4.8 Article

Preferential Location of Dopants in the Amorphous Phase of Oriented Regioregular Poly(3-hexylthiophene-2,5-diyl) Films Helps Reach Charge Conductivities of 3000 S cm-1

Journal

ADVANCED FUNCTIONAL MATERIALS
Volume 32, Issue 30, Pages -

Publisher

WILEY-V C H VERLAG GMBH
DOI: 10.1002/adfm.202202075

Keywords

doping; organic thermoelectrics; polymer semiconductors; thin films; transmission electron microscopy

Funding

  1. ANR [ANR -17-CE05-0012, ANR-19-CE05-0036]
  2. European Commission through Marie Sklodowska-Curie project HORATES [GA-955837]
  3. Agence Nationale de la Recherche (ANR) [ANR-19-CE05-0036] Funding Source: Agence Nationale de la Recherche (ANR)

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This contribution demonstrates that doping of oriented semicrystalline P3HT thin films can enhance charge conductivities and thermoelectric power factors. The doping mechanism is found to be intimately related to the semicrystalline structure of the polymer, and preferential doping of the amorphous phase can improve charge mobilities and thermoelectric power factors.
Doping polymer semiconductors is a central topic in plastic electronics and especially in the design of novel thermoelectric (TE) materials. In this contribution, it has been demonstrated that doping of oriented semicrystalline P3HT thin films with the dopant tris(4-bromophenyl)ammoniumyl hexachloroantimonate), known as magic blue (MB), helps reach charge conductivities of 3000 S cm(-1) and TE power factors of 170 +/- 30 mu W mK(-2) along the polymer chain direction. A combination of transmission electron microscopy, polarized optical absorption spectroscopy, Rutherford backscattering, and TE property measurements helps clarify the conditions necessary to achieve such high charge conductivities. A comparative study with different dopants demonstrates that the doping mechanism is intimately related to the semicrystalline structure of the polymer and whether crystalline, amorphous or both phases are doped. The highest charge mobilities are observed when the dopant MB is preferentially located in the amorphous phase of P3HT, leaving the structure of P3HT nanocrystals almost unaltered. In this case, the P3HT nanocrystals are doped from their interface with the surrounding amorphous phase. These results indicate that doping preferentially the amorphous phase of semicrystalline polymer semiconductors is an effective strategy to reduce polaron localization, enhance charge mobilities, and improve TE power factors.

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