaned
sequentially by ultrasonic in detergent, deionized water,
acetone and isopropanol for 30 min each. After an additional
treatment for 30 minutes in ultraviolet-ozone chamber, a thin
layer (30-40 nm) of PEDOT:PSS (Clevios P VP AI 4083, filtered
through 0.45 μm filter) was spin-coated onto each substrate at
3500 rpm for 1 min, the substrates were transferred into a
nitrogen-filled glove box (<0.1 ppm O2 and H2O). After
annealing in a glove box at 124 or 10 minutes, the substrates
was cooled to room temperature. Compound DOTs and
PC60BM were dissolved in chloroform (CF), then stirred for 4h.
The substrates were spin-coated with the solution of DOTs:
PC61BM in chloroform to form the photoactive layer. The
cathode made of LiF (1 nm) and aluminum (100 nm) was
sequentially deposited by vacuum evaporation under high
vacuum (<10-4
pa). The effective area of the devices was 0.09
cm2.
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The current density–voltage (J–V) characteristics was
measured in a N2-filled glove box using a Keithley 2400 source
meter under a simulated AM 1.5G (100 mW cm-2
) sun light
generated by white light from halogen tungsten lamp, filtered
by a Schott GG385 UV filter and a Hoya LB120 daylight filter.
External quantum efficiencies (EQE) were measured under
simulated one sun operation condition using bias light from a
532 nm solid state laser (Changchun New Industries, MGL-III-
532). Light from a 150 W tungsten halogen lamp (Osram
64610) was used as probe light and modulated with a
mechanical chopper before passing the monochromator (Zolix,
Omni-λ300) to select the wavelength. The response was
recorded as the voltage by an I-V converter (DNR-IV Convertor,
Suzhou D&R Instruments), using a lock-in amplifier (Stanford
Research Systems SR 830). A calibrated Si cell was used as
reference. The device for EQE measurement was kept behind a
quartz window in a nitrogen filled container.
3. Results and discussion
3.1 Synthesis and Structure Characterization
Synthesis
2,5-bis(2-octyldodecyl)-3,6-bis(thiophen-2-yl)pyrrolo[3,4-
c]pyrrole-1,4(2H,5H)-dione (DPP-H, scheme S1) is the most
widely used starting materials for synthesizing DPP based
materials. However, DPP-H is not suitable for peripheral
functionalization of DOTs, since DPP-H has two reactive
terminal C-H positions. To solve this problem, α-hexyl-thienyl
group was selected as the terminal blocking group. To ensure
necessary solubility and film-forming properties of the target
dendritic oligothiophenes, 2-octyldodecyl was selected as the
solubilizing group at the N-position of the DPP unit.
Scheme S1 depicts the synthetic route to the key
precursor B-DPP-T (Supporting information Scheme S1). 3-(5-
Bromothiophen-2-yl)-2,5-bis(2-octyldodecyl)-6-(thiophen-2-
yl)pyrrolo[3,4-c]pyrrole-1,4(2H,5H)-dione (DPP-Br) was
synthesized by bromination of DPP-H using 1.1 equivalent N-
bromosuccinimide (NBS), which gave a 55% yield (Scheme S1,
reaction i).31
Reaction of lithiated 2-hexylthiophene (T) with 2-
isopropyloxy-4,4,5,5-tetramethyl-1,3,2-dioxaborolane gave
corresponding boronic ester B-T in 90% yield (Scheme S1,
reaction ii). Suzuki coupling of DPP-Br with B-T by using
[Pd2(dba)3]·CHCl3/HP(tBu)3BF4 as catalyst gave asymmetrical
DPP derivative DPP-T in 94% yield (Scheme S1, reaction iii).
Iridium-catalyzed borylation of DPP-T by using
[Ir(OMe)(COD)]2/dtbpy as catalyst gave the key precursor B-
DPP-T in 85% yield (Scheme S1, reaction iv).32
Scheme 1 depicts the synthetic route to the first
generation dendron 3T-p-DPP and dendrimer 6T-p-DPP.
Palladium-catalyzed Suzuki coupling of diiodinated
terthiophene 3T-I6b
and B-DPP-T (1:2 mol/mol) gave the first
generation 1st
dendron 3T-p-DPP in 80% yield (Scheme 1,
reaction i). Side reactions within the Suzuki coupling reaction
include, 1) homocoupling of B-DPP-T to yield a dimer T-DPP-
DPP-T; 2) homocoupling of 3T-I with a following up Suzuki
coupling with B-DPP-T to give higher order oligomer T-DPP-3T-
3T-DPP-T, which are confirmed by mass-spectrometric analysis
on the crude products (Supporting information Scheme S2 and
Figure S1). Palladium-catalyzed Suzuki coupling of the
tetrabrominated sexithiophene core 6T-Br6b
with four
equivalents of B-DPP-T under the same coupling condition
gave the first generation 1st
DPP-terminated thiophene
dendrimer 6T-p-DPP in a yield of 81% (Scheme 1, reaction ii).
Both 3T-p-DPP and 6T-p-DPP were purified by preparative size-
exclusion chromatography (SEC, Bio-Rad Beads SX1) eluting
with THF. One step further, iridium-catalyzed borylation of 3T-
p-DPP selectively gave the corresponding boronic ester B-3T-p-
DPP (Scheme 1, reaction iii), which is a basic building block for
the construction of higher generational dendrons and
dendrimers.
The 2nd
generation DPP-terminated dendron 9T-p-DPP was
synthesized by Suzuki coupling of the tetraiodinated G2 dendron
9T-I6b
and four equivalents of boroinc ester B-DPP-T in a yield of
62% (Scheme 2, reaction i). The side products were separated
successfully by SEC with THF as eluent. Alternative synthetic route
to 9T-p-DPP was Suzuki coupling of the diiodinated terthiophene
3T-I and the G1 boronic ester B-3T-p-DPP (Scheme 2, reaction ii).
However, side products including 6T-p-DPP and (3T-3T-p-DPP)2
formed (Supporting information Scheme S3) originating from the
homocoupling of B-3T-p-DPP and homocoupling of 3T-I with a
following up Suzuki coupling with B-3T-p-DPP, respectively (Scheme
S3 and Figure S2 in supporting information). Owing to the similar
hydrodynamic molecular volume for these products, it is difficult to
purify the final compound by SEC purification. Only after multiple
Scheme 1. Synthesis of first-generation dendrons (3T-p-DPP, B-
3T-p-DPP) and dendrimer (6T-p-DPP). Reagents and conditions: i)
and ii) [Pd2(dba)3]·CHCl3, HP(tBu)3BF4, K2CO3, THF; iii)
[Ir(OMe)(COD)]2, dtbpy, HBpin, THF.
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SEC column chromatography separation, pure 9T-p-DPP was
obtained in a yield of 64%. The G2 DPP-terminated dendrimer 18T-
p-DPP was synthesized by Suzuki cross coupling of the
tetrabrominated G1 dendrimer 6T-Br with four equivalents of the
G1 boronic ester B-3T-p-DPP in 65% yield (Scheme 2, reaction iii).
Purification of 18T-p-DPP by preparative SEC was found to be much
easier than that of 9T-p-DPP, which was ascribed to large
hydrodynamic molecular volume difference for the product and
side-products.
The 3rd
generation DPP-terminated dendron 21T-p-DPP
was synthesizedby Suzuki cross coupling of the tetraiodinated
G2 dendron 9T-I and four equivalents of the G1 boronic ester
B-3T-p-DPP in 63% yield (Scheme 3). Purification of 21T-p-DPP
was found to be more difficult than that of 18T-p-DPP. On one
hand, the molecular weight of 21T-p-DPP is close to 10,000 Da,
reaching the separation limit for the preparative SEC column
we used. The uncompleted coupled side-products of this
reaction, on the other hand, have similar hydrodynamic
molecular volumes as the product. Nevertheless, the final
compound 21T-p-DPP can be purified by multiple SEC column
chromatography, which was confirmed by the mass
spectrometry (vide infra).
Structural characterization
All these compounds are highly soluble in organic solvent for
their hyperbranched structure and the multiple alkyl side chains on
the DPP units. The chemical structures of the synthesized
compounds were then characterized by 1H NMR,
13C NMR, MALDI-
TOF MS and high resolution MS. Owing to the unsymmetrical
molecular structure of these dendrimers, 1H NMR spectra of these
compounds are rather complicated, especially for the higher-
generation dendrimers. However, characteristic 1H resonance
peaks can be clearly identified for the small molecules. Figure S3
(supporting information) shows the full 1H NMR spectra of DOT-p-
DPPs. As can be seen from Figure S3, all these DOT-p-DPP showed
Scheme 2. Synthesis of second-generationdendron (9T-p-DPP) and dendrimer (18T-p-DPP). Reagents and conditions: i),
ii) and iii) [Pd2(dba)3]·CHCl3, HP(tBu)3BF4, K2CO3, THF.
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characteristic 1H resonance peaks at 4.0 and 1.9 ppm (protons of -
N-CH2-CH-R1(R2) on the DPP unit), 2.8 ppm (protons of Th-CH2-R on
the terminal thiophene unit), 8.9 ppm (Ha and Hb, β-H of the core
thiophene unit next to the DPP units, see more details in
supporting information Figure S3), confirming the successfully
attaching DPP units to the DOT periphery. Except for these
characteristic proton resonances of the terminal DPP units, 1H
resonance peaks of the core dendritic thiophene can be also clearly
seen. Figure S3b depicts the 1H NMR spectra of the small molecules
(3T-p-DPP, 6T-p-DPP, 9T-p-DPP) in aromatic region. For 3T-p-DPP,
except for the characteristic 1H resonance peaks at 8.9 ppm (Ha
and Hb, for the β-H of the core thiophene unit next to the DPP),
characteristic doublet peak couples at δ =7.34, 7.05 ppm (Hc and
Hd) can be clearly distinguished, which are assigned to the α,β-
protons of the central thiophene unit. Such a doublet peak couple
is changed to a single peak at 7.08 ppm for the 6T-p-DPP molecule,
which is reasonable since the central thiophene unit was
homocoupled. Interestingly, all the resonance peaks up-field
shifted for the 6T-p-DPP when compared with 3T-p-DPP, which
could be due to the shielding effect of the conjugated wedge-shape
dendron unit. It is worth noting that 1H NMR of 6T-p-DPP tends to
be broader and featureless, which was ascribed to more intensive
intermolecular interaction. Checking 1H NMR with other deuterated
solvent, such as THF-d8, CD2Cl2, C2D2Cl4, or diluting the solution
could not get a better resolution results. For 9T-p-DPP, a doublet
peak at 7.34 ppm can be also clearly seen, which is ascribed to the
α-proton of the central thiophene unit, confirming a wedge-shape
dendron molecular structure of the 9T-p-DPP. The H resonance
peaks become broader and featureless with the increase of
molecular size (Figure S3d in supporting information), which was
on one hand ascribed to more complicated molecular structure,
and on the other hand to the increased intermolecular interactions.
Nevertheless, 1H NMR peaks for the small molecules confirmed
defined molecular structure of them. In addition, it is fully
confirmed that DPP units were successfully attached to the
periphery of the dendritic oligothiophene core.
To further confirm the chemical structure of these compounds,
mass spectrometry of these compounds was measured by MALDI-
TOF MS and HR MS measurements. Figure 1a shows the MALDI-TOF
MS results of target DPP-functionalized thiophene dendrons and
dendrimers with defined isotopic patterns, and the HR MS results
are shown in supporting information. The obtained MS data of
these compounds are listed in Table 1. For small molecules (3T-p-
DPP, 6T-p-DPP, 9T-p-DPP), the isotopic patterns fit very well to the
simulated spectrometry, both for the MALDI-TOF MS and HR MS
results (See supporting information). For 18T-p-DPP and 21T-p-DPP,
the HR-MS showed broad and featureless spectra, which was
ascribed to the high molecular weight of these two compounds,
which is close to the measurement limit of the instrument.
However, the MALDI-TOF MS clearly showed the isotopic patterns
of these two compounds, which fits very well to the simulated one
(See supporting information). Nevertheless, the MS and NMR
results unambiguously confirmed the chemical structures of the
S
S
S
N
N
O
O
S S
C10H21
C8H17
C10H21
C8H17
S
C6H13
N
N O
O
S
S
C10H21
C8H17
C10H21
C8H17
SC6H13
BO
O
S
S
S
S
S
S
SS
S
I
I
I
I
9T-I
S
S
S
S
S
S
S
SS
N
NO
O
S
S
SC6H13
S
S
S
SS
SS
S
S
S
SS
C10H21
C8H17
C10H21
C8H17 N
N
O
OS
S
S
C6H13
C10H21C8H17
C10 H
21 C8
H17
N
N
O
OS
S
S
C6H13
C10H21C8H17
C10H21 C 8H 17
N
N
O
O
S
S SC6H13
C10H21
C8H17
C10H21
C8H17
N
N
O
O
S S
S
C6H13
C10H21
C8H17
C10H21C8H17
N
NO
O
S
S
SC6H13
C10H21
C8H17
C10H21
C8H17
N
N O
O
S
S
SC6H13
C10H21
C8H17
C10H21
C8H17
N
N
O
OS
S
S
C6H13
C10H21 C 8H 17
C10H21C8H17
B-3T-p-DPP
21T-p-DPP
i 63%
Scheme 3. Synthesis of third-generation dendron (21T-p-DPP). Reagents and conditions: i) [Pd2(dba)3]·CHCl3, HP(tBu)3BF4,
K2CO3, THF.
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synthesized macromolecules. In addition, all these compounds
show one predominant molecular ion peak signal (Figure 1a),
demonstrating an excellent monodispersity of these dendrons and
dendrimers.
Molecular weight properties and polydispersities of these
peripherally DPP-functionalized dendritic oligothiophenes were
further studied by gel permeation chromatography (GPC). The GPC
traces of these compounds are depicted in Figure 1b, and the
calculated average molecular weights as well as the polydispersity
of these compounds are listed in Table 1. Interestingly, wedge-
shaped thiophene dendrons exhibit smaller hydrodynamic volumes
than the corresponding dendrimers with similar molecular weight.
For example, the G2 DPP-terminated dendron 9T-p-DPP has a larger
25.0 27.5 30.0 32.5 35.0 37.5
Inte
nsit
y
Retention Volume(mL)
3T-p-DPP
6T-p-DPP
9T-p-DPP
18T-p-DPP
21T-p-DPP
b)
Figure 1. a) MALDI-TOF mass spectra (matrix: DCTB) of
DOT-p-DPPs, the insertion showed the isotopic patterns
for each compound, which corresponds well to the
simulated one (see supporting information for detail
comparison);b) GPC profile of dendrons and dendrimers
eluting with THF as the solvent.
HOMO LUMO
3T-p-DPP
6T-p-DPP
9T-p-DPP
18T-p-DPP
21T-p-DPP
Figure 2. DFT calculated optimal molecular conformations and
molecular orbital surfaces of the HOMO and LUMO levels of
conjugated dendrimers.
Table 1. HR MS and GPC analysis data of the synthesized DOTs
Compound Formula [M]+
calcd [M]+
founda GPC Analysis Results
Mnb Mw PDI
3T-p-DPP C140H208N4O4S9 2297.3682c 2297.3665
c 2512 2539 1.01
6T-p-DPP C280H414N8O8S18 4592.7207c 4592.7496
c 5405 5529 1.02
9T-p-DPP C292H420N8O8S21 4842.6906d 4842.6917
d 4683 4770 1.02
18T-p-DPP C584H838N16O16S42 9685.3664d 9685.3677
d 10436 11119 1.07
21T-p-DPP C596H844N16O16S45 9931.3293d 9931.2088
d 8577 9458 1.10
aBy HR MS, using DCTB as matrix;
bNumber average molecular weight, calculated against polystyrene standards;
cMonoisotopic
peak; d100% abundance peak.
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retention volume than 6T-p-DPP, although 9T-p-DPP has only three
thiophene units more than 6T-p-DPP, demonstrating a smaller
hydrodynamic volume of 9T-p-DPP. A similar trend was also found
in the TMS-protected all-thiophene dendrons and dendrimers,6b
and this could be ascribed to more condensed molecular structure
wedge-shaped dendrons. For smaller derivatives (3T-p-DPP, 6T-p-
DPP, 9T-p-DPP) investigated by GPC, the PDI indices were almost
constant and ranged from 1.01 to 1.02, indicating a high degree of
defined and monodisperse structures. Much broader GPC traces
were found for 18T-p-DPP and 21T-p-DPP, leading to slightly higher
PDI values of 1.07 and 1.10, respectively. Such a broader GPC trace
was ascribed to formation of aggregates of dendritic molecules,
which was also found in the all-thiophene dendrimers.6b
Molecular simulation
To investigate the molecular geometries and electronic
structures of DOT-p-DPPs, density functional theory (DFT)
calculations were carried out by using the Gaussian 09 program
with B3LYP/6-31G approach. Calculated optimal molecular
conformations and molecular orbital surfaces of the frontier
molecular orbitals (FMOs), including the highest occupied molecular
orbital (HOMO) and the lowest unoccupied molecular orbital
(LUMO) are shown in Figure 2 and the related data are listed in
Table 2. As can be seen in Figure 2, for DOT-p-DPPs, the electron
density distributions of the HOMO and LUMO levels are both
located on the peripheral DPP groups, which is in good accordance
with the cyclic voltammetry results, where both 1st
oxidation and
reduction processes are ascribed to the oxidation and reduction of
DPP units (vide infra). In addition, these results are also in good
agreement with the UV-vis absorption results where the low energy
absorption bands are ascribed to the DPP units. Slightly reduced
optical band gaps were found for the bigger molecules, which could
be attributed to slightly increased π-conjugation systems. The
molecular dimensionality of few nanometers was calculated for all
these compounds. Specially, 18T-p-DPP and 21T-p-DPP have a
molecular dimension of 6-7 nm, respectively, demonstrating
synthesized single molecular organic nanoparticle (supporting
information Figure S4).
3.2 UV-vis absorption and fluorescence spectroscopy
300 400 500 600 700 8000
1
2
3
4
ε
ε
ε
ε / 1
05
cm
L m
ol-
1
Wavelength(nm)
T-DPP-T
3T-p-DPP
6T-p-DPP
9T-p-DPP
18T-p-DPP
21T-p-DPP
a)
0 5 10 15 200
1
2
3
4
5
0 1 2 3 4 5 6 7 8 90
1
2
3
4
21
T-p
-DP
P
18T
-p-D
PP
9T
-p-D
PP
6T
-p-D
PP
3T
-p-D
PP
358 nm
416 nm
636 nm
ε
ε
ε ε / 1
05 c
m L
mo
l-1
Number of thiophene units of the dendritic core
b)
21T
-p-D
PP
18T
-p-D
PP
9T
-p-D
PP
6T
-p-D
PP
636 nm
ε
ε
ε ε / 1
05 c
m L
mo
l-1
Total DPP units
T-D
PP
-T
3T
-p-D
PP
300 400 500 600 700 800 900
0.0
0.2
0.4
0.6
0.8
1.0 T-DPP-T
3T-p-DPP
6T-p-DPP
9T-p-DPP
18T-p-DPP
21T-p-DPP
No
rmalized
Ab
so
rban
ce
Wavelength(nm)
c)
600 650 700 750 800 8500.0
0.2
0.4
0.6
0.8
1.0
Fluorescence Intensity(a.u.)
Wavelength(nm)
T-DPP-T
3T-p-DPP
6T-p-DPP
9T-p-DPP
18T-p-DPP
21T-p-DPP
d)
Figure 3. a) UV-vis spectra of DOT-p-DPPs in chloroform solution (1×10
−6 mol L
−1); b) linear correlation between the
molar excitation coefficients and the number of thiophene units or DPP units in the synthesized dendrons and
dendrimers; c) Normalized UV−Vis absorption spectra ofDOT-p-DPPs thin films; d) normalized fluorescence emission
spectra of DOT-p-DPPs.
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The UV-vis absorption and fluorescence spectroscopy of these
DOT-p-DPPs and the reference compound T-DPP-T were measured,
and the optical data are listed in Table 2. Figure 3a shows the UV-
Vis absorption of these compounds in chloroform solution. As can
be seen from Figure 3a, all compounds exhibit similar absorption
pattern, which can be divided into two parts, a high-energy
absorption band from 300 to 500 nm and a low-energy band from
500 to750 nm. The absorption band of these compounds in short
wavelength range (300-500 nm) was ascribed to the
superimposition of the absorption of the conjugated oligothiphene
unit with different conjugation length, supported by the linear
correlation between the molar extinction coefficient and the total
thiophene number of the dendritic oligothiophene core (Figure 3b),
which is similar to that in all-thiophene dendrons and dendrimers.6b
On the other hand, the molar extinction coefficient of the long
wavelength band (500-750 nm) was also found linearly correlated
to the number of the DPP units rather than the number of the
thiophene units (Figure 3b, insertion). Therefore, such a low-energy
absorption band was ascribed to the absorption of the periphery
DPP units. Owing to the multiple DPP units for the bigger molecules,
high molar extinction coefficient was obtained for these
compounds. Nevertheless, an molar extinction coefficient of 3.6 ×
105 cm
-1 L mol
-1 for both 18T-p-DPP and 21T-p-DPP is a high value
for a structure defined macromolecule. Figure 3c shows the
absorption spectra of the DOT-p-DPPs in thin solid film. In
comparison with the corresponding spectrum in chloroform
solution, the absorption spectrum in thin solid film was found be
broader and red-shifted (Figure 3c), which can be ascribed to the
intensive intermolecular interaction of these molecules in solid
film33
. Optical band gap (Eg) of these compounds determined from
the absorption onset λabsonset
decreases slightly with the increase of
molecular size (Table 2), indicating a slightly extended π-
conjugation chain length of the DPP unit and the α-oligothiophene
chain.7
Fluorescence emission spectra of the peripherally DPP-
functionalized dendritic oligothiophenes in chloroform are
displayed in Figure 3d. As can be seen from here, the reference
compound T-DPP-T showed an emission band peaking at 652 nm.
The emission band for the DOT-p-DPPs red-shifted slightly with the
increase of molecular size, with peak wavelength in the range of
670-680 nm, suggesting a slightly increased π-conjugation system in
these molecules, which is in consistence with the optical band gap
results. Interestingly, the emission wavelength of these dendrimers
was found to be independent of the excitation wavelength, i.e.
excitation on the dendritic thiophene core also leads to the
emission of the DPP units (Figure S5, in supporting information).
These results indicate that the excited energy is more delocalized
over the periphery DPP units rather than within the dendritic
oligothiophene core, suggesting an energy anti-funnel effect within
these molecules. This is different to the behavior of all-thiophene
dendrimers,10c, 25b
where excited state energy is more localized in
the core part of the molecules.
3.3 Redox Properties and Molecular Energy Levels
The electrochemical properties of the DOT-p-DPPs were
investigated by means of cyclic voltammetry (CV) and differential
pulse voltammetry (DPV). Figure 4a shows cyclic voltammograms of
these DOT-p-DPPs, and the DPV curves of these compounds are
shown in Figure S6 in supporting information. The redox potentials
data are listed in Table 2 for comparison. Interestingly, all these
Table 2. Photophysical and electrochemical data of DPP-functionalized dendritic oligothiophenes
λmaxsol
(nm)a
λonsetsol
(nm)a
λmaxem
(nm)b
εsol
[cm-1
L
mol-1
]c
Egopt(sol)
(eV)d
λmaxfilm
(nm)e
λonsetfilm
(nm)e
Egopt(film)
(eV)e,f
Eox10
(V)g,h
Eox20
(V)g,h
Eoxonset
(V) g
Ered0
(V)g,h
Eredonset
(V)g
EHOMO
(eV)i
ELUMO
(eV)j
Egcv
(eV) k
EHOMOcal
(eV)l
ELUMOcal
(eV)l
Egcal
(eV)m
T-DPP-T 623 665 652 58,260 1.86 586 719 1.72 0.30 0.56 0.22 -1.58 -1.50 -5.32 -3.60 1.72 — — —
3T-p-DPP 634 683 670 118,820 1.82 595 752 1.65 0.20 0.30 0.15 -1.63 -1.54 -5.25 -3.56 1.69 -4.81 -2.97 1.84
6T-p-DPP 635 695 681 215,500 1.78 609 766 1.62 0.20 0.34 0.10 -1.60 -1.57 -5.20 -3.53 1.67 -4.79 -3.09 1.70
9T-p-DPP 598 693 683 213,013 1.79 610 756 1.64 0.19 0.31 0.09 -1.59 -1.54 -5.19 -3.56 1.63 -4.90 -3.14 1.76
18T-p-DPP 602 702 685 359,140 1.77 613 758 1.64 0.25n 0.46
n 0.07
n -1.63
n -1.61
n -5.17 -3.49 1.68 -4.75 -3.03 1.72
21T-p-DPP 603 704 686 358,490 1.76 605 738 1.68 0.27o 0.45
o 0.08
o -1.60
o -1.57
o -5.18 -3.53 1.65 -4.76 -3.04 1.72
PCBMp — — — — — — — — — — — — — -5.91 -4.01 — — — —
aIn CHCl3 solution (10
−6mol L
−1);
bThe maxima emission peak with the excitation wavelength;
cExtinction coefficient ε
sol [cm
-1 L mol
-1] in solution was obtained by linear fitting
absorbance vs. concentration at 633 nm; dOptical band gap estimated from the absorption edge in solution, Eg
opt(sol) (eV) = 1240/λonset
sol[nm];
eSpin-coated from CHCl3 solution onto
the quartz;fOptical band gap in solid film, Eg
opt(film) (eV) = 1240/λonset
film [nm];
gCH2Cl2, [M]=1×10
-3 mol L
-1, TBAPF6 (0.1 M), 295 K, V = 100 mV s
-1, versus (Fc
+/Fc);
hdetermined by DPV
measurements; iCalculated from the cyclic voltammograms, ELUMO = –[Eox
onset + 5.10] (eV), where the vacuum energy level of Fc
+/Fc was set as -5.10 eV;
jCalculated from the cyclic
voltammograms, ELUMO = –[Eredonset
+ 5.10] (eV), where the vacuum energy level of Fc+/Fc was set as -5.10 eV;
k Eg
cv = Eox
onset ﹣ Ered
onset (eV);
lB3LYP/6-31G** energies by DFT;
mB3LYP/6-31G** HOMO-LUMO energy gaps;
nCH2Cl2, [M] = 5×10
-4 mol L
-1, TBAPF6 (0.1 M), 295 K, V=100 mV s
-1, versus (Fc
+/Fc);
oCH2Cl2, [M] = 2.5×10
-4 mol L
-1, TBAPF6 (0.1 M), 295 K,
V = 100 mV s-1
, versus (Fc+/Fc);
pfrom ref 35.
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compounds showed one reversible reduction process over the
negative potential range (0 - -2.0 V). The standard reduction
potentials were determined to be around -1.6 V vs. Fc+/Fc, which is
closed to that of the reference compound T-DPP-T. Therefore, such
a reversible reduction process was ascribed to the reduction of the
DPP units. Although the bigger molecules have more DPP units at
the periphery, the anode or cathode peak currents (ipa and ip
c) for
the reduction of DPP normalized to the DOT-p-DPP concentration
were found to be almost identical for all these compounds. This
result suggests that only one of these DPP units was reduced in
such a negative potential range.
The oxidation potentials of these compounds, on the other
hand, were found to be dependent on the molecular structure. For
example, the 1st
generation dendron, 3T-p-DPP displays three
reversible oxidation processes (Eox0 = 0.20, 0.30, and 0.55 V,
respectively) during the positive potential sweeping. For
comparison, the reference compound T-DPP-T showed two
reversible oxidation processes with Eox0 of 0.30 and 0.56 V. For 6T-
p-DPP, two oxidation processes were measured with Eox0 = 0.20,
0.30 V, respectively, which is quite similar to that of 3T-p-DPP.
Knowing that the 1st
oxidation potentials for trimethylsilane
terminated thiophenedendron (3T-Si) and dendrimer (6T-Si) are
0.82 and 0.53 V, respectively,6b
the measured 1st
oxidation
processes was then ascribed to the oxidation of periphery DPP unit
as well. For larger dendrons and dendrimer (9T-p-DPP, 18T-p-DPP
and 21T-p-DPP), the oxidation waves become broader, which could
be due to the fact that these compounds are composed of multiple
π-conjugated moieties. Nevertheless, the first oxidation potential
could be obtained by DPV measurement, which was found to be
negatively shifted with increasing generation of the dendrons and
dendrimers (See supporting information Figure S6). This was
ascribed to the increased π-conjugation length with the increase of
molecular size, which is in accordance with the shift trend of the
UV-Vis absorption band. It worth also to note that, although there is
one reactive α-H at the core thiophene ring in the dendrons (3T-p-
DPP, 9T-p-DPP and 21-p-DPP), neither dimerization nor
electropolymerization was found during positive potential sweeping,
which is unlike the all-thiophene dendrons where electrochemical
dimerization was found for these compounds during CV sweeping.6b
These results further confirmed that oxidation occurred on the
periphery DPP unit, which could not undergo dimerization or
polymerization.
HOMO/LUMO energy levels of these compounds were
determined from the onset oxidation (Eoxonset
) and the onset
reduction potentials (Eredonset
) according to Equation (1) and (2),
EHOMO = - (Eoxonset
+ 5.10) (eV) (1)
ELUMO = - (Eredonset
+ 5.10) (eV) (2)
EgCV
= Eoxonset
- Eredonset
(eV) (3)
whereby Eoxonset
and Eredonset
represent the onset oxidation and the
onset reduction potential value relative to the
ferrocene/ferricenium couple, respectively, for which an energy
level of -5.10 eV versus vacuum was taken.34
Energy levels of these
compounds are listed in Figure 4b. As can be seen here, all these
compounds show similar HOMO-LUMO energy levels almost
independent of the molecular structure. Again, this was ascribed to
the fact the frontier molecular orbitals are mostly localized over the
periphery DPP units.
In comparison with PC61BM,35
all these DOT-p-DPPs showed
higher HOMO and LUMO energy levels. The higher LUMO energy
levels of DOT-p-DPP would enables electron transfer from DOT-p-
DPPs to PCBM after photoexcitation. All these DOT-c-DPPs show
low-lying HOMO levels of -5.1 eV, which could be beneficial for
achieving high VOC when used in organic solar cells.
3.4 Application of these compounds as electron donor in organic
solar cells
Solution-processed bulk heterojunction solar cells with the
conventional device configuration of ITO/PEDOT:PSS/DOT-p-
DPP:PC61BM/LiF/Al (ITO:indium tin oxide; PEDOT:PSS: poly(3,4-
ethylenedioxythiophene):poly(styrenesulfonate); PC61BM: [6,6]-
phenyl-C61-butyric acid methyl ester) were fabricated and
characterized, where the DOT-p-DPPs and PC61BM were used as the
-2.0 -1.5 -1.0 -0.5 0.0 0.5 1.0
18T-p-DPP
I /
µµ µµA
E / V (vs. Fc+/Fc)
21T-p-DPP
3T-p-DPP
6T-p-DPP
9T-p-DPP
a) T-DPP-T
-6
-5
-4
-3
-5.18
21
T-p
-DP
P
-3.53
En
erg
y L
evel(
eV
)
3T
-p-D
PP
6T
-p-D
PP
9T
-p-D
PP
18
T-p
-DP
P
PC
61B
M-3.56 -3.53 -3.56 -3.49
-5.25 -5.20 -5.19 -5.17
-4.01
-5.95
b)
T-D
PP
-T
-3.60
-5.32
Figure 4. a) Cyclic voltammograms of T-DPP-T, 3T-p-DPP, 6T-p-DPP, 9T-p-
DPP (1×10-3
mol L-1
in CH2Cl2), 18T-p-DPP (5×10-4
mol L-1
in CH2Cl2), 21T-p-
DPP (2.5×10-4
mol L-1
in CH2Cl2), tetrabutylammonium hexafluorophosphate
(TBAPF6, 0.1 M), scan rate = 100 mV s-1
versus ferrocene/ferrocenium
(Fc+/Fc); b). Representation of HOMO–LUMO energy levels of selected
dendritic compounds obtained by electrochemical data. The values for
PC61BM are also given for comparison and were taken from reference 35.
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electron donor and acceptor, respectively. The DOT-p-DPP:PC61BM
blended ratio (w/w) was optimized for each compound (see
supporting information for details), and the optimized photovoltaic
performance of the optimized devices are given in Table 3. The
current–voltage (J–V) curves under light illumination and EQE
response spectra of the optimized devices are shown in Figure 5a
and Figure 5b, respectively.
As can be seen from the Table 3, the open circuit voltages(VOC)
for these DOT-p-DPP based devices are in the range of 0.75-0.81 V,
which are slightly higher when compared with the DPP based
polymer based devices.36
The VOC was found to be slightly
decreased with the increase of molecular size, which may be
ascribed to the slightly higher HOMO energy level for the larger
molecules (vide supra). Surprisingly, except for 3T-p-DPP based
device which showed a relative low fill factor (FF) of 0.41, all the
other DOT-p-DPP based devices showed high FF values with a
highest number of 0.69. The high FF was also found for DPP
polymer based devices.36a, 37
However, owing to the low short
circuit current (JSC), all these DPP based devices showed relative low
power conversion efficiency of around 1.0%. EQE spectra reflect
also the low incident photon-to-current efficiency for these cells.
To better understand the reason for the low device
performance, transmission electron microscope (TEM) images of
the blended film were measured. Figure 6 presents TEM images of
the DOT-p-DPPs:PC61BM films fabricated under the optimal
conditions. As can be seen, all blend films displayed obviously large
phase separation. Such an unusual nanophase separation was also
found for DPP polymer:fullerene blended films.38
Such unfavorable
nanophase separation is adverse for the JSC, since photogenerated
excitons cannot be dissociated efficiently and the electrons
generated in the photoactive layer cannot be collected by the
electrode efficiently. It worth also to note that the optimized DOT-
p-DPP:PC61BM blend ratio was found to be 1:4 or 1:5 (except for 3T-
p-DPP, which has an optimized ratio of 2:1), indicating an extreme
low electron donor content in this blended film. Increase the DOT-
p-DPP concentration led to poorer device performance (Supporting
information, Figure S8-S11, Table S2-S5). Such a low electron donor
contents lower the light absorption ability of the photoactive layer,
Table 3. Characterization of bulk heterojunction solar cells containing DPP-functionalized dendritic oligothiophenes as the
donor material and PC61BM as the acceptora.
Donor D:Ab EQEmax
c
(@wavelength[nm])
JSCd
[mA·cm-2
]
VOC
[V]
FF PCEe
[%]
3T-p-DPP 2:1 0.24 (576) 3.77 0.80 0.41 1.24(1.17±0.083)
6T-p-DPPf 1:5 0.17 (605) 2.28 0.81 0.67 1.24(1.18±0.075)
9T-p-DPP 1:4 0.10 (615) 1.75 0.76 0.65 0.86(0.83±0.043)
18T-p-DPP 1:5 0.13 (471) 2.04 0.77 0.59 0.93(0.87±0.058)
21T-p-DPP 1:4 0.14 (460) 1.97 0.75 0.69 1.02 (0.97±0.048)
aWith a standard device structure of ITO/PEDOT:PSS/DOT-p-DPP:PC61BM/LiF/Al;
bD: DOT-p-DPPs, A: PC61BM;
cExternal
quantum efficiencies (EQE) were measured under simulated one sun operation condition using bias light from a 532 nm
solid state laser, dJSC determined by integrating the EQE spectrum with the AM1.5 G spectrum; eAverage from over 8
devices. Tested under illumination of AM 1.5G 100 mW cm−2
; fThermal annealing at 90 °C.
0.0 0.5 1.0
-4
-3
-2
-1
0
1
Cu
rre
nt
de
ns
ity
(m
A/c
m2)
Voltage(V)
3T-p-DPP
6T-p-DPP
9T-p-DPP
18T-p-DPP
21T-p-DPP
a)
400 500 600 700 8000.00
0.05
0.10
0.15
0.20
0.25 3T-p-DPP
6T-p-DPP
9T-p-DPP
18T-p-DPP
21T-p-DPP
EQ
E
Wavelength(nm)
b)
Figure 5. a) J-V curves of the optimized DOT-p-DPP:PC61BM based BHJ
solar cells illuminated under standard AM1.5G conditions (100 mWcm-2
);
b) EQE spectra of the corresponding devices.
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which could be the 2nd
reason for the low JSC of the devices. Surface
morphology of the DOT-p-DPP:PC61BM films were measured by
atomic force microscope, and the results are shown in Figure S12 in
supporting information. For the 3T-p-DPP, 6T-p-DPP and 18T-p-DPP
based films, rather smooth surfaces were measured, suggesting
that morphology on the surface of these films might be different to
that in the bulk, whereas the 9T-p-DPP and 21T-p-DPP films show
large aggregates on the surface, demonstrating a molecular shape
related nanophase separation, which are in good accordance with
the TEM results. Nevertheless, the preliminary results showed that
DOT-p-DPPs could be used as electron donor in organic solar cells.
Further optimization the D:A nanomorphology are still needed to
achieve high device performance.
3.5 Two-Photon Absorption (TPA)
Organic optical materials with large TPA cross section have
attracted increasing attention owing to their applications in two-
photon bio-imaging and two-photon biosensing.29a
Conjugated
dendrimers are recognized as a special type of high performance
TPA materials for its intriguing chemical structures.29a
In
comparison with linear materials, conjugated dendrimers has larger
TPA cross section values owing to a higher density of effective
chromophores in an ordered and confined geometry, strong
interchromophore interactions and efficient intramolecular charge
transfer.39
Therefore, TPA behaviors of the synthesized DPP
decorated thiophene dendrimers were then measured and tested.
TPA cross-sections of the various molecules as a function of
excitation wavelength are shown in Figure 7. For comparison, the
TPA spectra of the reference molecules T-DPP-T and DPP-3T-DPP
with linear structures (see chemical structures in supporting
information, Figure S13) are also shown in Figure7. As shown in
Figure 7, all linear molecules (T-DPP-T and DPP-3T-DPP) have a
small TPA cross-section value of less than 1000 GM. In comparison
with the linear oligothiophenes, DPP-based dendritic
oligothiophenes show significant enhancement in TPA cross-section
values, which could be ascribed to the cooperative enhancement
effect derive from the 3D special dendritic structures,29a with a high
density of effective chromophores as well as stronger
intramolecular and intermolecular interaction among the branched
multichromophores.39, 40
For example, 3T-p-DPP and DPP-3T-DPP
are two configurational isomers with the same molecular weight.
Figure 6. Bright-field TEM images of DOT-p-DPPs:PC61BM blend films. a) 3T-p-DPP; b) 6T-p-DPP; c) 9T-p-DPP; d) 18T-p-DPP; e) 21T-p-DPP.
800 850 900 9500
1000
2000
3000
4000
5000
6000
7000
TP
A C
ros
s-s
ecti
on
s/G
M
Wavelength/nm
T-DPP-T
DPP-3T-DPP
3T-p-DPP
6T-p-DPP
9T-p-DPP
18T-p-DPP
Figure 7. TPA spectra of DPP-functionalized dendritic
oligothiophenes. TPA of the linear model compound T-DPP-T and
3T-DPP-3T were also added for comparison.
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However, 3T-p-DPP with branched structures has substantially
215% larger TPA cross-section values than the corresponding linear
isomer DPP-3T-DPP, which is in accordance with the previous
report.28
The first generation dendron 3T-p-DPP has a TPA cross section
peak value of 2499 GM at λ=810 nm, and the corresponding first
generation dendrimer 6T-p-DPP has a TPA cross section peak value
of 6984 GM, which is 180% larger than the value for 3T-p-DPP. The
increased TPA cross section peak value for 6T-p-DPP, in comparison
with 3T-p-DPP is mainly attributed to the extended conjugation
length. Surprisingly, the TPA cross section peak values have not
increased with increasing generation of molecules with wavelength
in the range from 780 nm to 880 nm. The second generation
dendron 9T-p-DPP has a TPA cross section peak value of 3252 GM
at λ=810 nm, and the corresponding second generation dendrimer
18T-p-DPP has a TPA cross section peak value of 3672 GM. The
phenomenon may be related to the increased steric hindrance
which decreased the orbital overlap of the α−α linkage around
the thiophene chain.41
It should be noted that a large TPA is
attributed to an extended π-conjuated system as well as an
increased intramolecule charge transfer. However, the TPA cross
section peak values have increased gradually with increasing the
generation of DOT-p-DPPs in the wavelength range from 880 nm to
980 nm. 9T-p-DPP has a TPA cross section peak value of 1978 GM at
λ=930 nm, and 18T-p-DPP has a TPA cross section peak value of
2110 GM. The diketopyrrolopyrrole group may be mainly
responsible for the TPA band in the longer wavelength range
considering the relative lower bandgap of the unit. Thus larger
generation of DOT-p-DPPs would exhibit a larger TPA value with the
increasing number of diketopyrrolopyrrole building blocks provided
that their steric hindrance is relatively insignificant. These initial
results clearly demonstrate that peripherally diketopyrrolopyrrole-
functionalized dendritic oligothiophenes are a potentially suitable
class of two-photon absorbing materials.
Conclusion
In summary, a new series of three dimensional
conjugated thiophene dendrons and dendrimers with
peripheral DPP units were synthesized by a step by step
synthesis approach that involves Ir-catalyzed boronation, and
palladium-catalyzed Suzuki cross coupling reaction. All these
peripherally DPP-functionalized DOTs are highly soluble in
common organic solvents, thus facilitating the full structure
characterization, including NMR, MALDI-TOF MS and HR-MS.
Both MS and GPC analysis showed the monodisperse nature of
these molecules. Optical and electrochemical properties
investigation, as well as the theoretical simulation results
confirmed that the frontier molecular orbitals are mostly
localized on the periphery DPP units, which leads to similar
optical band gaps and HOMO/LUMO energy levels for all these
functionalized dendrimers. Applications of these DPP-
functionalized DOTs in organic photovoltaic devices showed a
low performance with power conversion efficiencies around
1%. High FF of more than 0.6 was measured for these DPP
dendrimers, which is similar to that of DPP based polymers.
Unfavorable nanophase separation and low DOT-p-DPP
concentration in the blend films were the main reason for the
low JSC of these devices. In addition, these branched DPP
dendrimers showed very high two photon absorption cross
section, and a clear dendritic effect can be seen from these
results.
Acknowledgements
The authors greatly appreciate the financial supports from the
National Natural Science Foundation of China (Grant No.
21274163, 21573020, 21303252) and Natural Science
Foundation of Jiangsu Province (Grant No. BK20130352). W.G.
and C.-Q.M. would like to thank Prof. Peter Bäuerle and Dr.
Makus Wunderlin (Ulm University, Germany) for their helpful
discussion and HR-MALDI-MS measurement of 3T-p-DPP and
6T-p-DPP. W.G. and C.-Q.M.and J. D. would like to thank Dr.
Ying Wu and Prof. Zhengping Liu (Beijing Normal University,
China) for their help in GPC analysis.
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Page 16 of 17Polymer Chemistry
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View Article OnlineDOI: 10.1039/C6PY02161A
Graphical Abstract
Structure defined DPP functionalized conjugated thiophene dendrimers with narrow optical band
gap and high TPA cross section are reported.
For Table of Contents use only
Submit the graphic at the actual size to be used for the TOC so that it will fit in an
area no larger than 3.25 inches by 1.75 inches (approx. 8.5 cm by 4.75 cm).
Page 17 of 17 Polymer Chemistry
Pol
ymer
Che
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Acc
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dM
anus
crip
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Publ
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10
Janu
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2017
. Dow
nloa
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by U
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of
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- Sa
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10/0
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17 1
5:42
:39.
View Article OnlineDOI: 10.1039/C6PY02161A