Heteroatom substitution can favorably alter electronic transport in conductive polymers to improve their thermoelectric performance. This study reports the spectroscopic, structural, and thermoelectric properties of poly(3–(3′,7′-dimethyloctyl) chalcogenophenes) or P3RX doped with 2,3,5,6-tetrafluoro-7,7,8,8-tetracyanoquinodimethane (F4TCNQ), where the heteroatom [X = thiophene (T), selenophene (Se), tellurophene (Te)], the doping methodology, and extent of doping are systematically varied. Spectroscopic measurements reveal that while all P3RX polymers are appreciably doped, the doping mechanism is inherently different. Poly(3-hexylthiophene) (P3HT, used as a control) and poly(3–(3′,7′-dimethyloctyl)tellurophene) (P3RTe) are doped primarily via integer charge transfer (ICT), whereas poly(3–(3′,7′-dimethyloctyl)selenophene) (P3RSe) and poly(3–(3′,7′-dimethyloctyl)thiophene) (P3RT) are doped via charge transfer complex (CTC) mechanisms. Despite these differences, all polymers saturate with roughly the same number of F4TCNQ counterions (1 dopant per 4 to 6 heterocycles), reinforcing the idea that the extent of charge transfer varies with the doping mechanism. Grazing incidence wide-angle x-ray scattering measurements provide insight into the structural driving forces behind different doping mechanisms—P3RT and P3RSe have similar microstructures in which F4TCNQ intercalates between the π-stacked backbones resulting in CTC doping (localized carriers), while P3HT and P3RTe have microstructures in which F4TCNQ intercalates in the alkyl side chain region, giving rise to ICT doping (delocalized carriers). These structural and spectroscopic observations shed light on why P3HT and P3RTe obtain electrical conductivities ca. 3 S/cm, while P3RT and P3RSe have conductivities <10−3 S/cm under the same thin film processing conditions. Ultimately, this work quantifies the effects of heteroatom, microstructural ordering, extent of doping, and doping mechanism, thereby providing rational guidance for designing future thermoelectric polymer-dopant systems.
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Microstructure and heteroatom dictate the doping mechanism and thermoelectric properties of poly(alkyl-chalcogenophenes)
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7 June 2021
Research Article|
June 07 2021
Microstructure and heteroatom dictate the doping mechanism and thermoelectric properties of poly(alkyl-chalcogenophenes)
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Special Collection:
Organic and Hybrid Thermoelectrics
Madeleine P. Gordon;
Madeleine P. Gordon
1
The Molecular Foundry, Lawrence Berkeley National Laboratory
, Berkeley, California 94720, USA
2
Applied Science and Technology Graduate Group, University of California
, Berkeley, Berkeley, California 94720, USA
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Shawn A. Gregory;
Shawn A. Gregory
3
School of Materials Science and Engineering, Georgia Institute of Technology
, Atlanta, Georgia 30332, USA
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Jamie P. Wooding;
Jamie P. Wooding
3
School of Materials Science and Engineering, Georgia Institute of Technology
, Atlanta, Georgia 30332, USA
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Shuyang Ye;
Shuyang Ye
4
Department of Chemistry, University of Toronto
, 80 St. George Street, Toronto, Ontario M5S 1A1, Canada
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Gregory M. Su
;
Gregory M. Su
5
Materials Sciences Division, Lawrence Berkeley National Laboratory
, Berkeley, California 94720, USA
6
Advanced Light Source, Lawrence Berkeley National Laboratory
, Berkeley, California 94720, USA
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Dwight S. Seferos;
Dwight S. Seferos
4
Department of Chemistry, University of Toronto
, 80 St. George Street, Toronto, Ontario M5S 1A1, Canada
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Mark D. Losego
;
Mark D. Losego
3
School of Materials Science and Engineering, Georgia Institute of Technology
, Atlanta, Georgia 30332, USA
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Jeffrey J. Urban
;
Jeffrey J. Urban
a)
1
The Molecular Foundry, Lawrence Berkeley National Laboratory
, Berkeley, California 94720, USA
a)Authors to whom correspondence should be addressed: [email protected]; [email protected]; and [email protected]
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Shannon K. Yee
;
Shannon K. Yee
a)
7
G. W. Woodruff School of Mechanical Engineering, Georgia Institute of Technology
, Atlanta, Georgia 30332, USA
a)Authors to whom correspondence should be addressed: [email protected]; [email protected]; and [email protected]
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Akanksha K. Menon
Akanksha K. Menon
a)
7
G. W. Woodruff School of Mechanical Engineering, Georgia Institute of Technology
, Atlanta, Georgia 30332, USA
a)Authors to whom correspondence should be addressed: [email protected]; [email protected]; and [email protected]
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Madeleine P. Gordon
1,2
Shawn A. Gregory
3
Jamie P. Wooding
3
Shuyang Ye
4
Gregory M. Su
5,6
Dwight S. Seferos
4
Mark D. Losego
3
Jeffrey J. Urban
1,a)
Shannon K. Yee
7,a)
Akanksha K. Menon
7,a)
1
The Molecular Foundry, Lawrence Berkeley National Laboratory
, Berkeley, California 94720, USA
2
Applied Science and Technology Graduate Group, University of California
, Berkeley, Berkeley, California 94720, USA
3
School of Materials Science and Engineering, Georgia Institute of Technology
, Atlanta, Georgia 30332, USA
4
Department of Chemistry, University of Toronto
, 80 St. George Street, Toronto, Ontario M5S 1A1, Canada
5
Materials Sciences Division, Lawrence Berkeley National Laboratory
, Berkeley, California 94720, USA
6
Advanced Light Source, Lawrence Berkeley National Laboratory
, Berkeley, California 94720, USA
7
G. W. Woodruff School of Mechanical Engineering, Georgia Institute of Technology
, Atlanta, Georgia 30332, USA
a)Authors to whom correspondence should be addressed: [email protected]; [email protected]; and [email protected]
Note: This paper is part of the APL Special Collection on Organic and Hybrid Thermoelectrics.
Appl. Phys. Lett. 118, 233301 (2021)
Article history
Received:
March 31 2021
Accepted:
May 20 2021
Citation
Madeleine P. Gordon, Shawn A. Gregory, Jamie P. Wooding, Shuyang Ye, Gregory M. Su, Dwight S. Seferos, Mark D. Losego, Jeffrey J. Urban, Shannon K. Yee, Akanksha K. Menon; Microstructure and heteroatom dictate the doping mechanism and thermoelectric properties of poly(alkyl-chalcogenophenes). Appl. Phys. Lett. 7 June 2021; 118 (23): 233301. https://doi.org/10.1063/5.0052604
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