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How to measure absolute P3HT crystallinity via 13 C CPMAS NMR
Author(s) -
Nieuwendaal Ryan C.
Publication year - 2016
Publication title -
magnetic resonance in chemistry
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.483
H-Index - 72
eISSN - 1097-458X
pISSN - 0749-1581
DOI - 10.1002/mrc.4443
Subject(s) - chemistry , measure (data warehouse) , crystallinity , absolute (philosophy) , nuclear magnetic resonance spectroscopy , analytical chemistry (journal) , nuclear magnetic resonance , stereochemistry , crystallography , organic chemistry , physics , data mining , philosophy , epistemology , computer science
We outline the details of acquiring quantitative 13 C cross‐polarization magic angle spinning (CPMAS) nuclear magnetic resonance on the most ubiquitous polymer for organic electronic applications, poly(3‐hexylthiophene) (P3HT), despite other groups' claims that CPMAS of P3HT is strictly nonquantitative. We lay out the optimal experimental conditions for measuring crystallinity in P3HT, which is a parameter that has proven to be critical in the electrical performance of P3HT‐containing organic photovoltaics but remains difficult to measure by scattering/diffraction and optical methods despite considerable efforts. Herein, we overview the spectral acquisition conditions of the two P3HT films with different crystallinities (0.47 and 0.55) and point out that because of the chemical similarity of P3HT to other alkyl side chain, highly conjugated main chain polymers, our protocol could straightforwardly be extended to other organic electronic materials. Variable temperature 1 H NMR results are shown as well, which (i) yield insight into the molecular dynamics of P3HT, (ii) add context for spectral editing techniques as applied to quantifying crystallinity, and (iii) show why T 1ρ H , the 1 H spin–lattice relaxation time in the rotating frame, is a more optimal relaxation filter for distinguishing between crystalline and noncrystalline phases of highly conjugated alkyl side‐chain polymers than other relaxation times such as the 1 H spin–spin relaxation time, T 2 H , and the spin–lattice relaxation time in the toggling frame, T 1xz H . A 7 ms T 1ρ H spin lock filter, prior to CPMAS, allows for spectroscopic separation of crystalline and noncrystalline 13 C nuclear magnetic resonance signals. Published 2016. This article is a U.S. Government work and is in the public domain in the USA.