2023
DOI: 10.1039/d2tc03684c
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P- and N-dopable ambipolar bulk heterojunction thermoelectrics based on ladder-type conjugated polymers

Abstract: Ambipolar bulk heterojunction polymer thermoelectrics was demonstrated for the first time using the classic n-type poly(benzimidazobenzophenanthrolinedione) ladder polymer (BBL) and the new p-type 6H-pyrrolo[3,2-b:4,5-b′]bis[1,4]benzothiazine ladder polymer (PBBTL). The blend films...

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Cited by 10 publications
(12 citation statements)
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“…Ladder-type conjugated polymers (LCPs) are a promising class of conjugated polymers where the polymer backbone is composed of double-stranded fused-ring structure that limits its torsional rotation. Because of this, LCPs usually have highly rigid coplanar conformations that exhibit excellent mechanical properties, as well as thermal and chemical stability. Coplanar polymer backbones can extend intrachain delocalization that facilitate intrachain charge transfer and are also beneficial for strong π–π interactions that promote interchain charge transport. These unique advantages render ladder-type conjugated polymers as highly promising in organic electronic devices including organic thin film transistors (OTFTs), , organic electrochemical transistors (OECTs), , organic thermoelectrics (OTEs), lithium-/sodium-ion batteries (LIBs/SIBs), and supercapacitors. , However, the greatest challenge for LCPs synthesis and characterization is insolubility, either due to cross-linking or high molecular weight. The latter becomes an issue when the π-system in each repeating unit becomes too big.…”
mentioning
confidence: 99%
“…Ladder-type conjugated polymers (LCPs) are a promising class of conjugated polymers where the polymer backbone is composed of double-stranded fused-ring structure that limits its torsional rotation. Because of this, LCPs usually have highly rigid coplanar conformations that exhibit excellent mechanical properties, as well as thermal and chemical stability. Coplanar polymer backbones can extend intrachain delocalization that facilitate intrachain charge transfer and are also beneficial for strong π–π interactions that promote interchain charge transport. These unique advantages render ladder-type conjugated polymers as highly promising in organic electronic devices including organic thin film transistors (OTFTs), , organic electrochemical transistors (OECTs), , organic thermoelectrics (OTEs), lithium-/sodium-ion batteries (LIBs/SIBs), and supercapacitors. , However, the greatest challenge for LCPs synthesis and characterization is insolubility, either due to cross-linking or high molecular weight. The latter becomes an issue when the π-system in each repeating unit becomes too big.…”
mentioning
confidence: 99%
“…Demand for n-type dopants for efficient and stable doping is increasing since the device applications such as OLEDs, [26][27][28][29] complementary circuits, [30][31][32] and thermoelectric generation all simultaneously require both p-and n-doping. [33][34][35] Even though various materials and methods were introduced for ntype doping of OSCs such as (i) using alkali metals, [36][37][38] (ii) molecular compounds with significantly shallow HOMO, [39][40][41][42][43] and (iii) air-stable precursor molecules that can donate an electron to the matrix material in the deposited film, [44][45][46] we focus here on the latter two due to the doping stability of alkali metals, 47) One of the earliest works on n-type molecular dopants with low IE is bis(cyclopentadienyl)-cobalt(ΙΙ) (cobaltocene, CoCp 2 ), which is a strong reducing agent with an ionization energy of about 4 eV, and an n-type dopant capable of shifting the Fermi level of OSC by 0.5 eV to the conduction band. 43) In addition, interfacial doping of CoCp 2 reduced the charge injection barrier at the Au/PEDOT:PSS interface, demonstrating decent current enhancement that is comparable to that of p-doping of N,N′-diphenyl-N,N′-bis(1-naphthyl) −1,1′-bi-phenyl-4,4′diamine (α-NPD) with F 4 TCNQ.…”
Section: P-type Molecular Dopantsmentioning
confidence: 99%
“…These include: thermoelectric materials, which generate electrical signals in response to temperature changes; thermoresponsive deformation materials, which undergo structural changes with temperature variation; thermochromic materials, which exhibit color changes with temperature fluctuations; and thermistor materials, which display changes in electrical resistance based on temperature alterations. [20][21][22][23][24][25][26][27][28][29][30][31][32][33][34][35][36][37][38] However, relying solely on a single temperature-sensing material restricts the ability to accurately identify and monitor potential electrical hazards and health risks in the presence of complex indoor temperature a College of Materials Science and Engineering, Shenzhen University, Shenzhen 518055, China. E-mail: iouydu@szu.edu.cn, chengm@szu.edu.cn b College of Civil and Transportation Engineering, Shenzhen University, Shenzhen 518060, China † Electronic supplementary information (ESI) available.…”
Section: Introductionmentioning
confidence: 99%