Kumar Pawan, Abutaha Anas, Wu Gang, Gordon Madeleine P, Recatala-Gomez Jose, Urban Jeffrey J, Hippalgaonkar Kedar
Institute of Materials Research and Engineering, Agency for Science Technology and Research, 2 Fusionopolis Way, 08-03 Innovis, Singapore 138634, Singapore.
Qatar Environment and Energy Research Institute (QEERI), Hamad Bin Khalifa University (HBKU), Post Office Box 34110, Doha, Qatar.
ACS Appl Mater Interfaces. 2025 Feb 12;17(6):9431-9439. doi: 10.1021/acsami.4c20823. Epub 2025 Jan 29.
Thermoelectric properties of conducting polymers typically suffer from molecular chain disordering, as charge transport is predominantly controlled by morphology. This is especially more problematic when counterions are introduced to tune the carrier concentration for optimal thermoelectric performance, which disturbs the morphology further. In this work, we introduce a new avenue for enhancing thermoelectric properties without needing to regulate the morphology, namely, by controlling the coulombic interaction between polarons and counterions. We perform de-doping thermoelectric experiments over 3 orders of magnitude change in electrical conductivity of three distinct thermoelectric polymers, namely, poly(3-hexylthiophene-2,5-diyl) (P3HT), poly[2,5-bis(3-dodecylthiophen-2-yl)thieno[3,2-]thiophene] (PBTTT-C), and poly[2,5-(2-octyldodecyl)-3,6-diketopyrrolopyrrole--5,5-(2,5-di(thien-2-yl)thieno[3,2-]thiophene)] (OD-PDPP2T-TT) conjugated polymers, followed by grazing-incidence wide-angle X-ray scattering (GIWAXS) to study their respective morphologies. We demonstrate a 9-fold enhancement in the thermoelectric power factor in OD-PDPP2T-TT compared to PBTTT-C and link it to the coulombic screening of charge carriers, including in the optimally doped regime. We support this hypothesis using Boltzmann transport equations and show that, in both P3HT and PBTTT-C, as the polymer is doped, impurity scattering remains the dominant scattering mechanism, while in OD-PDPP2T-TT, the scattering mechanism changes from impurity to acoustic phonon limited, resulting in more effective screening of ionized counterions. Our results provide an additional knob to enhance the fundamental understanding of thermoelectric physics of conducting polymers and provide a pathway to achieve higher performance in the field of organic thermoelectrics.
导电聚合物的热电性能通常会受到分子链无序的影响,因为电荷传输主要由形态控制。当引入抗衡离子以调节载流子浓度以实现最佳热电性能时,这一问题尤其严重,因为这会进一步扰乱形态。在这项工作中,我们引入了一条无需调节形态即可增强热电性能的新途径,即通过控制极化子与抗衡离子之间的库仑相互作用。我们对三种不同的热电聚合物,即聚(3-己基噻吩-2,5-二基)(P3HT)、聚[2,5-双(3-十二烷基噻吩-2-基)噻吩并[3,2-]噻吩](PBTTT-C)和聚[2,5-(2-辛基十二烷基)-3,6-二酮吡咯并吡咯-5,5-(2,5-二(噻吩-2-基)噻吩并[3,2-]噻吩](OD-PDPP2T-TT)共轭聚合物,在电导率变化超过3个数量级的范围内进行了去掺杂热电实验,随后进行掠入射广角X射线散射(GIWAXS)以研究它们各自的形态。我们证明,与PBTTT-C相比,OD-PDPP2T-TT的热电功率因数提高了9倍,并将其与电荷载流子的库仑屏蔽联系起来,包括在最佳掺杂状态下。我们使用玻尔兹曼输运方程支持这一假设,并表明,在P3HT和PBTTT-C中,随着聚合物的掺杂,杂质散射仍然是主要的散射机制,而在OD-PDPP2T-TT中,散射机制从杂质散射转变为声子散射受限,从而导致对电离抗衡离子的更有效屏蔽。我们的结果为增强对导电聚合物热电物理的基本理解提供了一个额外的手段,并为在有机热电领域实现更高性能提供了一条途径。