Two‐Step Design Rule for Simultaneously High Conductivity and Seebeck Coefficient in Conjugated Polymer‐Based Thermoelectrics

Abstract The trade‐off between enhancing conductivity (σ) through doping while concurrently observing a reduction in the Seebeck coefficient (S) presents a key challenge in organic thermoelectrics. Here, a two‐step structural design strategy is developed, where the first step enhances the backbone p...

Full description

Saved in:
Bibliographic Details
Main Authors: Zelong Li, Wei Fu, Dorothea Scheunemann, Xiaoran Wei, Maximilian Litterst, Priya Mariam Viji, Yong Cui, Jianhui Hou, Junhui Tang, Ziqi Liang, Zehua Qu, Martijn Kemerink, Ruiqian Guo, Guangzheng Zuo
Format: Article
Language:English
Published: Wiley 2025-01-01
Series:Advanced Science
Subjects:
Online Access:https://doi.org/10.1002/advs.202409382
Tags: Add Tag
No Tags, Be the first to tag this record!
_version_ 1841553150940545024
author Zelong Li
Wei Fu
Dorothea Scheunemann
Xiaoran Wei
Maximilian Litterst
Priya Mariam Viji
Yong Cui
Jianhui Hou
Junhui Tang
Ziqi Liang
Zehua Qu
Martijn Kemerink
Ruiqian Guo
Guangzheng Zuo
author_facet Zelong Li
Wei Fu
Dorothea Scheunemann
Xiaoran Wei
Maximilian Litterst
Priya Mariam Viji
Yong Cui
Jianhui Hou
Junhui Tang
Ziqi Liang
Zehua Qu
Martijn Kemerink
Ruiqian Guo
Guangzheng Zuo
author_sort Zelong Li
collection DOAJ
description Abstract The trade‐off between enhancing conductivity (σ) through doping while concurrently observing a reduction in the Seebeck coefficient (S) presents a key challenge in organic thermoelectrics. Here, a two‐step structural design strategy is developed, where the first step enhances the backbone planarity which enhances the conductivity by an improved ordering of conjugated polymers (CPs). The second step, which is fluorination of the backbone, improves the Seebeck coefficient by the controlled induction of energetic disorder, stemming from the fluorine's disruption of the homogeneous electrostatic potential across the CP backbone. This strategy is applied to two series of donor‐acceptor (D‐A) types of CPs based on the BDT donor unit and BDD and TT as acceptor units, respectively. A maximum power factor (PF) over 155 (142.7 ± 12.7) µW m−1 K−2, coupled with S ≈202 (194.6 ± 7.6) µV K−1 is achieved, leading to up to 32‐fold enhancement of the PF compared to the initial non‐planar and non‐fluorinated polymer. This study provides valuable conceptual insights for designing CPs with high conductivity and Seebeck coefficient.
format Article
id doaj-art-6423090db76541a0a9d5d5b3c85b3da6
institution Kabale University
issn 2198-3844
language English
publishDate 2025-01-01
publisher Wiley
record_format Article
series Advanced Science
spelling doaj-art-6423090db76541a0a9d5d5b3c85b3da62025-01-09T11:44:46ZengWileyAdvanced Science2198-38442025-01-01121n/an/a10.1002/advs.202409382Two‐Step Design Rule for Simultaneously High Conductivity and Seebeck Coefficient in Conjugated Polymer‐Based ThermoelectricsZelong Li0Wei Fu1Dorothea Scheunemann2Xiaoran Wei3Maximilian Litterst4Priya Mariam Viji5Yong Cui6Jianhui Hou7Junhui Tang8Ziqi Liang9Zehua Qu10Martijn Kemerink11Ruiqian Guo12Guangzheng Zuo13Institute for Electric Light Sources School of Information Science and Technology Fudan University Shanghai 200433 P. R. ChinaInstitute for Electric Light Sources School of Information Science and Technology Fudan University Shanghai 200433 P. R. ChinaInstitute for Molecular Systems Engineering and Advanced Materials Heidelberg University Im Neuenheimer Feld 225 69120 Heidelberg GermanyInstitute for Electric Light Sources School of Information Science and Technology Fudan University Shanghai 200433 P. R. ChinaInstitute for Molecular Systems Engineering and Advanced Materials Heidelberg University Im Neuenheimer Feld 225 69120 Heidelberg GermanyInstitute for Molecular Systems Engineering and Advanced Materials Heidelberg University Im Neuenheimer Feld 225 69120 Heidelberg GermanyState Key Laboratory of Polymer Physics and Chemistry Beijing National Laboratory for Molecular Sciences CAS Research/Education Center for Excellence in Molecular Sciences Institute of Chemistry Chinese Academy of Sciences Beijing 100190 P. R. ChinaState Key Laboratory of Polymer Physics and Chemistry Beijing National Laboratory for Molecular Sciences CAS Research/Education Center for Excellence in Molecular Sciences Institute of Chemistry Chinese Academy of Sciences Beijing 100190 P. R. ChinaDepartment of Materials Science Fudan University Shanghai 200433 P. R. ChinaDepartment of Materials Science Fudan University Shanghai 200433 P. R. ChinaState Key Laboratory of Molecular Engineering of Polymers Department of Macromolecular Science Fudan University Shanghai 200433 P. R. ChinaInstitute for Molecular Systems Engineering and Advanced Materials Heidelberg University Im Neuenheimer Feld 225 69120 Heidelberg GermanyInstitute for Electric Light Sources School of Information Science and Technology Fudan University Shanghai 200433 P. R. ChinaInstitute for Electric Light Sources School of Information Science and Technology Fudan University Shanghai 200433 P. R. ChinaAbstract The trade‐off between enhancing conductivity (σ) through doping while concurrently observing a reduction in the Seebeck coefficient (S) presents a key challenge in organic thermoelectrics. Here, a two‐step structural design strategy is developed, where the first step enhances the backbone planarity which enhances the conductivity by an improved ordering of conjugated polymers (CPs). The second step, which is fluorination of the backbone, improves the Seebeck coefficient by the controlled induction of energetic disorder, stemming from the fluorine's disruption of the homogeneous electrostatic potential across the CP backbone. This strategy is applied to two series of donor‐acceptor (D‐A) types of CPs based on the BDT donor unit and BDD and TT as acceptor units, respectively. A maximum power factor (PF) over 155 (142.7 ± 12.7) µW m−1 K−2, coupled with S ≈202 (194.6 ± 7.6) µV K−1 is achieved, leading to up to 32‐fold enhancement of the PF compared to the initial non‐planar and non‐fluorinated polymer. This study provides valuable conceptual insights for designing CPs with high conductivity and Seebeck coefficient.https://doi.org/10.1002/advs.202409382conductivityenergetic disorderfluorine substitutionorganic thermoelectricsseebeck coefficient
spellingShingle Zelong Li
Wei Fu
Dorothea Scheunemann
Xiaoran Wei
Maximilian Litterst
Priya Mariam Viji
Yong Cui
Jianhui Hou
Junhui Tang
Ziqi Liang
Zehua Qu
Martijn Kemerink
Ruiqian Guo
Guangzheng Zuo
Two‐Step Design Rule for Simultaneously High Conductivity and Seebeck Coefficient in Conjugated Polymer‐Based Thermoelectrics
Advanced Science
conductivity
energetic disorder
fluorine substitution
organic thermoelectrics
seebeck coefficient
title Two‐Step Design Rule for Simultaneously High Conductivity and Seebeck Coefficient in Conjugated Polymer‐Based Thermoelectrics
title_full Two‐Step Design Rule for Simultaneously High Conductivity and Seebeck Coefficient in Conjugated Polymer‐Based Thermoelectrics
title_fullStr Two‐Step Design Rule for Simultaneously High Conductivity and Seebeck Coefficient in Conjugated Polymer‐Based Thermoelectrics
title_full_unstemmed Two‐Step Design Rule for Simultaneously High Conductivity and Seebeck Coefficient in Conjugated Polymer‐Based Thermoelectrics
title_short Two‐Step Design Rule for Simultaneously High Conductivity and Seebeck Coefficient in Conjugated Polymer‐Based Thermoelectrics
title_sort two step design rule for simultaneously high conductivity and seebeck coefficient in conjugated polymer based thermoelectrics
topic conductivity
energetic disorder
fluorine substitution
organic thermoelectrics
seebeck coefficient
url https://doi.org/10.1002/advs.202409382
work_keys_str_mv AT zelongli twostepdesignruleforsimultaneouslyhighconductivityandseebeckcoefficientinconjugatedpolymerbasedthermoelectrics
AT weifu twostepdesignruleforsimultaneouslyhighconductivityandseebeckcoefficientinconjugatedpolymerbasedthermoelectrics
AT dorotheascheunemann twostepdesignruleforsimultaneouslyhighconductivityandseebeckcoefficientinconjugatedpolymerbasedthermoelectrics
AT xiaoranwei twostepdesignruleforsimultaneouslyhighconductivityandseebeckcoefficientinconjugatedpolymerbasedthermoelectrics
AT maximilianlitterst twostepdesignruleforsimultaneouslyhighconductivityandseebeckcoefficientinconjugatedpolymerbasedthermoelectrics
AT priyamariamviji twostepdesignruleforsimultaneouslyhighconductivityandseebeckcoefficientinconjugatedpolymerbasedthermoelectrics
AT yongcui twostepdesignruleforsimultaneouslyhighconductivityandseebeckcoefficientinconjugatedpolymerbasedthermoelectrics
AT jianhuihou twostepdesignruleforsimultaneouslyhighconductivityandseebeckcoefficientinconjugatedpolymerbasedthermoelectrics
AT junhuitang twostepdesignruleforsimultaneouslyhighconductivityandseebeckcoefficientinconjugatedpolymerbasedthermoelectrics
AT ziqiliang twostepdesignruleforsimultaneouslyhighconductivityandseebeckcoefficientinconjugatedpolymerbasedthermoelectrics
AT zehuaqu twostepdesignruleforsimultaneouslyhighconductivityandseebeckcoefficientinconjugatedpolymerbasedthermoelectrics
AT martijnkemerink twostepdesignruleforsimultaneouslyhighconductivityandseebeckcoefficientinconjugatedpolymerbasedthermoelectrics
AT ruiqianguo twostepdesignruleforsimultaneouslyhighconductivityandseebeckcoefficientinconjugatedpolymerbasedthermoelectrics
AT guangzhengzuo twostepdesignruleforsimultaneouslyhighconductivityandseebeckcoefficientinconjugatedpolymerbasedthermoelectrics