PMID-sentid Pub_year Sent_text comp_official_name comp_offsetprotein_name organism prot_offset 31261759-5 2019 On the contrary, in the latter case, due to higher viscosity of the solution, mechanical stretching induced on the polymer during spin-coating deposition is the main factor inducing self-alignment of the beta-phase. Polymers 115-122 spindlin 1 Homo sapiens 130-134 31161171-0 2019 Spin crossover and photomagnetic behaviors in one-dimensional looped coordination polymers. Polymers 82-90 spindlin 1 Homo sapiens 0-4 30628435-0 2019 Anisotropic Magnetoresistance in NiFe-Based Polymer Spin Valves. Polymers 44-51 spindlin 1 Homo sapiens 52-56 30628435-4 2019 These findings suggest that the mechanisms responsible for the transport mode in polymer spin-valve devices also strongly depend on the interface between the ferromagnetic electrodes and organic semiconductor layer. Polymers 81-88 spindlin 1 Homo sapiens 89-93 30511863-0 2018 Diffusion of Rodlike Polymers: Pulsed Gradient Spin Echo NMR of Poly(gamma-stearyl-alpha,l-glutamate) Solutions and the Importance of Helix Stability. Polymers 21-29 spindlin 1 Homo sapiens 47-51 30328634-0 2018 Filtering the NMR Spectra of Complex Mixtures through Polymer-Mediated Paramagnetic Spin Relaxation. Polymers 54-61 spindlin 1 Homo sapiens 84-88 30328634-1 2018 A polymer-mediated paramagnetic spin relaxation (PSR) filter is presented for the selective suppression of signals from polymer-interacting species in the 1D and 2D NMR spectra of mixtures. Polymers 2-9 spindlin 1 Homo sapiens 32-36 30328634-1 2018 A polymer-mediated paramagnetic spin relaxation (PSR) filter is presented for the selective suppression of signals from polymer-interacting species in the 1D and 2D NMR spectra of mixtures. Polymers 120-127 spindlin 1 Homo sapiens 32-36 30673291-5 2019 It is found that for up to particle diameters of a few micrometers, particle deposition can be described by a theoretical approach developed for the spin-casting of polymer solutions (Karpitschka, S.; Weber, C. M.; Riegler, H. Chem. Polymers 165-172 spindlin 1 Homo sapiens 149-153 30645012-4 2019 The fabrication of a spin-OLED that uses a conjugated polymer as bipolar spin collector layer and ferromagnetic electrodes is reported here. Polymers 54-61 spindlin 1 Homo sapiens 21-25 30645012-4 2019 The fabrication of a spin-OLED that uses a conjugated polymer as bipolar spin collector layer and ferromagnetic electrodes is reported here. Polymers 54-61 spindlin 1 Homo sapiens 73-77 30192035-4 2018 Moreover, they quantify the interchain interaction mediated by the terminal nitroxide group of two spin triads in neighboring polymer chains. Polymers 126-133 spindlin 1 Homo sapiens 99-103 30401913-2 2018 Spin-coated thin films of ethyl-violet molecules dispersed in a polymer host (EV) were used as cubic nonlinear optical media because of their transparency at both the fundamental (1230 nm) and the third harmonic (410 nm) wavelengths. Polymers 64-71 spindlin 1 Homo sapiens 0-4 29727182-0 2018 Isotropic Effective Spin-Orbit Coupling in a Conjugated Polymer. Polymers 56-63 spindlin 1 Homo sapiens 20-24 29577465-3 2018 The light-responsive spin-silenced polymer is synthesized via an Ugi post-polymerization modification incorporating paramagnetic nitroxides and a light cleavable fluorophore moiety. Polymers 35-42 spindlin 1 Homo sapiens 21-25 29633838-1 2018 The rate of the light-induced spin transition in a coordination polymer network solid dramatically increases when included as the core in mesoscale core-shell particles. Polymers 64-71 spindlin 1 Homo sapiens 30-34 29656407-3 2018 The crosslinked high-performance polymers (SPIN) are constructed by using cation-pi interactions. Polymers 33-41 spindlin 1 Homo sapiens 43-47 29505264-0 2018 Toward Achieving Highly Ordered Fluorinated Surfaces of Spin-Coated Polymer Thin Films by Optimizing the Air/Liquid Interfacial Structure of the Casting Solutions. Polymers 68-75 spindlin 1 Homo sapiens 56-60 29505264-1 2018 Thin polymer films with well-assembled fluorinated groups on their surfaces are not easily achieved via spin-coating film-fabrication methods because the solution solidifies very rapidly during spin-coating, which hinders the fluorinated moieties from segregating and organizing on the film surface. Polymers 5-12 spindlin 1 Homo sapiens 194-198 28346780-0 2017 High-Spin Polymers: Ferromagnetic Coupling of S = 1 Hexaazacyclophane Units up to a Pure S = 2 Polycyclophane. Polymers 10-18 spindlin 1 Homo sapiens 5-9 28594451-0 2017 Two-Step Spin-Crossover with Three Inequivalent FeII Sites in a Two-Dimensional Hofmann-Type Coordination Polymer. Polymers 106-113 spindlin 1 Homo sapiens 9-13 28346780-6 2017 Most importantly, in this polymer, four spins can be ferromagnetically ordered via both couplers, which leads to the high spin state. Polymers 26-33 spindlin 1 Homo sapiens 40-44 27351974-0 2016 Orthogonally Spin-Coated Bilayer Films for Photochemical Immobilization and Patterning of Sub-10-Nanometer Polymer Monolayers. Polymers 107-114 spindlin 1 Homo sapiens 13-17 28032750-0 2017 Surface-Mediated Solidification of a Semiconducting Polymer during Time-Controlled Spin-Coating. Polymers 52-59 spindlin 1 Homo sapiens 83-87 28032750-1 2017 Spin-casting a polymer semiconductor solution over a short period of only a few seconds dramatically improved the molecular ordering and charge transport properties of the resulting semiconductor thin films. Polymers 15-22 spindlin 1 Homo sapiens 0-4 27417666-0 2017 Guest-Dependent Spin-Transition Behavior of Porous Coordination Polymers. Polymers 64-72 spindlin 1 Homo sapiens 16-20 27417666-1 2017 The host-guest composites of Hofmann-type iron(II) spin-transition (ST) porous coordination polymers incorporating guest molecules show guest-dependent ST behavior in accordance with the respective guest species, which may be a gas, solvent, halogen, or organic molecule. Polymers 92-100 spindlin 1 Homo sapiens 51-55 27819367-5 2016 A control of the spin crossover properties can be achieved by precise tuning of the crystallinity of the coordination polymer via successive addition of the starting material Fe(L) and bipy. Polymers 118-125 spindlin 1 Homo sapiens 17-21 27819367-7 2016 Furthermore, the use of blockcopolymers allows a further functionalization of the obtained nanoparticles by variation of the polymer blocks and an easy deposition of the composite material on surfaces via spin coating. Polymers 31-38 spindlin 1 Homo sapiens 205-209 27499328-7 2017 Our own studies on this subject are enabled by the application of magnetic resonance relaxometry methods relying on spin labels tethered to polyelectrolyte constituents or added as spin labeled probe molecules that partition into the dense versus the equilibrium coacervate phase, permitting the extraction of information on local polymer dynamics, polymer packing and local water dynamics. Polymers 331-338 spindlin 1 Homo sapiens 116-120 27499328-7 2017 Our own studies on this subject are enabled by the application of magnetic resonance relaxometry methods relying on spin labels tethered to polyelectrolyte constituents or added as spin labeled probe molecules that partition into the dense versus the equilibrium coacervate phase, permitting the extraction of information on local polymer dynamics, polymer packing and local water dynamics. Polymers 331-338 spindlin 1 Homo sapiens 181-185 27499328-7 2017 Our own studies on this subject are enabled by the application of magnetic resonance relaxometry methods relying on spin labels tethered to polyelectrolyte constituents or added as spin labeled probe molecules that partition into the dense versus the equilibrium coacervate phase, permitting the extraction of information on local polymer dynamics, polymer packing and local water dynamics. Polymers 349-356 spindlin 1 Homo sapiens 116-120 27499328-7 2017 Our own studies on this subject are enabled by the application of magnetic resonance relaxometry methods relying on spin labels tethered to polyelectrolyte constituents or added as spin labeled probe molecules that partition into the dense versus the equilibrium coacervate phase, permitting the extraction of information on local polymer dynamics, polymer packing and local water dynamics. Polymers 349-356 spindlin 1 Homo sapiens 181-185 27184565-3 2016 This study demonstrates the feasibility of preparing a hyperpolarized [1-(13) C]2-methylpropan-2-ol (tert-butanol) solution free of persistent radicals by using spin-labeled thermoresponsive hydrophilic polymer networks as polarizing agents. Polymers 203-210 spindlin 1 Homo sapiens 161-165 26437656-1 2015 UNLABELLED: Aqueous dispersion of conductive polymer poly(3,4-ethylenedioxythiophene)-poly(styrenesulfonate) ( PEDOT: PSS) was deposited on spin-coated and drop cast nanofibrillar cellulose (NFC)-glycerol (G) matrix on a glass substrate. Polymers 45-52 spindlin 1 Homo sapiens 140-144 26905980-0 2016 Spin-Casting Polymer Brush Films for Stimuli-Responsive and Anti-Fouling Surfaces. Polymers 13-20 spindlin 1 Homo sapiens 0-4 26905980-2 2016 Herein, a series of well-defined amphiphilic asymmetric polymer brushes containing hetero side chains, hydrophobic polystyrene (PS) and hydrophilic poly(ethylene glycol) (PEG), was employed to prepare uniform thin films by spin-casting. Polymers 56-63 spindlin 1 Homo sapiens 223-227 26335946-0 2015 Depolymerization of Free-Radical Polymers with Spin Migrations. Polymers 33-41 spindlin 1 Homo sapiens 47-51 26523547-3 2015 Nevertheless, the interface resistance between the polymer and metallic electrodes is orders of magnitudes larger than the expected spin resistance of the active channel. Polymers 51-58 spindlin 1 Homo sapiens 132-136 26505645-3 2015 Spin-coated two-dimensional non-close-packed colloidal crystals are utilized as etching masks to pattern subwavelength-structured cone arrays directly on polymer substrates. Polymers 154-161 spindlin 1 Homo sapiens 0-4 26445886-0 2015 Influence of conformational changes on spin crossover properties and superstructure formation in 2D coordination polymers [Fe(hbtz)2(RCN)2](ClO4)2. Polymers 113-121 spindlin 1 Homo sapiens 39-43 27358736-0 2015 Unravelling the chemical design of spin-crossover nanoparticles based on iron(ii)-triazole coordination polymers: towards a control of the spin transition. Polymers 104-112 spindlin 1 Homo sapiens 35-39 27358736-0 2015 Unravelling the chemical design of spin-crossover nanoparticles based on iron(ii)-triazole coordination polymers: towards a control of the spin transition. Polymers 104-112 spindlin 1 Homo sapiens 139-143 26172431-0 2015 Homoleptic Iron(II) Complexes with the Ionogenic Ligand 6,6"-Bis(1H-tetrazol-5-yl)-2,2"-bipyridine: Spin Crossover Behavior in a Singular 2D Spin Crossover Coordination Polymer. Polymers 169-176 spindlin 1 Homo sapiens 100-104 25868686-0 2015 Probing long-range carrier-pair spin-spin interactions in a conjugated polymer by detuning of electrically detected spin beating. Polymers 71-78 spindlin 1 Homo sapiens 32-36 25868686-0 2015 Probing long-range carrier-pair spin-spin interactions in a conjugated polymer by detuning of electrically detected spin beating. Polymers 71-78 spindlin 1 Homo sapiens 37-41 25868686-0 2015 Probing long-range carrier-pair spin-spin interactions in a conjugated polymer by detuning of electrically detected spin beating. Polymers 71-78 spindlin 1 Homo sapiens 37-41 24144347-3 2013 Moreover, we found that a low doping of spin radicals in polymer MEH-PPV causes a significant change on the MFC signal: an amplitude increase and a line-shape narrowing under light illumination at room temperature. Polymers 57-64 spindlin 1 Homo sapiens 40-44 25183547-0 2014 Spin crossover probes confer multistability to organic conducting polymers. Polymers 66-74 spindlin 1 Homo sapiens 0-4 24695952-2 2014 The new method, called Spin Echo Small Angle Neutron Scattering (SESANS) provides accurate information about particle composition, including the degree of solvent penetration into the polymer brush grafted on to the PMMA spheres to prevent aggregation. Polymers 184-191 spindlin 1 Homo sapiens 23-27 22486959-4 2012 Spin-lattice relaxation times of the protons in the hydrogel, detected by solid state NMR, are indicative of mobility within the polymer. Polymers 129-136 spindlin 1 Homo sapiens 0-4 23897214-6 2013 These coordination polymers show a spin-canting antiferromagnetism and metamagnetism behaviour for Co(II) and HS HS/LS LS spin-crossover phenomena for Fe(II), respectively. Polymers 19-27 spindlin 1 Homo sapiens 35-39 23897214-6 2013 These coordination polymers show a spin-canting antiferromagnetism and metamagnetism behaviour for Co(II) and HS HS/LS LS spin-crossover phenomena for Fe(II), respectively. Polymers 19-27 spindlin 1 Homo sapiens 126-130 23644525-4 2013 Here we show that a pure spin current can be produced in a solution-processed conducting polymer by pumping spins through a ferromagnetic resonance in an adjacent magnetic insulator, and that this generates an electric voltage across the polymer film. Polymers 89-96 spindlin 1 Homo sapiens 25-29 23644525-4 2013 Here we show that a pure spin current can be produced in a solution-processed conducting polymer by pumping spins through a ferromagnetic resonance in an adjacent magnetic insulator, and that this generates an electric voltage across the polymer film. Polymers 238-245 spindlin 1 Homo sapiens 25-29 23644525-5 2013 We demonstrate that the experimental characteristics of the generated voltage are consistent with it being generated through an inverse spin Hall effect in the conducting polymer. Polymers 171-178 spindlin 1 Homo sapiens 136-140 23644525-6 2013 In contrast with inorganic materials, the conducting polymer exhibits coexistence of high spin-current to charge-current conversion efficiency and long spin lifetimes. Polymers 53-60 spindlin 1 Homo sapiens 90-94 23644525-6 2013 In contrast with inorganic materials, the conducting polymer exhibits coexistence of high spin-current to charge-current conversion efficiency and long spin lifetimes. Polymers 53-60 spindlin 1 Homo sapiens 152-156 23205911-3 2012 The presence of meta-phenylenes in the polymer chemical structure allows for the ferromagnetic coupling of electronic spins, which leads to the formation of high spin states. Polymers 39-46 spindlin 1 Homo sapiens 118-122 23205911-5 2012 Quantitative magnetization measurements reveal that the doped polymer contains mainly S = 2 spin states and a fraction of S = 3/2 spin states. Polymers 62-69 spindlin 1 Homo sapiens 92-96 23205911-5 2012 Quantitative magnetization measurements reveal that the doped polymer contains mainly S = 2 spin states and a fraction of S = 3/2 spin states. Polymers 62-69 spindlin 1 Homo sapiens 130-134 23205911-7 2012 To the best of our knowledge, this polymer is the first example of a linear doped polyarylamine combining such high spin states with high doping efficiency. Polymers 35-42 spindlin 1 Homo sapiens 116-120 21888426-3 2011 Spin-coated polymer films such as poly(methyl methacrylate), high-impact polystyrene or acrylonitrile-butadiene-styrene, or gas-phase methane were used as carbon sources. Polymers 12-19 spindlin 1 Homo sapiens 0-4 22755597-0 2012 Spin-dependent polaron recombination in conjugated polymers. Polymers 51-59 spindlin 1 Homo sapiens 0-4 21303156-8 2011 These results strongly propose that there is a new way for the organic polymer to be applied as a spin-filter. Polymers 71-78 spindlin 1 Homo sapiens 98-102 20862430-6 2010 The proposed model qualitatively describes the main scenario of spin crossover effect in the chain polymer heterospin complex of copper(ii) hexafluoroacetylacetonate with methyl pyrazol-substituted nitronyl nitroxide containing two-spin exchange clusters. Polymers 99-106 spindlin 1 Homo sapiens 64-68 20862430-6 2010 The proposed model qualitatively describes the main scenario of spin crossover effect in the chain polymer heterospin complex of copper(ii) hexafluoroacetylacetonate with methyl pyrazol-substituted nitronyl nitroxide containing two-spin exchange clusters. Polymers 99-106 spindlin 1 Homo sapiens 113-117 20872039-5 2010 This modelling approach revealed that the width of the polymer/polymer interfaces formed by spin coating was in the range 15-20nm. Polymers 55-62 spindlin 1 Homo sapiens 92-96 21231063-2 2010 The resonance at g = 2.0028(3) is due to polarons in the polymer, and exhibits spin locking at high microwave fields. Polymers 57-64 spindlin 1 Homo sapiens 79-83 20872039-0 2010 Thin film polymer photonics: Spin cast distributed Bragg reflectors and chirped polymer structures. Polymers 10-17 spindlin 1 Homo sapiens 29-33 20872039-1 2010 Polymer based photonic structures were produced by spin coating up to 50 alternating layers of polystyrene (PS) and poly(vinylpyrrolidone) (PVP) from mutually exclusive (orthogonal) solvents. Polymers 0-7 spindlin 1 Homo sapiens 51-55 20872039-5 2010 This modelling approach revealed that the width of the polymer/polymer interfaces formed by spin coating was in the range 15-20nm. Polymers 63-70 spindlin 1 Homo sapiens 92-96 19831361-2 2009 Variable-temperature magnetic susceptibility measurements demonstrate that spin-crossover is operative in the polymer film, and resistivity measurements on indium-tin oxide coated glass slides containing the polymer film exhibit intriguing temperature-dependent profiles. Polymers 110-117 spindlin 1 Homo sapiens 75-79 20549004-1 2010 A kind of spin crossover-macromolecule polymer composite material, [Fe(NH(2)trz)(3)(ClO(4))(2)]-PVP (NH(2)trz is 4-amino-1,2,4-triazole and PVP is polyvinylpyrrolidone), appears as homogeneous film with a regular structure in nano-scale and shows the spin crossover (SC) phenomenon. Polymers 39-46 spindlin 1 Homo sapiens 10-14 20687680-0 2010 Second-harmonic generation in conjugated polymer films: A sensitive probe of how bulk polymer crystallinity changes with spin speed. Polymers 41-48 spindlin 1 Homo sapiens 121-125 20687680-0 2010 Second-harmonic generation in conjugated polymer films: A sensitive probe of how bulk polymer crystallinity changes with spin speed. Polymers 86-93 spindlin 1 Homo sapiens 121-125 20568878-0 2009 Spin-flip processes of polarons by magnetic impurities in conjugated polymers. Polymers 69-77 spindlin 1 Homo sapiens 0-4 20568878-1 2009 By employing an adaptive time-dependent density-matrix-renormalization-group method, the spin-flip process of polarons is investigated in a polymer chain with magnetic impurities. Polymers 140-147 spindlin 1 Homo sapiens 89-93 20568878-2 2009 Being driven by an external electric field, a polaron carrying both spin 1/2 and charge +/-e moves at a constant speed in the polymer chain. Polymers 126-133 spindlin 1 Homo sapiens 68-76 19831361-2 2009 Variable-temperature magnetic susceptibility measurements demonstrate that spin-crossover is operative in the polymer film, and resistivity measurements on indium-tin oxide coated glass slides containing the polymer film exhibit intriguing temperature-dependent profiles. Polymers 208-215 spindlin 1 Homo sapiens 75-79 15778714-0 2005 Spin-conserving carrier recombination in conjugated polymers. Polymers 52-60 spindlin 1 Homo sapiens 0-4 19070468-2 2009 The fluctuations of this operator are responsible for spin-lattice relaxation in polymer chains. Polymers 81-88 spindlin 1 Homo sapiens 54-58 19070468-5 2009 It is shown that these non-local chain modes dominate proton spin-lattice relaxation dispersion of flexible polymers at frequencies up to about 10(8)Hz. Polymers 108-116 spindlin 1 Homo sapiens 61-65 18711386-0 2008 Spin Rabi flopping in the photocurrent of a polymer light-emitting diode. Polymers 44-51 spindlin 1 Homo sapiens 0-4 18692367-1 2008 The use of spin-diffusion NMR for the measurement of domain sizes in multiphase materials is becoming increasingly popular, in particular for the study of heterogeneous polymers. Polymers 169-177 spindlin 1 Homo sapiens 11-15 18201075-1 2008 Spin-coating one polymer solution on another spin-cast polymer film is believed to result in unfavorable interfacial mixing. Polymers 17-24 spindlin 1 Homo sapiens 0-4 18201075-1 2008 Spin-coating one polymer solution on another spin-cast polymer film is believed to result in unfavorable interfacial mixing. Polymers 17-24 spindlin 1 Homo sapiens 45-49 18201075-1 2008 Spin-coating one polymer solution on another spin-cast polymer film is believed to result in unfavorable interfacial mixing. Polymers 55-62 spindlin 1 Homo sapiens 0-4 18201075-1 2008 Spin-coating one polymer solution on another spin-cast polymer film is believed to result in unfavorable interfacial mixing. Polymers 55-62 spindlin 1 Homo sapiens 45-49 17764298-0 2007 Deuteron and proton spin-lattice relaxation dispersion of polymer melts: intrasegment, intrachain, and interchain contributions. Polymers 58-65 spindlin 1 Homo sapiens 20-24 17308673-0 2007 Spin crossover behavior in a family of iron(II) zigzag chain coordination polymers. Polymers 74-82 spindlin 1 Homo sapiens 0-4 17392926-0 2007 Antireflective structures via spin casting of polymer latex. Polymers 46-53 spindlin 1 Homo sapiens 30-34 17392926-3 2007 We report what we believe to be the first example of preparing antireflective coatings on glass slides by spin casting polymer latex. Polymers 119-126 spindlin 1 Homo sapiens 106-110 17441143-2 2007 In hydrocarbon solvents, these polymers formed a physical gel and showed a thermoreversible spin transition upon the sol-gel phase transition. Polymers 31-39 spindlin 1 Homo sapiens 92-96 16142241-0 2005 An interfacial instability in a transient wetting layer leads to lateral phase separation in thin spin-cast polymer-blend films. Polymers 108-115 spindlin 1 Homo sapiens 98-102 16142241-1 2005 Spin-coating is a very widely used technique for making uniform thin polymer films. Polymers 69-76 spindlin 1 Homo sapiens 0-4 16142241-3 2005 The efficiency of such devices can be improved by using blends of polymers; these phase separate during the spin-coating process, creating the complex morphology that leads to performance improvements. Polymers 66-74 spindlin 1 Homo sapiens 108-112 18828613-0 2008 Spin-assembled nanolayer of a hyperbranched polymer on the anode in organic light-emitting diodes: the mechanism of hole injection and electron blocking. Polymers 44-51 spindlin 1 Homo sapiens 0-4 16618130-2 2006 Spin-coated hexagonal non-close-packed silica colloidal crystals embedded in a polymer matrix are used as starting templates to create 2D polymeric microwell arrays. Polymers 79-86 spindlin 1 Homo sapiens 0-4 16637327-3 2006 Changes in specific surface tension of spin-labeled molecules of serum albumin, hemoglobin, and antibodies were studied depending on protein concentration, the structure of the reporter group, ligand state of the protein, and the presence of salts, water-soluble polymers, and D2O. Polymers 263-271 spindlin 1 Homo sapiens 39-43 12885198-5 2003 Spin-coated polymer films were characterized through contact angle measurements to give the Lifschitz-van der Waals, electron acceptor and electron donor terms of the surface free energy, gamma(s)LW, gamma(s)+ and gamma(s)- respectively. Polymers 12-19 spindlin 1 Homo sapiens 0-4 12633395-0 2003 Spin-dependent electron-hole capture kinetics in luminescent conjugated polymers. Polymers 72-80 spindlin 1 Homo sapiens 0-4 15700994-2 2005 The products from irradiation of the polymer were characterized by SQUID measurements, which revealed that a persistent triplet carbene unit incorporated into a pi-network of the phenylacetylene polymer indeed acts as a spin source to generate a high-spin ground state, although the estimated spin multiplicities are not as high as that expected from the degree of polymerization. Polymers 37-44 spindlin 1 Homo sapiens 220-224 15700994-2 2005 The products from irradiation of the polymer were characterized by SQUID measurements, which revealed that a persistent triplet carbene unit incorporated into a pi-network of the phenylacetylene polymer indeed acts as a spin source to generate a high-spin ground state, although the estimated spin multiplicities are not as high as that expected from the degree of polymerization. Polymers 37-44 spindlin 1 Homo sapiens 251-255 15700994-2 2005 The products from irradiation of the polymer were characterized by SQUID measurements, which revealed that a persistent triplet carbene unit incorporated into a pi-network of the phenylacetylene polymer indeed acts as a spin source to generate a high-spin ground state, although the estimated spin multiplicities are not as high as that expected from the degree of polymerization. Polymers 37-44 spindlin 1 Homo sapiens 251-255 15700994-2 2005 The products from irradiation of the polymer were characterized by SQUID measurements, which revealed that a persistent triplet carbene unit incorporated into a pi-network of the phenylacetylene polymer indeed acts as a spin source to generate a high-spin ground state, although the estimated spin multiplicities are not as high as that expected from the degree of polymerization. Polymers 195-202 spindlin 1 Homo sapiens 220-224 15700994-2 2005 The products from irradiation of the polymer were characterized by SQUID measurements, which revealed that a persistent triplet carbene unit incorporated into a pi-network of the phenylacetylene polymer indeed acts as a spin source to generate a high-spin ground state, although the estimated spin multiplicities are not as high as that expected from the degree of polymerization. Polymers 195-202 spindlin 1 Homo sapiens 251-255 15700994-2 2005 The products from irradiation of the polymer were characterized by SQUID measurements, which revealed that a persistent triplet carbene unit incorporated into a pi-network of the phenylacetylene polymer indeed acts as a spin source to generate a high-spin ground state, although the estimated spin multiplicities are not as high as that expected from the degree of polymerization. Polymers 195-202 spindlin 1 Homo sapiens 251-255 12809214-0 2003 Cooperative thermal and optical switching of spin states in a new two-dimensional coordination polymer. Polymers 95-102 spindlin 1 Homo sapiens 45-49 16290413-0 2002 Spin probe study on the interaction of chitosan-derived polymer surfactants with lipid membrane. Polymers 56-63 spindlin 1 Homo sapiens 0-4 8688068-0 1996 Structure in Thin and Ultrathin Spin-Cast Polymer Films The molecular organization in ultrathin polymer films (thicknesses less than 1000 angstroms) and thin polymer films (thicknesses between 1000 and 10,000 angstroms) may differ substantially from that of bulk polymers, which can lead to important differences in resulting thermophysical properties. Polymers 42-49 spindlin 1 Homo sapiens 32-36 11677602-7 2001 This suggests that recombination is spin-independent for the monomer, but that a spin-dependent process, favouring singlet formation, is effective in the polymer. Polymers 154-161 spindlin 1 Homo sapiens 81-85 9245357-0 1997 A Double-Modulation ESR Study of Internal Dynamics in the Glassy Polymer Matrix Detected by a Nitroxide Spin Probe The double-modulation ESR spin-probe technique was employed to study slow-motional dynamics in amorphous polymer matrices of polybutadiene, polyisobutylene, poly(methyl methacrylate), and paraffin. Polymers 65-72 spindlin 1 Homo sapiens 104-108 9245357-1 1997 It was shown that the low-lying excitation levels of the polymer matrix, found in the range from 77 to 190 K below the internal spin-probe transition, affect the effective relaxation rate of a perdeuterated nitroxide probe. Polymers 57-64 spindlin 1 Homo sapiens 128-132 1665991-1 1991 The molecular motions of spin-labelled ligands covalently bound by spacer groups to an hydrophobic and an hydrophilic polymer matrix were evaluated by ESR spectroscopy. Polymers 118-125 spindlin 1 Homo sapiens 25-29 8345788-1 1993 Spin-echo sequences with echo times as short as 3.5 msec were implemented on a standard 1.5 T NMR whole-body imager for 1H imaging of polymers in the solid-state. Polymers 134-142 spindlin 1 Homo sapiens 0-4 9960544-0 1993 Spin-lattice relaxation of polymers: The memory-function formalism. Polymers 27-35 spindlin 1 Homo sapiens 0-4 34464139-0 2021 Probing an Isolated Conjugated Polymer Molecule with Radiation-Generated Spin-Correlated Polaron Pairs. Polymers 31-38 spindlin 1 Homo sapiens 73-77 34913703-1 2021 We propose a mechanism for generating pure spin current in heterojunction organic solar cells, with the donor and acceptor both being degenerate ground-state polymers; thus, solitons can be formed. Polymers 158-166 spindlin 1 Homo sapiens 43-47 34748346-0 2021 Solid-State NMR and Impedance Spectroscopy Study of Spin Dynamics in Proton-Conducting Polymers: An Application of Anisotropic Relaxing Model. Polymers 87-95 spindlin 1 Homo sapiens 52-56 34677055-0 2021 Synergic Bistability between Spin Transition and Fluorescence in Polyfluorene Composites with Spin Crossover Polymers. Polymers 109-117 spindlin 1 Homo sapiens 29-33 34677055-0 2021 Synergic Bistability between Spin Transition and Fluorescence in Polyfluorene Composites with Spin Crossover Polymers. Polymers 109-117 spindlin 1 Homo sapiens 94-98 34677055-5 2021 A strong synergy was observed between the spin transition of the Fe(II) compound and variations in the fluorescence of the organic polymer. Polymers 131-138 spindlin 1 Homo sapiens 42-46 34677936-0 2021 Comparison of the Mechanical Properties of a Conjugated Polymer Deposited Using Spin Coating, Interfacial Spreading, Solution Shearing, and Spray Coating. Polymers 56-63 spindlin 1 Homo sapiens 80-84 34292678-2 2021 This phenomenon, termed the chiral-induced spin selectivity (CISS), effect has been observed in chiral molecules, supramolecular structures, polymers, and metal-organic films. Polymers 141-149 spindlin 1 Homo sapiens 43-47 34464139-1 2021 An understanding of the interplay between the spin and electronic degrees of freedom of polarons migrating along conjugated polymer molecules is required to further the development of organic electronics and spintronics. Polymers 124-131 spindlin 1 Homo sapiens 46-50 34464139-2 2021 In this study, a novel experimental approach is proposed for studying spin-correlated polaron pairs (PPs) on an isolated molecule of a conjugated polymer. Polymers 146-153 spindlin 1 Homo sapiens 70-74 10040434-0 1989 Spin dynamics in the conducting polymer, polyaniline. Polymers 32-39 spindlin 1 Homo sapiens 0-4 34279097-0 2021 Spin Crossover in a Series of Non-Hofmann-Type Fe(II) Coordination Polymers Based on (Hg(SeCN)3)- or (Hg(SeCN)4)2- Building Blocks. Polymers 67-75 spindlin 1 Homo sapiens 0-4 34128522-3 2021 Two new coordination polymers with the general formula (FeII(1,2,3-triazole)2MII(CN)4) (M = Pt, Pd) undergo abrupt hysteretic spin crossover in the range of 190-225 K as revealed by magnetic susceptibility measurements. Polymers 21-29 spindlin 1 Homo sapiens 126-130 35612618-0 2022 The memory of thin polymer films generated by spin coating. Polymers 19-26 spindlin 1 Homo sapiens 46-50 35612618-7 2022 For instance, the magnitudes of shrinkage of melt-spun fibers and of filaments from crumpled spin coated polymer films are similar. Polymers 105-112 spindlin 1 Homo sapiens 93-97 35474302-0 2022 High-mobility semiconducting polymers with different spin ground states. Polymers 29-37 spindlin 1 Homo sapiens 53-57 35474302-2 2022 Although high-spin ground states have been observed in some quinoidal type small molecules or doped organic semiconductors, semiconducting polymers with high-spin at their neutral ground state are rarely reported. Polymers 139-147 spindlin 1 Homo sapiens 158-162 35474302-3 2022 Here we report three high-mobility semiconducting polymers with different spin ground states. Polymers 50-58 spindlin 1 Homo sapiens 74-78 35474302-5 2022 We demonstrate that the electronic structure, spin density, and solid-state interchain interactions in the high-spin polymers are crucial for their ground states. Polymers 117-125 spindlin 1 Homo sapiens 46-50 35474302-5 2022 We demonstrate that the electronic structure, spin density, and solid-state interchain interactions in the high-spin polymers are crucial for their ground states. Polymers 117-125 spindlin 1 Homo sapiens 112-116 35474302-6 2022 Polymers with a triplet ground state (S = 1) could exhibit doublet (S = 1/2) behavior due to different spin distributions and solid-state interchain spin-spin interactions. Polymers 0-8 spindlin 1 Homo sapiens 103-107 35474302-6 2022 Polymers with a triplet ground state (S = 1) could exhibit doublet (S = 1/2) behavior due to different spin distributions and solid-state interchain spin-spin interactions. Polymers 0-8 spindlin 1 Homo sapiens 149-153 35474302-6 2022 Polymers with a triplet ground state (S = 1) could exhibit doublet (S = 1/2) behavior due to different spin distributions and solid-state interchain spin-spin interactions. Polymers 0-8 spindlin 1 Homo sapiens 154-158 35474302-8 2022 Our results demonstrate a rational approach to obtain high-mobility semiconducting polymers with different spin ground states. Polymers 83-91 spindlin 1 Homo sapiens 107-111 35394001-0 2022 Spin-orbit coupling and the fine optical structure of chiral helical polymers. Polymers 69-77 spindlin 1 Homo sapiens 0-4 3007091-11 1985 Spin trapping has been used to identify radicals in organic liquids, in polymer degradation and in the decomposition of organometallic compounds. Polymers 72-79 spindlin 1 Homo sapiens 0-4 32875794-0 2020 ON/OFF Photoswitching and Thermoinduced Spin Crossover with Cooperative Luminescence in a 2D Iron(II) Coordination Polymer. Polymers 115-122 spindlin 1 Homo sapiens 40-44 33949416-2 2021 In this article, we show that spin coating, a widely utilized method for obtaining ultra-thin polymer films, has been utilised to modulate the self-assembly of peptide molecules, which has traditionally been achieved by chemical functionalisation of the molecules. Polymers 94-101 spindlin 1 Homo sapiens 30-34 33926182-1 2021 In past studies, spin selective transport was observed in polymers and supramolecular structures that are based on homochiral building blocks possessing stereocenters. Polymers 58-66 spindlin 1 Homo sapiens 17-21 33926182-5 2021 The spin polarization correlates with the intensity of the CD spectra of the polymers, indicating that the effect is nonlocal. Polymers 77-85 spindlin 1 Homo sapiens 4-8 33325977-0 2021 Impact of the process conditions on polymer pattern morphology during spin coating over topological surfaces. Polymers 36-43 spindlin 1 Homo sapiens 70-74 33325977-2 2021 Spin coating is a relatively robust method to develop uniform polymer films over the substrate surface. Polymers 62-69 spindlin 1 Homo sapiens 0-4 33325977-3 2021 However, polymer casting over a topographically prepatterned surface using the spin coating technique is challenging because of the complex transport phenomena involved in the process. Polymers 9-16 spindlin 1 Homo sapiens 79-83 33325977-5 2021 In this work the phase separation dynamics during the spinodal decomposition of a polymer-solvent system in a spin coating process is mathematically investigated. Polymers 82-89 spindlin 1 Homo sapiens 54-58 33404212-0 2021 Open-Shell and Closed-Shell Quinoid-Aromatic Conjugated Polymers: Unusual Spin Magnetic and High Charge Transport Properties. Polymers 56-64 spindlin 1 Homo sapiens 74-78 33404212-7 2021 This work successfully demonstrated how the control of the closed/open-shell character of quinoidal building blocks changes charge transport and spin properties of quinoidal conjugated polymers via quinoid-aromatic interconversion. Polymers 185-193 spindlin 1 Homo sapiens 145-149 32643717-0 2020 Electrical conductivity and magnetic bistability in metal-organic frameworks and coordination polymers: charge transport and spin crossover at the nanoscale. Polymers 94-102 spindlin 1 Homo sapiens 125-129 32657582-1 2020 Two types of experiments conducted to investigate the effect of pressure on the spin crossover (SCO) properties of the 2D Fe(II) coordination polymer formulated {Fe[bipy(ttr)2]}n are reported, namely, (1) magnetic measurements performed at variable temperature and at fixed pressure and (2) visible spectroscopy at variable pressure and fixed temperature. Polymers 142-149 spindlin 1 Homo sapiens 80-84 32496753-1 2020 Integration of the ON-OFF cooperative spin crossover (SCO) properties of FeII coordination polymers as components of electronic and/or spintronic devices is currently an area of great interest for potential applications. Polymers 91-99 spindlin 1 Homo sapiens 38-42 32248213-5 2020 Here, we show that the association of ultra-small 1.2 nm platinum nanoparticles with FeII triazole-based spin crossover coordination polymers leads to self-assemblies, extremely well organized at the sub-3 nm scale. Polymers 133-141 spindlin 1 Homo sapiens 105-109 32248213-8 2020 Coordinating polymers are therefore ideal candidates for the elaboration of robust, well-organized, hybrid self-assemblies with metallic nanoparticles, while maintaining sensitive functional properties, such as spin crossover. Polymers 13-21 spindlin 1 Homo sapiens 211-215 32533565-0 2020 Spin Filtering Along Chiral Polymers. Polymers 28-36 spindlin 1 Homo sapiens 0-4 32533565-1 2020 Spin dependent conduction and polarization in chiral polymers were studied, when the polymers are organized as self-assembled monolayers and the conduction is along the polymer backbone, namely along its longer axis. Polymers 53-61 spindlin 1 Homo sapiens 0-4 32533565-1 2020 Spin dependent conduction and polarization in chiral polymers were studied, when the polymers are organized as self-assembled monolayers and the conduction is along the polymer backbone, namely along its longer axis. Polymers 85-93 spindlin 1 Homo sapiens 0-4 32533565-1 2020 Spin dependent conduction and polarization in chiral polymers were studied, when the polymers are organized as self-assembled monolayers and the conduction is along the polymer backbone, namely along its longer axis. Polymers 53-60 spindlin 1 Homo sapiens 0-4 32533565-2 2020 Large spin polarization and magnetoresistance effects were observed, which showed a clear dependence on the secondary structure of the polymer. Polymers 135-142 spindlin 1 Homo sapiens 6-10 32338886-0 2020 Effect of Mechanochemical Recrystallization on the Thermal Hysteresis of 1D FeII-triazole Spin Crossover Polymers. Polymers 105-113 spindlin 1 Homo sapiens 90-94 32301607-3 2020 In this paper, we report the synthesis and crystal structures of the metal-organic coordination polymers {FeII(Mepz)[AuI(CN)2]2} ([Au]) and {FeII(Mepz)2[AgI(CN)2]2} ([Ag]), where Mepz = 2-methylpyrazine, along with characterization of their spin-state behavior by variable-temperature SQUID magnetometry and Mossbauer spectroscopy. Polymers 96-104 spindlin 1 Homo sapiens 241-245 32109121-0 2020 Separation of Spin and Charge Transport in Pristine pi-Conjugated Polymers. Polymers 66-74 spindlin 1 Homo sapiens 14-18 32109121-1 2020 We have experimentally tested whether spin-transport and charge-transport in pristine pi-conjugated polymer films at room temperature occur via the same electronic processes. Polymers 100-107 spindlin 1 Homo sapiens 38-42 32109121-2 2020 We have obtained the spin diffusion coefficient of several pi-conjugated polymer films from the spin diffusion length measured by the technique of inverse spin Hall effect and the spin relaxation time measured by pulsed electrically detected magnetic resonance spectroscopy. Polymers 73-80 spindlin 1 Homo sapiens 21-25 32109121-2 2020 We have obtained the spin diffusion coefficient of several pi-conjugated polymer films from the spin diffusion length measured by the technique of inverse spin Hall effect and the spin relaxation time measured by pulsed electrically detected magnetic resonance spectroscopy. Polymers 73-80 spindlin 1 Homo sapiens 96-100 32109121-2 2020 We have obtained the spin diffusion coefficient of several pi-conjugated polymer films from the spin diffusion length measured by the technique of inverse spin Hall effect and the spin relaxation time measured by pulsed electrically detected magnetic resonance spectroscopy. Polymers 73-80 spindlin 1 Homo sapiens 96-100 32109121-2 2020 We have obtained the spin diffusion coefficient of several pi-conjugated polymer films from the spin diffusion length measured by the technique of inverse spin Hall effect and the spin relaxation time measured by pulsed electrically detected magnetic resonance spectroscopy. Polymers 73-80 spindlin 1 Homo sapiens 96-100