12 research outputs found

    Poly((2-alkylbenzo[1,2,3]triazole-4,7-diyl)vinylene)s for Organic Solar Cells

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    Poly((2-Alkylbenzo[1,2,3]triazole-4,7-diyl)vinylene)s (pBTzVs) synthesized by Stille coupling show different absorption spectra, solid-state morphology, and photovoltaic performance, depending on straight-chain versus branched-chain (pBTzV12 and pBTzV20) pendant substitution. Periodic boundary condition density functional computations show limited alkyl pendant effects on isolated chain electronic properties; however, pendants could influence polymer backbone conjugative planarity and polymer solid film packing. The polymers are electronically ambipolar, with best performance by pBTzV12 with hole and electron transport mobilities of 4.86 x 10(-6) and 1.96 x 10(-6) cm(2) V-1 s(-1), respectively. pBTzV12 gives a smooth film morphology, whereas pBTzV20 gives a very different fibrillar morphology. For ITO/PEDOT:PSS/(1:1 w/w polymer: PC71BM)/LiF/Al devices, pBTzV12 gives power conversion efficiency (PCE) up to 2.87%, and pBTzV20 gives up to PCE = 1.40%; both have open-circuit voltages of V-OC=0.6-0.7 V. (C) 2015 Wiley Periodicals, Inc

    Rigid Core Anthracene and Anthraquinone Linked Nitronyl and Iminoyl Nitroxide Biradicals

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    The first syntheses of bis­(nitronyl nitroxide) and bis­(iminoyl nitroxide) (diNN, diIN) biradicals linked through rigid acene core conjugating anthracene (A) and anthraquinone (AQ) units are reported. Computational modeling predicts weak intramolecular exchange in AQ-linked systems, but A-linked biradicals to have ground state multiplicities consistent with the Borden-Davidson disjointness model. Solution electron spin resonance spectra showed inter-radical exchange-coupled triplet states, except for 2,6-AQ biradicals showing isolated spin spectra. Crystallography of the A-linked biradicals shows a key role for inter-radical contacts for molecular packing. DiINs showed lower-dimensional dyad packing with disorder at the radical units: the conformationally more symmetrical diNNs gave staircase one-dimensional or brickwork two-dimensional lattices. Core anthracene unit stacking was only seen in two systems with bromine on the central anthracene ring: the (large) bromine occupies alternate side placement in dyad stacks for the diIN, chain stacks for the diNN. Magnetism of 2,7-A-linked systems showed predominant ferromagnetic intramolecular triplet-singlet splitting of 24–28 K for diNNs and 8 K for diINs, plus weak antiferromagnetic (AFM) interactions from intermolecular contacts. The 2,6-A-linked biradicals showed AFM exchange between spins. Both A and AQ cores offer possibilities for electronic material development, with a combination of multiple radical spins and π-electron-rich acene cores

    Magnetic Mn and Co Complexes with a Large Polycyclic Aromatic Substituted Nitronylnitroxide

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    2-(1′-Pyrenyl)-4,4,5,5-tetramethyl-4,5-dihydro-1<i>H</i>-imidazole-3-oxide-1-oxyl (PyrNN) was reacted with M­(hfac)<sub>2</sub> (M = Mn­(II) and Co­(II), hfac = hexafluoracetylacetonate) to give two isostructural ML<sub>2</sub> stoichiometry M­(hfac)<sub>2</sub>(PyrNN)<sub>2</sub> complexes and a ML stoichiometry one-dimensional (1-D) polymer chain complex [Mn­(hfac)<sub>2</sub>(PyrNN)]. The ML<sub>2</sub> complexes have similar crystal structures with monoclinic unit cells, in which one NO unit from each PyrNN ligand is bonded to the transition metal on cis vertices of a distorted octahedron. The major magnetic interactions are intracomplex metal-to-radical exchange (<i>J</i>), and intermolecular exchange across a close contact between the uncoordinated NO units (<i>J</i>′). For M = Mn­(II) an approximate chain model fit gives <i>g</i> = 2.0, <i>J</i> = (−)­125 cm<sup>–1</sup> and <i>J</i>′ = (−)­49 cm<sup>–1</sup>; for M = Co­(II), <i>g</i> = 2.4, <i>J</i> = (−)­180 cm<sup>–1</sup>, and <i>J</i>′ = (−)­70 cm<sup>–1</sup>. Hybrid density functional theory (DFT) computations modeling the intermolecular exchange by using only the radical units across the close contact are in good accord with the estimated values of <i>J</i>′. The chain type complex structure shows solvent incorporation for overall structure [Mn­(hfac)<sub>2</sub>(PyrNN)]<sub><i>n</i></sub>·0.5­(CHCl<sub>3</sub>)·0.5­(C<sub>7</sub>H<sub>16</sub>). Both NO groups of the PyrNN ligand are complexed to form helical chains, with very strong metal to radical antiferromagnetic exchange that gives overall ferrimagnetic behavior

    Magnetic Mn and Co Complexes with a Large Polycyclic Aromatic Substituted Nitronylnitroxide

    No full text
    2-(1′-Pyrenyl)-4,4,5,5-tetramethyl-4,5-dihydro-1<i>H</i>-imidazole-3-oxide-1-oxyl (PyrNN) was reacted with M­(hfac)<sub>2</sub> (M = Mn­(II) and Co­(II), hfac = hexafluoracetylacetonate) to give two isostructural ML<sub>2</sub> stoichiometry M­(hfac)<sub>2</sub>(PyrNN)<sub>2</sub> complexes and a ML stoichiometry one-dimensional (1-D) polymer chain complex [Mn­(hfac)<sub>2</sub>(PyrNN)]. The ML<sub>2</sub> complexes have similar crystal structures with monoclinic unit cells, in which one NO unit from each PyrNN ligand is bonded to the transition metal on cis vertices of a distorted octahedron. The major magnetic interactions are intracomplex metal-to-radical exchange (<i>J</i>), and intermolecular exchange across a close contact between the uncoordinated NO units (<i>J</i>′). For M = Mn­(II) an approximate chain model fit gives <i>g</i> = 2.0, <i>J</i> = (−)­125 cm<sup>–1</sup> and <i>J</i>′ = (−)­49 cm<sup>–1</sup>; for M = Co­(II), <i>g</i> = 2.4, <i>J</i> = (−)­180 cm<sup>–1</sup>, and <i>J</i>′ = (−)­70 cm<sup>–1</sup>. Hybrid density functional theory (DFT) computations modeling the intermolecular exchange by using only the radical units across the close contact are in good accord with the estimated values of <i>J</i>′. The chain type complex structure shows solvent incorporation for overall structure [Mn­(hfac)<sub>2</sub>(PyrNN)]<sub><i>n</i></sub>·0.5­(CHCl<sub>3</sub>)·0.5­(C<sub>7</sub>H<sub>16</sub>). Both NO groups of the PyrNN ligand are complexed to form helical chains, with very strong metal to radical antiferromagnetic exchange that gives overall ferrimagnetic behavior

    Sensing of proteins in human serum using conjugates of nanoparticles and green fluorescent protein

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    There is a direct correlation between protein levels and disease states in human serum, which makes it an attractive target for sensors and diagnostics. However, this is challenging because serum features more than 20,000 proteins, with an overall protein content greater than 1 mM. Here we report a sensor based on a hybrid synthetic–biomolecule that uses arrays of green fluorescent protein and nanoparticles to detect proteins at biorelevant concentrations in both buffer and human serum. Distinct and reproducible fluorescence-response patterns were obtained from five serum proteins (human serum albumin, immunoglobulin G, transferrin, fibrinogen and α-antitrypsin), both in buffer and when spiked into human serum. Using linear discriminant analysis we identified these proteins with an identification accuracy of 100% in buffer and 97% in human serum. The arrays were also able to discriminate between different concentrations of the same protein, as well as a mixture of different proteins in human seru
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