fine-tuning energy levels via asymmetric end groups ... · s1 supporting information fine-tuning...
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JOUL, Volume 4
Supplemental Information
Fine-Tuning Energy Levels via Asymmetric
End Groups Enables Polymer
Solar Cells with Efficiencies over 17%
Zhenghui Luo, Ruijie Ma, Tao Liu, Jianwei Yu, Yiqun Xiao, Rui Sun, Guanshui Xie, JunYuan, Yuzhong Chen, Kai Chen, Gaoda Chai, Huiliang Sun, Jie Min, JianZhang, Yingping Zou, Chuluo Yang, Xinhui Lu, Feng Gao, and He Yan
S1
Supporting Information
Fine-tuning Energy Levels via Asymmetric End Groups Enables Polymer
Solar Cells with Efficiencies over 17%
Zhenghui Luo,1,2,10 Ruijie Ma,1,2,10 Tao Liu, 1,2,10* Jianwei Yu,3 Yiqun Xiao,4 Rui Sun,5
Guanshui Xie,6 Jun Yuan,7 Yuzhong Chen,1,2 Kai Chen,1,2 Gaoda Chai,1,2 Huiliang Sun,1
Jie Min,5 Jian Zhang,6 Yingping Zou,7 Chuluo Yang,8 Xinhui Lu,4,* Feng Gao,3 He Yan,
1,2,9,11*
1Hong Kong University of Science and Technology-Shenzhen Research Institute, No. 9
Yuexing first RD, Hi-tech Park, Nanshan, Shenzhen 518057, P. R. China. 2Department of Chemistry and Hong Kong Branch of Chinese National Engineering
Research Center for Tissue Restoration & Reconstruction, Hong Kong University of
Science and Technology (HKUST), Clear Water Bay, Kowloon, Hong Kong, China. 3Department of Physics, Chemistry and Biology (IFM), Linköping University,
Linköping SE-58183, Sweden 4Department of Physics, Chinese University of Hong Kong, New Territories, Hong Kong,
China. 5The Institute for Advanced Studies, Wuhan University, Wuhan 430072, China. 6School of Materials Science and engineering, Guangxi Key Laboratory of Information
Materials, Guilin University of Electronic Technology, 1st Jinji Road, Guilin, 541004, P.
R. China. 7College of Chemistry and Chemical Engineering, Central South University, Changsha
410083, P. R. China
8Shenzhen Key Laboratory of Polymer Science and Technology, College of Materials
Science and Engineering, Shenzhen University, Shenzhen 518060, China. 9State Key Laboratory of Luminescent Materials and Devices, South China University of
Technology, Guangzhou 510640, China. 10These authors contributed equally. 11Lead Contact
*Correspondence: [email protected] (T.L.), [email protected] (X.L), [email protected]
(H.Y.)
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Materials and Measurements
All solvents and reagents were used as received from commercial sources and used
without further purification unless otherwise specified. 1H NMR (400 MHz) and 13C NMR
(100 MHz) spectra were measured on a MERCURYVX300 spectrometers. Mass spectra
were recorded on a Shimadzu spectrometer. UV-vis-NIR absorption spectra were recorded
on a Shimadzu UV-2700 recording spectrophotometer. Cyclic voltammetry (CV)
measurements were carried out on a CHI voltammetric analyzer at room temperature.
Tetrabutylammonium hexafluorophosphate (n-Bu4NPF6, 0.1 M) was used as the
supporting electrolyte. The conventional three-electrode configuration consists of a
platinum working electrode with a 2 mm diameter, a platinum wire counter electrode, and
a Ag/AgCl wire reference electrode. Cyclic voltammograms were obtained at a scan rate
of 100 mV/s. PL spectra were measured with a Shimadzu RF-5301PC fluorescence
spectrophotometer. The film morphology was measured using an atomic force microscope
(AFM, Bruker-ICON2-SYS) using the tapping mode. The RMS values of the surface AFM
images are averaged based on five times testing on different areas for each sample. DFT
calculations were performed by using Gaussian at the B3LYP-D3(BJ)/def2-SVP level, and
the long alkyl chain was simplified as methyl.
Device fabrication and characterization
Solar cells were fabricated in a conventional device configuration of
ITO/PEDOT:PSS/active layers/PNDIT-F3N/Ag. The ITO substrates were first scrubbed
by detergent and then sonicated with deionized water, acetone and isopropanol
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subsequently, and dried overnight in an oven. The glass substrates were treated by UV-
Ozone for 30 min before use. PEDOT:PSS (Heraeus Clevios P VP AI 4083) was spin-cast
onto the ITO substrates at 4000 rpm for 30 s, and then dried at 150 °C for 15 min in air.
The PM6 (Mn =40.8 KDa with PDI of 2.04): acceptor blends (1:1.2 weight ratio) were
dissolved in chloroform (the total concentration of blend solutions was 15 mg mL-1 for all
blends), 0.5% (vol%) 1-chloronaphthalene was utilized as the solvent additive, and stirred
overnight in a nitrogen-filled glove box. The blend solution was spin-cast at 3000 rpm for
30 s. A thin PNDIT-F3N layer was coated on the active layer, followed by the deposition
of Ag (100 nm) (evaporated under 5×10-5 Pa through a shadow mask). The optimal active
layer thickness measured by a Bruker Dektak XT stylus profilometer was about 105 nm.
The current density-voltage (J-V) curves of all encapsulated devices were measured using
a Keithley 2400 Source Meter in air under AM 1.5G (100 mW cm-2) using a Newport solar
simulator. The light intensity was calibrated using a standard Si diode (with KG5 filter,
purchased from PV Measurement to bring spectral mismatch to unity). Optical microscope
(Olympus BX51) was used to define the device area (5.9 mm²). EQEs were measured using
an Enlitech QE-S EQE system equipped with a standard Si diode. Monochromatic light
was generated from a Newport 300W lamp source.
To confirm the reliability of the champion PCE of the PM6:BTP-2F-ThCl-based device,
we sent our acceptor material of BTP-2F-ThCl to two different research groups to
reproduce the result, namely, Min Jie’s group and Zhang jian’s group. The optimal J-V
curves of PSCs and corresponding IPCE spectra are exhibited in Figure S9. In Min's group,
S4
they used the same device conditions as our group, and the PM6:BTP-2F-ThCl-based
device yields a PCE of 16.8%, with a VOC of 0.862 V, a JSC of 25.4 mA/cm2 along with a
FF of 0.768. However, in Zhang’s group, even if they employed PDINO instead of PNDIT-
F3N as the electron transport layer, the PM6:BTP-2F-ThCl-based device yields a PCE of
16.9%, with VOC of 0.883 V, a JSC of 25.3 mA/cm2 along with a FF of 0.755. These results
indicate the reliability of champion PCE of the PM6:BTP-2F-ThCl-based device.
Mobility Measurements
Hole and electron mobility were measured using the space charge limited current (SCLC)
method. Device structures are ITO/MoOx/active layer/MoOx/Ag for hole-only devices and
ITO/ZnO/active layer/PNDIT-F3N/Ag for electron-only devices. The SCLC mobilities
were calculated by MOTT-Gurney equation: J = 9ε0εrμV2/8L3. Where J is the current
density, εr is the relative dieletiric constant of active layer material usually 2-4 for organic
semiconductor, herein we use a relative dielectric constant of 3, ε0 is the permittivity of
empty space, µ is the mobility of hole or electron and L is the thickness of the active layer,
V is the internal voltage in the device, and V = VApplied – VBuilt-in (in the hole-only and the
electron-only devices, the Vbi values are 0.2 V and 0 V respectively), where VApplied is the
voltage applied to the device, and VBuilt-in is the built-in voltage resulting from the relative
work function difference between the two electrodes.
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GIWAXS measurement
GIWAXS measurement were carried out with a Xeuss 2.0 SAXS/WAXS laboratory
beamline using a Cu X-ray source (8.05 keV, 1.54 Å) and a Pilatus3R 300K detector. The
incidence angle is 0.2°. The samples for GIWAXS measurements are fabricated on silicon
substrates using the same recipe for the devices.
Scheme S1. Synthesis of BTP-2F-ThCl and IT-2FCl.
Synthesis of BTP-2F-ThCl:
BTP-4F-CHO (200 mg, 0.195 mmol), compound 2 (49.3 mg, 0.2145 mmol), compound 3
(50.2 mg, 0.2145 mmol), chloroform (20 mL), and pyridine (1 mL) were added to a two-
necked round-bottomed flask. The mixture was deoxygenated with nitrogen for 30 min and
then refluxed for 24 h. After cooling to room temperature, the mixture was poured into
methanol (200 mL) and filtered. The residue was purified by column chromatography on
silica gel using petroleum ether/dichloromethane (1:1) as eluent, yielding a dark blue solid
(113 mg, 40%). 1H NMR (CDCl3, 400 MHz): δ [ppm]: 9.07 (s, 1H), 8.97 (s, 1H), 8.51–
S6
8.47 (m, 1H), 8.10 (s, 1H), 7.72 (t, J = 7.3 Hz, 1H), 4.81 (s, 4H), 3.18 (s, 4H), 2.18 (s, 2H),
1.84 (d, J = 6.4 Hz, 4H), 1.47 (s, 4H), 1.37–0.96 (m, 44H), 0.92–0.65 (m, 18H). 13C NMR
(100 MHz, CDCl3): δ [ppm]: 186.14, 158.67, 153.86, 147.39, 145.24, 141.45, 138.03,
137.82, 136.54, 136.00, 135.15, 133.90, 133.38, 133.23, 131.59, 130.45, 126.50, 125.20,
119.90, 114.83), 113.70, 112.40, 77.29, 77.03, 76.71, 66.32, 55.72, 40.39, 31.91, 31.19,
30.12, 29.24, 27.61, 23.20, 22.89, 22.69, 14.12, 13.78, 10.48, 10.11. MS (MALDI-TOF)
m/z: [M+H]+ calcd. for (C80H85ClF2N8O2S6): 1454.4776; Found: 1454.4776.
Synthesis of IT-2FCl:
IT-CHO (200 mg, 0.196 mmol), compound 2 (49.6 mg, 0.2156 mmol), compound 3 (50.5
mg, 0.2156 mmol), chloroform (30 mL), and pyridine (1 mL) were added to a two-necked
round-bottomed flask. The mixture was deoxygenated with nitrogen for 30 min and then
refluxed for 24 h. After cooling to room temperature, the mixture was poured into methanol
(200 mL) and filtered. The residue was purified by column chromatography on silica gel
using petroleum ether/dichloromethane (1:2) as eluent, yielding a dark blue solid (88.3 mg,
30%). 1H NMR (CDCl3, 400 MHz): δ [ppm]: 8.85 (s, 1H), 8.78 (s, 1H), 8.53 (dd, J = 7.5
Hz, 1H), 8.22 (s, 2H), 8.12 (s, 1H), 7.75-7.67 (m, 3H), 7.22 (d, J = 7.9 Hz, 8H), 7.15 (d, J
= 7.8 Hz, 8H), 2.58 (t, J = 7.6 Hz, 8H), 1.65-1.57 (m, 8H), 1.35-1.20 (m, 24H), 0.92-0.82
(m, 12H). 13C NMR (100 MHz, CDCl3): δ [ppm]: 185.12, 179.19, 157.55, 155.26, 154.19,
153.30, 153.03, 147.59, 147.38, 146.87, 143.42, 141.99, 140.69, 139.15, 138.83, 138.14,
137.78, 136.88, 136.42, 135.33, 131.24, 128.29, 127.59, 127.23, 124.89, 121.14, 118.09,
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114.46, 114.10, 113.53, 76.73, 76.41, 76.09, 67.02, 62.65, 34.98, 31.07, 30.63, 28.56, 21.96,
13.46. MS (MALDI-TOF) m/z: [M+H]+ calcd. for (C92H77ClF2N4O2S5): 1502.4307; Found:
1502.4296.
Figure S1. 1H NMR spectrum of BTP-2F-ThCl in CDCl3.
S8
Figure S2. 13C NMR spectrum of BTP-2F-ThCl in CDCl3.
Figure S3. MS spectrum (MALDI-TOF) of BTP-2F-ThCl.
lzh-43, MW=1458; DCTB;
m/z1400 1405 1410 1415 1420 1425 1430 1435 1440 1445 1450 1455 1460 1465 1470 1475 1480 1485 1490 1495 1500 1505 1510 1515
%
0
100
yan191107_2 4 (0.132) Cn (Cen,2, 10.00, Ar); Sb (5,20.00 ); Sm (SG, 2x3.00); Cm (4:15) TOF LD+ 4.30e31456.3555
1455.3699
1454.3820
1451.4705
1457.3326
1458.3212
1459.3008
1460.2939
1461.2612
1462.2878
S9
Figure S4. 1H NMR spectrum of IT-2FCl in CDCl3.
Figure S5. 13C NMR spectrum of IT-2FCl in CDCl3.
S10
Figure S6. MS spectrum (MALDI-TOF) of IT-2FCl.
Figure S7. The frontier molecular orbitals obtained by DFT for BTP-4F, BTP-2F-ThCl
and BTP-2ThCl.
lzh-5; MW=1502; DCTB
m/z1455 1460 1465 1470 1475 1480 1485 1490 1495 1500 1505 1510 1515 1520 1525 1530 1535 1540 1545 1550 1555
%
0
100
yan191126_1 16 (0.534) Cn (Cen,2, 10.00, Ar); Sb (5,20.00 ); Sm (SG, 2x3.00); Cm (3:17) TOF LD+ 2911504.4258
1502.4296
1499.51941479.74241459.8209 1469.6145 1489.8700
1505.4268
1506.4302
1507.4169
1508.4218
1509.4114
1551.96951514.5022 1529.23821522.4368 1535.46081548.7607
1558.1600
S11
Figure S8. Space-charge-limited (SCLC) J-V characteristics of neat BTP-4F, BTP-2F-
ThCl and BTP-2ThCl film under dark condition.
Figure S9. The Photovoltaic Properties: (A) J-V characteristics of the best OSCs under
the illumination of AM 1.5G, 100 mW cm−2; (B) IPCE spectra of the best devices based
on PM6:BTP-2F-ThCl.
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Figure S10. Device stability: (A) The long-term stability of PM6:BTP-4F, PM6:BTP-2F-
ThCl and PM6:BTP-2ThCl-based PSCs within 30 days packaged conventional devices
stored in air; (B) The photostability of PM6:BTP-4F, PM6:BTP-2F-ThCl and PM6:BTP-
2ThCl-based PSCs within 108 hours packaged conventional devices under LED flood
light with a power of 150W illumination.
Table S1 The parameters of exciton dissociation efficiency and charge collection
efficiency.
Active layer Jsat
(mA/cm2)
Jpha
(mA/cm2)
Jphb
(mA/cm2)
ηdiss (%) ηcoll (%)
PM6:BTP-4F 26.60 25.19 22.30 94.7 83.9
PM6:BTP-2F-
ThCl
26.70 25.38 23.06 95.0 86.3
PM6:BTP-
2ThCl
25.80 23.46 18.91 90.9 73.3
a: Under short circuit condition; b: Under the maximal power output condition
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Figure S11. J-V characteristics in dark for hole-only (A) and electron-only (B) devices
based on PM6:BTP-4F, PM6:BTP-2F-ThCl and PM6:BTP-2ThCl blends.
Table S2. The parameters of hole mobilities and electron mobilities.
Active layer μh
(10-4 cm2 V-1 s-1)
μe
(10-4 cm2 V-1 s-1)
μh/μe
PM6:BTP-4F 5.89 3.69 1.60
PM6:BTP-2F-ThCl 5.21 3.28 1.58
PM6:BTP-2ThCl 4.78 2.55 1.87
Figure S12. 2D GIWAXS patterns of PM6:BTP-4F, PM6:BTP-2F-ThCl and PM6:BTP-
2ThCl blend films.
S14
Figure S13. The contact angle images of neat PM6, BTP-4F, BTP-2F-ThCl and BTP-
2ThCl films.
Table S3. Contact angles of water and ethylene glycol (EG), and surface free energy, and
Flory–Huggins interaction parameters of PM6, BTP-4F, BTP-2F-ThCl, and BTP-2ThCl.
The average contact angles and standard deviations were obtained from 5 films.
Surface θwater (o) θEG (o) γ (mN/m)(a) χ [PM6, i](b)
PM6 107.1 ± 0.5 75.6 ± 0.7 27.4
BTP-4F 90.3 ± 0.4 57.3 ± 0.8 33.1 0.27
BTP-2F-ThCl 89.4 ± 0.6 69.3 ± 1.0 21.8 0.31
BTP-2ThCl 100.0 ± 0.3 66.6 ± 0.5 31.4 0.13
(a) The surface free energy (γ) calculated by Young’s equation.
(b) The Flory-Huggins interaction parameters between the donor (D) and the acceptor (A)
calculated using χ = (√γD-√γA)2.
Figure S14. GISAXS intensity profiles and best fittings along the in-plane direction.
S15
Table S4. Summary of parameters measured and calculated from FTPS-EQE and EL.
Device Eg
pv
(eV)
EQEEL
10-4
Eloss
(eV)
q∆VSQ
oc
(eV)
∆E1=Egap-q∆VSQ
oc
(eV)
qVrad
oc
(eV)
∆E2 =q∆Vrad.
oc
(eV)
∆E3= q∆Vnon-
rad oc
(eV)
Voccal
(eV)
BTP-4F 1.40 0.69 0.56 1.14 0.26 1.09 0.05 0.25 0.84
BTP-2F-ThCl 1.40 1.7 0.53 1.14 0.26 1.09 0.05 0.22 0.87
BTP-2ThCl 1.41 3.0 0.52 1.15 0.26 1.10 0.05 0.21 0.89