Increased Exciton Dipole Moment Translates into Charge-transfer Excitons in Thiophene-fluorinated Low-bandgap Polymers for Organic Photovoltaic Applications Elisa Collado-Fregoso 1 , Pierre Boufflet 1 , Zhuping Fei 1 *, Eliot Gann 2,3 Shahid Ashraf 1 , Zhe Li 1,4 , Christopher R. McNeill 3 , James R. Durrant 1,4 * and Martin Heeney 1 * 1 Centre for Plastic Electronics, Department of Chemistry, Imperial College London, Exhibition Road, London SW7 2AZ, United Kingdom 2 Australian Synchrotron, 800 Blackburn Road, Clayton, VIC 3169, Australia 3 Materials Science and Engineering, Monash University, Wellington Road, Clayton, VIC 3800, Australia 4 SPECIFIC IKC, College of Engineering, Swansea University, Central Avenue, Baglan, Port Talbot, SA12 7AX, U.K. Supporting Information 1. UV absorption coefficient 2. Theoretical calculations 3. Crystallinity and morphology of neat and blend materials 4. Transient absorption spectroscopy 1. UV absorption coefficient 400 600 800 1000 0 1x10 4 2x10 4 3x10 4 4x10 4 5x10 4 Absorption Coefficient [cm -1 ] Wavelength [nm] F0 F4 Figure S1. UV-vis absorption coefficient of 0F and 4F in 1,2-dichlorobenzene solution at RT.
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Increased Exciton Dipole Moment Translates into Charge ...€¦ · BM and 0F:PC 70 BM blend films taken at 284 eV. The scattering profile of the 0F blend is peaked at a lower q-value
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Increased Exciton Dipole Moment Translates into Charge-transfer Excitons in Thiophene-fluorinated Low-bandgap Polymers for Organic Photovoltaic Applications
Elisa Collado-Fregoso1, Pierre Boufflet
1, Zhuping Fei
1*, Eliot Gann
2,3 Shahid Ashraf
1, Zhe
Li1,4
, Christopher R. McNeill3, James R. Durrant
1,4* and Martin Heeney
1*
1 Centre for Plastic Electronics, Department of Chemistry, Imperial College London, Exhibition Road, London
SW7 2AZ, United Kingdom 2 Australian Synchrotron, 800 Blackburn Road, Clayton, VIC 3169, Australia
3 Materials Science and Engineering, Monash University, Wellington Road, Clayton, VIC 3800, Australia
4 SPECIFIC IKC, College of Engineering, Swansea University, Central Avenue, Baglan, Port Talbot, SA12
7AX, U.K.
Supporting Information
1. UV absorption coefficient
2. Theoretical calculations
3. Crystallinity and morphology of neat and blend materials
4. Transient absorption spectroscopy
1. UV absorption coefficient
400 600 800 1000
0
1x104
2x104
3x104
4x104
5x104
Ab
so
rpti
on
Co
eff
icie
nt
[cm
-1]
Wavelength [nm]
F0
F4
Figure S1. UV-vis absorption coefficient of 0F and 4F in 1,2-dichlorobenzene solution at RT.
2. Theoretical calculations
Table S1. Calculations for ground and excitated state dipole using B3LYP/6-31G(d) (top) or
WB97XD/6-311G(d,p) (bottom) for one donor-acceptor repeat unit.
B3LYP/6-31G(D)
μg (D) μe (D) Δμge (D)
x y z overall x y z overall
Change
DTBT/0F anti -1.5588 2.1497 0.0014 2.66
-13.9781 4.2876 0.0009 14.62
12.60
DTBT/0F syn -0.8005 -0.0617 -0.1016 0.81
-11.7771 -2.5768 -0.051 12.06
11.26
DTBT/0F anti-syn -0.8914 0.9518 0.0001 1.30
-11.8078 -1.8924 -0.0013 11.96
11.28
DTBT/0F syn-anti -2.0608 3.0285 0.0576 3.66
-14.4379 4.8541 0.0423 15.23
12.51
TFDTBT/4F anti -2.8344 4.6342 -1.0927 5.54
-22.9772 6.0996 -1.8319 23.84
20.21
TFDTBT/4F syn -2.575 3.6763 -0.0001 4.49
-15.4222 0.8998 0.0001 15.45
13.14
TFDTBT/4F anti-syn -2.1712 2.8211 -0.9099 3.67
-21.4436 4.6244 0.2784 21.94
19.39
TFDTBT/4F syn-anti 2.0844 -1.2319 0.9196 2.59
15.99 1.0761 0.5618 16.04
14.10
WB97XD/6-311G(d,p)
μg (D)
μe (D)
Δμge (D)
x y z overall x y z overall Change
DTBT/0F anti -0.8423 1.9511 0.8163 2.28
-6.0514 3.6606 0.0884 7.07
5.53
DTBT/0F syn -0.2332 0.0528 0.1709 0.29
-4.955 -2.1051 0.3117 5.39
5.19
DTBT/0F anti-syn -0.1794 0.6776 1.0092 1.23
-4.6341 -1.3617 2.1752 5.30
5.04
DTBT/0F syn-anti -1.2793 2.8506 0.5975 3.18
-6.6675 4.454 0.5013 8.03
5.62
TFDTBT/4F anti 2.1444 -4.5918 -1.3456 5.24
9.8617 -5.448 -1.8206 11.41
7.78
TFDTBT/4F syn -1.895 4.1948 -0.0011 4.60
-7.8955 2.2322 0.0011 8.20
6.31
TFDTBT/4F anti-syn 1.4053 -1.5798 1.8657 2.82
8.2774 0.0165 1.8936 8.49
7.06
TFDTBT/4F syn-anti -1.4838 2.4949 -0.7663 3.00
-8.226 3.9304 0.081 9.12
6.95
3. Crystallinity and morphology of neat and blend materials
Figure S2. AFM Topography and phase images of F0/PC70BM 1:2 blend (a) and (b), and F4/PC70BM
1:2 blend (c) and (d). Size: 1x1 µm.
Figure S3. Top: R-SoXS scattering profiles taken of 4F:PC70BM and 0F:PC70BM blend films taken
at 284 eV. The scattering profile of the 0F blend is peaked at a lower q-value indicating a larger
domain spacing, with the top axis giving the corresponding real-space size. Intergration of the
scattering profiles reveals a ratio of 1:1.45 0F:4F or relative purities of 100% for 4F and 68.6% for 0F
Bottom: Contrast functions calcualted from the optical constatns of 0F, 4F and PC70BM that were
used to determin the energy of maximum materials constrate (284 eV).
Figure S4. Grazing incidence wide-angle x-ray scattering of neat F0 and F4 and F0/PC70BM and
F0/PC70BM blends along with out-of-plane and in-plane line-outs.
PCBM
4. Transient absorption spectroscopy
Figure S5.Sub-picosecond resolved TAS traces at the excitation energy densities presented in this
study (3 uJ/cm2) and lower energy intensities (1 uJ/cm
2) showing that the dynamics are comparable
over this range. a) F0/PC70BM 1:2 blend films and b) F4/PC70BM 1:2 blend films.
Figure S6. Microsecond-resolved transients taken exciting at 660 nm with 5 J/cm2 and probing at
1160 nm for F0 neat film (a) and F0 blend film (c) and at 1060 for F4 neat film (b) and F4 blend film
baa
100f 1p 10p 100p 1n0.0
0.5
1.0
1.5
2.0
O
D / m
OD
t / s
F4 blend, 1 uJ/cm2 x 3.6
F4 blend, 3 uJ/cm2
100f 1p 10p 100p 1n0.0
0.5
1.0
1.5
2.0
O
D / m
OD
t / s
F0 blend, 1 uJ/cm2 x 3.1
F0 blend, 3 uJ/cm2
a
1 101E-5
1E-4
1E-3
0.01
0.1
O
D [m
OD
]
t [s]
F0 blend N2
F0 blend O2
c
1 101E-5
1E-4
1E-3
0.01
0.1
O
D [m
OD
]
t [s]
F4 blend N2
F4 blend O2
d
0 2 4 6 8 10
0.00
0.01
0.02
0.03
0.04
O
D [m
OD
]
t [s]
F4 neat N2
F4 neat O2
0 2 4 6 8 10
0.00
0.01
0.02
0.03
O
D [m
OD
]
t [s]
F0 neat N2
F0 neat O2
a b
(d) showing the presence of triplets in F4 neat, and the absence of them in both blends. See main text
for the discussion on F0 neat. The blends were plotted in log-log scales to emphasize the linear
behaviour, characteristic of polarons.
1 10 100 10000.0
0.2
0.4
0.6
0.8
1.0
1.2
No
rm
OD
[a.u
.]
t [ps]
950 nm
1100 nm
1150 nm
1200 nm
Figure S7. Probed-wavelength dependence of the F4 exciton dynamics showing the the blue-shift of
the signal in the first 10 ps, after excitation at 710 nm with an intensity of 3 J/cm2. In red, best-
triexponential fits.
Table S2. Best tri-exponential fits, 𝑦 = 𝑦0 + 𝐴1𝑒−𝑥 𝜏1⁄ + 𝐴2𝑒−𝑥 𝜏2⁄ + 𝐴3𝑒−𝑥 𝜏3⁄ to the IR exciton
decays for different probed wavelentghts. Values are reported ± standard error.