TY - JOUR
T1 - Charge Separation in Intermixed Polymer:PC70BM Photovoltaic Blends: Correlating Structural and Photophysical Length Scales as a Function of Blend Composition
AU - Utzat, Hendrik
AU - Dimitrov, Stoichko D.
AU - Wheeler, Scot
AU - Collado-Fregoso, Elisa
AU - Tuladhar, Pabitra Shakya
AU - Schroeder, Bob C.
AU - McCulloch, Iain
AU - Durrant, James R.
N1 - KAUST Repository Item: Exported on 2020-10-01
Acknowledgements: The authors thank Florent Deledalle for the helpful discussions of nongeminate recombination dynamics and Safa Shoaee for measuring TEM images. We also thank the EPSRC (EP/IO1927B/1 and EP/K011987/1) for funding. B.C.S. acknowledges the National Research Fund of Luxembourg for financial support. This work is partially funded by the European regional Development Fund through the Welsh Government.
PY - 2017/4/24
Y1 - 2017/4/24
N2 - A key challenge in achieving control over photocurrent generation by bulk-heterojunction organic solar cells is understanding how the morphology of the active layer impacts charge separation and in particular the separation dynamics within molecularly intermixed donor-acceptor domains versus the dynamics between phase-segregated domains. This paper addresses this issue by studying blends and devices of the amorphous silicon-indacenodithiophene polymer SiIDT-DTBT and the acceptor PCBM. By changing the blend composition, we modulate the size and density of the pure and intermixed domains on the nanometer length scale. Laser spectroscopic studies show that these changes in morphology correlate quantitatively with the changes in charge separation dynamics on the nanosecond time scale and with device photocurrent densities. At low fullerene compositions, where only a single, molecularly intermixed polymer-fullerene phase is observed, photoexcitation results in a ∼ 30% charge loss from geminate polaron pair recombination, which is further studied via light intensity experiments showing that the radius of the polaron pairs in the intermixed phase is 3-5 nm. At high fullerene compositions (≥67%), where the intermixed domains are 1-3 nm and the pure fullerene phases reach ∼4 nm, the geminate recombination is suppressed by the reduction of the intermixed phase, making the fullerene domains accessible for electron escape.
AB - A key challenge in achieving control over photocurrent generation by bulk-heterojunction organic solar cells is understanding how the morphology of the active layer impacts charge separation and in particular the separation dynamics within molecularly intermixed donor-acceptor domains versus the dynamics between phase-segregated domains. This paper addresses this issue by studying blends and devices of the amorphous silicon-indacenodithiophene polymer SiIDT-DTBT and the acceptor PCBM. By changing the blend composition, we modulate the size and density of the pure and intermixed domains on the nanometer length scale. Laser spectroscopic studies show that these changes in morphology correlate quantitatively with the changes in charge separation dynamics on the nanosecond time scale and with device photocurrent densities. At low fullerene compositions, where only a single, molecularly intermixed polymer-fullerene phase is observed, photoexcitation results in a ∼ 30% charge loss from geminate polaron pair recombination, which is further studied via light intensity experiments showing that the radius of the polaron pairs in the intermixed phase is 3-5 nm. At high fullerene compositions (≥67%), where the intermixed domains are 1-3 nm and the pure fullerene phases reach ∼4 nm, the geminate recombination is suppressed by the reduction of the intermixed phase, making the fullerene domains accessible for electron escape.
UR - http://hdl.handle.net/10754/625579
UR - http://pubs.acs.org/doi/full/10.1021/acs.jpcc.7b02898
UR - http://www.scopus.com/inward/record.url?scp=85020943445&partnerID=8YFLogxK
U2 - 10.1021/acs.jpcc.7b02898
DO - 10.1021/acs.jpcc.7b02898
M3 - Article
SN - 1932-7447
VL - 121
SP - 9790
EP - 9801
JO - The Journal of Physical Chemistry C
JF - The Journal of Physical Chemistry C
IS - 18
ER -