PMID-sentid Pub_year Sent_text comp_official_name comp_offsetprotein_name organism prot_offset 12588119-7 2003 Spin densities at carbon in the C(6)H(5) and C(3)F(7) groups were estimated from the (1)H and (19)F contact shifts. Carbon 18-24 spindlin 1 Homo sapiens 0-4 16774310-0 2006 Spin-dependent transport through a magnetic carbon nanotube-molecule junction. Carbon 44-50 spindlin 1 Homo sapiens 0-4 15181635-0 2004 Acceleration of carbon-13 spin-lattice relaxation times in amino acids by electrolytes. Carbon 16-22 spindlin 1 Homo sapiens 26-30 15181635-1 2004 Measurements of the enhancement, by various electrolytes, of the spin-lattice relaxation time of carbon-13 at different locations in a number of amino acids are reported. Carbon 97-103 spindlin 1 Homo sapiens 65-69 15181635-2 2004 Spin-lattice relaxation times T1 of all the carbons in amino acids generally tend to decrease with increase in the concentration of electrolytes, the largest effects often being observed for the charged carboxylate groups of the amino acids. Carbon 44-51 spindlin 1 Homo sapiens 0-4 15181635-3 2004 Carboxylic carbons in amino acids are the sensitive "acceptor" of the 13C spin-lattice relaxation accelerating effects offered by electrolytes, and the 13C spin-lattice relaxation accelerating ability of electrolytes decreases in the order Mg(ClO4)2 > MgCl2 > CaCl2 > NaCl > KCl > LiClO4 > NaOH. Carbon 11-18 spindlin 1 Homo sapiens 74-78 15181635-3 2004 Carboxylic carbons in amino acids are the sensitive "acceptor" of the 13C spin-lattice relaxation accelerating effects offered by electrolytes, and the 13C spin-lattice relaxation accelerating ability of electrolytes decreases in the order Mg(ClO4)2 > MgCl2 > CaCl2 > NaCl > KCl > LiClO4 > NaOH. Carbon 11-18 spindlin 1 Homo sapiens 156-160 17251975-0 2007 Transformation of spin information into large electrical signals using carbon nanotubes. Carbon 71-77 spindlin 1 Homo sapiens 18-22 17251975-6 2007 This spintronic system combines a number of favourable properties that enable this performance; the long spin lifetime in nanotubes due to the small spin-orbit coupling of carbon; the high Fermi velocity in nanotubes that limits the carrier dwell time; the high spin polarization in the manganite electrodes, which remains high right up to the manganite-nanotube interface; and the resistance of the interfacial barrier for spin injection. Carbon 172-178 spindlin 1 Homo sapiens 5-9 16439134-4 2006 Spin adducts from other oxygen- and carbon-centered radicals (e.g., derived from methanol or linoleic acid hydroperoxide) are also described. Carbon 36-42 spindlin 1 Homo sapiens 0-4 16392473-0 2005 Spin-unrestricted linear-scaling electronic structure theory and its application to magnetic carbon-doped boron nitride nanotubes. Carbon 93-99 spindlin 1 Homo sapiens 0-4 12713312-3 2003 Spin delocalization on the nitro group is proposed to explain the stability of the carbon-centered radical generated. Carbon 83-89 spindlin 1 Homo sapiens 0-4 11133279-1 2001 A general and very simple strategy for achieving clean spin-state-selective excitation with full sensitivity in carbon-selective gradient-enhanced 1D HMQC and HSQC pulse schemes is presented. Carbon 112-118 spindlin 1 Homo sapiens 55-59 12076159-4 2002 The lowest D values have been found for the hydrazonyl-substituted derivatives, which implies the lowest spin density at the carbon center and, thus, the most efficacious radical stabilization through spin delocalization. Carbon 125-131 spindlin 1 Homo sapiens 105-109 12076159-4 2002 The lowest D values have been found for the hydrazonyl-substituted derivatives, which implies the lowest spin density at the carbon center and, thus, the most efficacious radical stabilization through spin delocalization. Carbon 125-131 spindlin 1 Homo sapiens 201-205 12005586-0 2002 Spin-orbit coupling and electron spin resonance theory for carbon nanotubes. Carbon 59-65 spindlin 1 Homo sapiens 33-37 11929297-5 2002 The formation of hydroxyl and carbon-centered radicals was indicated by electron paramagnetic resonance spectra using alpha-(4-pyridyl-1-oxide)-N-tert-butylnitrone or 5-(diethoxyphosphoryl)-5-methyl-1-pyrroline-N-oxide as spin traps. Carbon 30-36 spindlin 1 Homo sapiens 222-226 11133279-5 2001 Such an approach affords a suite of powerful selective 1D (13)C-edited NMR experiments which are helpful for resonance assignment purposes in overcrowded proton spin systems and also for the accurate determination of the magnitude and sign of long-range proton-carbon coupling constants in CH spin sytems for samples at natural abundance. Carbon 261-267 spindlin 1 Homo sapiens 161-165 11133279-5 2001 Such an approach affords a suite of powerful selective 1D (13)C-edited NMR experiments which are helpful for resonance assignment purposes in overcrowded proton spin systems and also for the accurate determination of the magnitude and sign of long-range proton-carbon coupling constants in CH spin sytems for samples at natural abundance. Carbon 261-267 spindlin 1 Homo sapiens 293-297 11674159-0 1999 Stereochemical Determination of Acyclic Structures Based on Carbon-Proton Spin-Coupling Constants. Carbon 60-66 spindlin 1 Homo sapiens 74-78 11030922-0 2000 Spin transport in interacting quantum wires and carbon nanotubes We present a general formulation of spin-dependent transport through a clean one-dimensional interacting quantum wire or carbon nanotube, connected to noncollinear ferromagnets via tunnel junctions. Carbon 48-54 spindlin 1 Homo sapiens 101-105 11030922-0 2000 Spin transport in interacting quantum wires and carbon nanotubes We present a general formulation of spin-dependent transport through a clean one-dimensional interacting quantum wire or carbon nanotube, connected to noncollinear ferromagnets via tunnel junctions. Carbon 186-192 spindlin 1 Homo sapiens 0-4 11030922-0 2000 Spin transport in interacting quantum wires and carbon nanotubes We present a general formulation of spin-dependent transport through a clean one-dimensional interacting quantum wire or carbon nanotube, connected to noncollinear ferromagnets via tunnel junctions. Carbon 186-192 spindlin 1 Homo sapiens 101-105 11017299-0 2000 Carbon nanotube based magnetic tunnel junctions Spin-coherent quantum transport in carbon nanotube magnetic tunnel junctions is investigated theoretically. Carbon 0-6 spindlin 1 Homo sapiens 48-52 11084289-9 2000 Addition of Fe(2+) under anaerobic conditions to an aqueous suspension of linoleic acid hydroperoxide and the spin trap resulted in the detection of three different species: a carbon-centered radical adduct, an acyl radical adduct, and the hydroxyl adduct. Carbon 176-182 spindlin 1 Homo sapiens 110-114 10991284-0 2000 Spin configurations of a carbon nanotube in a nonuniform external potential We study, theoretically, the ground state spin of a carbon nanotube in the presence of an external potential. Carbon 25-31 spindlin 1 Homo sapiens 0-4 10991284-0 2000 Spin configurations of a carbon nanotube in a nonuniform external potential We study, theoretically, the ground state spin of a carbon nanotube in the presence of an external potential. Carbon 25-31 spindlin 1 Homo sapiens 118-122 10991284-0 2000 Spin configurations of a carbon nanotube in a nonuniform external potential We study, theoretically, the ground state spin of a carbon nanotube in the presence of an external potential. Carbon 128-134 spindlin 1 Homo sapiens 0-4 10991284-0 2000 Spin configurations of a carbon nanotube in a nonuniform external potential We study, theoretically, the ground state spin of a carbon nanotube in the presence of an external potential. Carbon 128-134 spindlin 1 Homo sapiens 118-122 11017299-0 2000 Carbon nanotube based magnetic tunnel junctions Spin-coherent quantum transport in carbon nanotube magnetic tunnel junctions is investigated theoretically. Carbon 83-89 spindlin 1 Homo sapiens 48-52 29711260-0 1998 Crystal Structures of Chiral Diastereoisomers of a Carbon-Based High-Spin Molecule. Carbon 51-57 spindlin 1 Homo sapiens 69-73 9200687-2 1997 Spin-labeled biotin-PEs were prepared with the nitroxide group at position C-5, C-8, C-10, C-12, or C-14 of the sn-2 chain and were incorporated at 1 mol % in lipid bilayer membranes of dimyristoylphosphatidylcholine. Carbon 75-76 spindlin 1 Homo sapiens 0-4 20700828-3 1998 This approach removes the main relaxation source (the dipolar coupling to the directly bound 13C spin) and leads to a significant reduction of the proton and carbon relaxation rates. Carbon 158-164 spindlin 1 Homo sapiens 97-101 9200687-2 1997 Spin-labeled biotin-PEs were prepared with the nitroxide group at position C-5, C-8, C-10, C-12, or C-14 of the sn-2 chain and were incorporated at 1 mol % in lipid bilayer membranes of dimyristoylphosphatidylcholine. Carbon 80-81 spindlin 1 Homo sapiens 0-4 8911636-2 1996 Samples containing nickel (III), of low crystallinity, with small particle size and high surface areas can in the presence of H2O2, cause the generation of the hydroxyl radical (as detected by spin trapping with 5,5-dimethyl-1-pyrroline N-oxide or DMPO) and/or another highly reactive species capable of cleaving the C-S bond in dimethyl sulphoxide. Carbon 317-318 spindlin 1 Homo sapiens 193-197 8012523-3 1994 Compared to the spin trap 5,5-dimethyl-pyrroline-1-oxide, a higher lifetime of hydroxyl radical adducts and a higher selectivity related to the trapping of carbon-centered radicals was found. Carbon 156-162 spindlin 1 Homo sapiens 16-20 32794861-0 2020 Topologically Protected Correlated End Spin Formation in Carbon Nanotubes. Carbon 57-63 spindlin 1 Homo sapiens 39-43 8347671-6 1993 (3) In fluid-phase PC membranes possessing short alkyl chains (12-14 carbons), the activation energy of the rotational diffusion of 16-doxylstearic acid spin label (16-SASL) is significantly lower at a carotenoid concentration of 10 mol%. Carbon 69-76 spindlin 1 Homo sapiens 153-157 33780054-0 2021 Low-Spin and High-Spin Perferryl Intermediates in Non-Heme Iron Catalyzed Oxidations of Aliphatic C-H Groups. Carbon 64-65 spindlin 1 Homo sapiens 4-8 33780054-0 2021 Low-Spin and High-Spin Perferryl Intermediates in Non-Heme Iron Catalyzed Oxidations of Aliphatic C-H Groups. Carbon 64-65 spindlin 1 Homo sapiens 18-22 34937899-1 2021 Spin-ordered electronic states in hydrogen-terminated zigzag nanographene give rise to magnetic quantum phenomena1,2 that have sparked renewed interest in carbon-based spintronics3,4. Carbon 155-161 spindlin 1 Homo sapiens 0-4 34870421-0 2021 Molecular Functionalization and Emergence of Long-Range Spin-Dependent Phenomena in Two-Dimensional Carbon Nanotube Networks. Carbon 100-106 spindlin 1 Homo sapiens 56-60 34911952-4 2021 In its anionic state, the carbon impurity is computed to have a magnetic moment of 1 muB resulting from an unpaired electron populating a spin-polarized in-gap orbital. Carbon 26-32 spindlin 1 Homo sapiens 138-142 34197074-0 2021 A Spin-Coated Hydrogel Platform Enables Accurate Investigation of Immobilized Individual Single-Walled Carbon Nanotubes. Carbon 103-109 spindlin 1 Homo sapiens 2-6 34516595-7 2021 The electrical control on spin polarization is realized in pure-carbon systems, showing great application potential. Carbon 64-70 spindlin 1 Homo sapiens 26-30 34739026-3 2021 We focus on the recently reported encapsulation of Fe(II) spin-crossover complexes in single-walled carbon nanotubes, with new measurements that support the theoretical findings. Carbon 100-106 spindlin 1 Homo sapiens 58-62 34650056-5 2021 In contrast to carbon nanotubes, where nanotube chirality determines spin-orbit coupling breaking the SU(4) symmetry of the electronic states relevant for the Kondo effect, we study a planar carbon material where a small spin-orbit coupling of nominally flat graphene is enhanced by zero-point out-of-plane phonons. Carbon 191-197 spindlin 1 Homo sapiens 221-225 34213354-0 2021 Perchlorinated Triarylmethyl Radical 99% Enriched 13C at the Central Carbon as EPR Spin Probe Highly Sensitive to Molecular Tumbling. Carbon 69-75 spindlin 1 Homo sapiens 83-87 34207418-0 2021 Direct Pattern Growth of Carbon Nanomaterials by Laser Scribing on Spin-Coated Cu-PI Composite Films and Their Gas Sensor Application. Carbon 25-31 spindlin 1 Homo sapiens 67-71 33715691-0 2021 The Effects of Fe Film Thickness and the H2 Annealing Time on the Spin-Capability of Carbon Nanotube Forest with Chemical Vapor Deposition Method. Carbon 85-91 spindlin 1 Homo sapiens 66-70 33715691-1 2021 The effects of as-deposited iron (Fe) film thickness and the hydrogen (H2) annealing time on the spin-capability of carbon nanotube (CNT) forest have been studied. Carbon 116-122 spindlin 1 Homo sapiens 97-101 33715691-2 2021 Both, the as-deposited Fe film thickness and the H2 annealing time significantly changed the morphology of Fe nanoparticles (NPs) after annealing process during the synthesis step of spin-capable carbon nanotube (SCNT) forest. Carbon 196-202 spindlin 1 Homo sapiens 183-187 35335782-0 2022 Surface Transformation of Spin-on-Carbon Film via Forming Carbon Iron Complex for Remarkably Enhanced Polishing Rate. Carbon 34-40 spindlin 1 Homo sapiens 26-30 34168836-1 2021 We report on the discovery and detailed exploration of the unconventional photo-switching mechanism in metallofullerenes, in which the energy of the photon absorbed by the carbon cage pi-system is transformed to mechanical motion of the endohedral cluster accompanied by accumulation of spin density on the metal atoms. Carbon 172-178 spindlin 1 Homo sapiens 287-291 35522997-2 2022 We report the synthesis and operation mode of two all-organic molecular spin-state switches that can be photochemically switched from a diamagnetic (electron paramagnetic resonance (EPR)-silent) to a paramagnetic (EPR-active) form at cryogenic temperatures due to a reversible electrocyclic reaction of its carbon skeleton. Carbon 307-313 spindlin 1 Homo sapiens 72-76 35475353-2 2022 Although heteroatom doping has been developed into an effective method to modify carbon nanomaterials for various heterogeneous adsorption and catalytic oxidation systems, the active source regulated by intrinsic electron and spin structures is still obscure. Carbon 81-87 spindlin 1 Homo sapiens 226-230 35475353-9 2022 This work established a relation between electron and spin structures for adsorption and photocatalysis, paving a new way to design modified carbon nanomaterials to control OMPs. Carbon 141-147 spindlin 1 Homo sapiens 54-58 35380441-0 2022 Spin-Forbidden Carbon-Carbon Bond Formation in Vibrationally Excited alpha-CO. Carbon 15-21 spindlin 1 Homo sapiens 0-4 35380441-0 2022 Spin-Forbidden Carbon-Carbon Bond Formation in Vibrationally Excited alpha-CO. Carbon 22-28 spindlin 1 Homo sapiens 0-4 35335782-1 2022 To scale down semiconductor devices to a size less than the design rule of 10 nm, lithography using a carbon polymer hard-mask was applied, e.g., spin-on-carbon (SOC) film. Carbon 154-160 spindlin 1 Homo sapiens 146-150 35103399-1 2022 The spin polarization of carbon nanomaterials is crucial to design spintronic devices. Carbon 25-31 spindlin 1 Homo sapiens 4-8 2519722-4 1989 Spin-lattice relaxation times of the various carbon atoms indicated that the overall molecular reorientation time (tau R) of the molecule is 0.02 ns at 30 degrees C. An Arrhenius plot of the data showed that the activation energy (Ea) for molecular tumbling is 13.4 kJ/mol. Carbon 45-51 spindlin 1 Homo sapiens 0-4 444472-3 1979 At high substrate/enzyme ratios, the spin-spin relaxation rates of C(1)-C(3) are faster than for the other carbons and are in the order C(1) greater than C(2) greater than C(3). Carbon 67-68 spindlin 1 Homo sapiens 37-41 2555279-8 1989 Analysis of the EPR spectra revealed hyperfine splitting constants that indicated the presence of carbon-centered radical spin adducts in both organ tissues from animals exposed to endotoxin for twenty-five minutes. Carbon 98-104 spindlin 1 Homo sapiens 122-126 444472-3 1979 At high substrate/enzyme ratios, the spin-spin relaxation rates of C(1)-C(3) are faster than for the other carbons and are in the order C(1) greater than C(2) greater than C(3). Carbon 67-68 spindlin 1 Homo sapiens 42-46 444472-3 1979 At high substrate/enzyme ratios, the spin-spin relaxation rates of C(1)-C(3) are faster than for the other carbons and are in the order C(1) greater than C(2) greater than C(3). Carbon 107-114 spindlin 1 Homo sapiens 37-41 444472-3 1979 At high substrate/enzyme ratios, the spin-spin relaxation rates of C(1)-C(3) are faster than for the other carbons and are in the order C(1) greater than C(2) greater than C(3). Carbon 107-114 spindlin 1 Homo sapiens 42-46 444472-3 1979 At high substrate/enzyme ratios, the spin-spin relaxation rates of C(1)-C(3) are faster than for the other carbons and are in the order C(1) greater than C(2) greater than C(3). Carbon 72-73 spindlin 1 Homo sapiens 37-41 444472-3 1979 At high substrate/enzyme ratios, the spin-spin relaxation rates of C(1)-C(3) are faster than for the other carbons and are in the order C(1) greater than C(2) greater than C(3). Carbon 72-73 spindlin 1 Homo sapiens 42-46 444472-3 1979 At high substrate/enzyme ratios, the spin-spin relaxation rates of C(1)-C(3) are faster than for the other carbons and are in the order C(1) greater than C(2) greater than C(3). Carbon 72-73 spindlin 1 Homo sapiens 37-41 444472-3 1979 At high substrate/enzyme ratios, the spin-spin relaxation rates of C(1)-C(3) are faster than for the other carbons and are in the order C(1) greater than C(2) greater than C(3). Carbon 72-73 spindlin 1 Homo sapiens 42-46 444472-6 1979 Spin-spin and spin-lattice relaxation rates were measured for odd-carbon 13C-enriched 1-dodecanal in the presence of luciferase. Carbon 66-72 spindlin 1 Homo sapiens 0-4 5263759-2 1970 The study has yielded the magnitude and sign of spin densities at the carbon atoms in the pi system of the 9-cis, 13-cis, and all trans isomers. Carbon 70-76 spindlin 1 Homo sapiens 48-52 4525318-1 1974 Carbon-13 spin-lattice relaxation time measurements of amino acids. Carbon 0-6 spindlin 1 Homo sapiens 10-14 4525318-4 1974 For the carboxyl carbon, spin rotation is proposed as the predominant relaxation mechanism, whereas the other carbons are relaxed mainly by the dipole-dipole mechanism, and their relaxation times are relatively independent of changes in concentration and pD. Carbon 17-23 spindlin 1 Homo sapiens 25-29 4515601-2 1973 Spin-lattice relaxation (T(1)) of the [(13)C]carbons of the sugar was measured in the absence and presence of the two transition metal derivatives of the protein. Carbon 45-52 spindlin 1 Homo sapiens 0-4 33652428-4 2021 Theoretical results not only uncover the narrowest nanoribbon structures to realize the SSE and other inspiring thermal spin transport features, but also push carbon-based material candidates towards thermoelectric conversion device applications. Carbon 159-165 spindlin 1 Homo sapiens 120-124 33707459-0 2021 Spin-state-dependent electrical conductivity in single-walled carbon nanotubes encapsulating spin-crossover molecules. Carbon 62-68 spindlin 1 Homo sapiens 0-4 33707459-0 2021 Spin-state-dependent electrical conductivity in single-walled carbon nanotubes encapsulating spin-crossover molecules. Carbon 62-68 spindlin 1 Homo sapiens 93-97 33946296-0 2021 H2S-Sensing Studies Using Interdigitated Electrode with Spin-Coated Carbon Aerogel-Polyaniline Composites. Carbon 68-74 spindlin 1 Homo sapiens 56-60 33784082-0 2021 Enhancing Chemo- and Stereoselectivity in C-H Bond Oxygenation with H2O2 by Nonheme High-Spin Iron Catalysts: The Role of Lewis Acid and Multimetal Centers. Carbon 10-11 spindlin 1 Homo sapiens 89-93 33755594-4 2021 The theoretical results not only uncover the narrowest nanoribbon structures to realize the SSE and other inspiring thermal spin transport features, but also push carbon-based material candidates towards thermoelectric conversion device applications. Carbon 163-169 spindlin 1 Homo sapiens 124-128 33543976-0 2021 Long-Distance Ultrafast Spin Transfer over a Zigzag Carbon Chain Structure. Carbon 52-58 spindlin 1 Homo sapiens 24-28 33543976-2 2021 The spin-density transfer takes place between two Ni atoms and over a 40-atom-long zigzag carbon chain. Carbon 90-96 spindlin 1 Homo sapiens 4-8 32819099-2 2020 The paramagnetic 13C Knight shift of alkyl chain carbons, which is proportional to the local electron spin density, exhibits an electron spin delocalization that exponentially decays along the alkyl chain. Carbon 49-56 spindlin 1 Homo sapiens 102-106 33167619-3 2020 We find that although the CISS effect is entirely attributed in the literature to molecular spin filtering, spin-orbit coupling being partially inherited from the metal electrodes plays an important role in our calculations on ideal carbon helices, even though this effect cannot explain the experimental conductance results. Carbon 233-239 spindlin 1 Homo sapiens 108-112 33225168-8 2020 The spin-lattice relaxation time of carbon nuclei varies from 1 to 107 s. The range of molecular correlation time also varies from 10-4 to 10-8 s. These remarkable diversities of motional dynamics of the molecules imply that there exist various motional degrees of freedom within this valuable drug and these motional degrees of freedom are independent of each other, which may be the reason for the biological activities exhibited by the drug. Carbon 36-42 spindlin 1 Homo sapiens 4-8 32819099-2 2020 The paramagnetic 13C Knight shift of alkyl chain carbons, which is proportional to the local electron spin density, exhibits an electron spin delocalization that exponentially decays along the alkyl chain. Carbon 49-56 spindlin 1 Homo sapiens 137-141 32603158-5 2020 However, 1D systems with linear dispersion at the Fermi energy, such as metallic carbon nanotubes, are an exception since spin pumping is chiral even without interactions. Carbon 81-87 spindlin 1 Homo sapiens 122-126 32761263-1 2020 In this paper, we investigate the effects of spin-dependent electron and defect in the carbon-based molecular device. Carbon 87-93 spindlin 1 Homo sapiens 45-49 32761263-4 2020 The spin effect and switching symbiosis are shown in this carbon-based device. Carbon 58-64 spindlin 1 Homo sapiens 4-8 32789172-0 2020 Giant spin signals in chemically functionalized multiwall carbon nanotubes. Carbon 58-64 spindlin 1 Homo sapiens 6-10 32789172-5 2020 Second, the spin information is brought toward the conducting inner shells of a multiwall carbon nanotube used as a confined nanoguide benefiting from both weak spin-orbit and hyperfine interactions. Carbon 90-96 spindlin 1 Homo sapiens 12-16 32789172-5 2020 Second, the spin information is brought toward the conducting inner shells of a multiwall carbon nanotube used as a confined nanoguide benefiting from both weak spin-orbit and hyperfine interactions. Carbon 90-96 spindlin 1 Homo sapiens 161-165 31978918-0 2020 Spin current generation and control in carbon nanotubes by combining rotation and magnetic field. Carbon 39-45 spindlin 1 Homo sapiens 0-4 30986772-0 2019 The gapless energy spectrum and spin-Peierls instability of 1D Heisenberg spin systems in polymeric complexes of transition metals and hypothetical carbon allotropes. Carbon 148-154 spindlin 1 Homo sapiens 74-78 31894693-5 2020 The polymer blend exhibits a remarkably enhanced spin relaxation length (56 nm) and carrier mobility compared to pristine PBDTTT-C-T. From film microstructural characterizations, we propose that the enhanced spin/carrier transport properties are attributed to the formation of interlinked nanonetwork comprising of the PBDTTT-C-T chain bundles in the inert matrix to afford efficient intrachain charge conduction pathway. Carbon 122-130 spindlin 1 Homo sapiens 49-53 31894693-5 2020 The polymer blend exhibits a remarkably enhanced spin relaxation length (56 nm) and carrier mobility compared to pristine PBDTTT-C-T. From film microstructural characterizations, we propose that the enhanced spin/carrier transport properties are attributed to the formation of interlinked nanonetwork comprising of the PBDTTT-C-T chain bundles in the inert matrix to afford efficient intrachain charge conduction pathway. Carbon 122-130 spindlin 1 Homo sapiens 208-212 31268193-4 2019 This finding is quite unexpected because the initial spin density at the terminal carbon atom of FeC4 + , which serves as the hydrogen acceptor site, is low. Carbon 82-88 spindlin 1 Homo sapiens 53-57 31268193-6 2019 Thus, a highly localized spin density is generated in situ at the terminal carbon atom. Carbon 75-81 spindlin 1 Homo sapiens 25-29 31449383-0 2019 Detection of Spin Reversal via Kondo Correlation in Hybrid Carbon Nanotube Quantum Dots. Carbon 59-65 spindlin 1 Homo sapiens 13-17 31246329-0 2019 Highly Selective and Catalytic Oxygenations of C-H and C=C Bonds by a Mononuclear Nonheme High-Spin Iron(III)-Alkylperoxo Species. Carbon 21-22 spindlin 1 Homo sapiens 95-99 31246329-0 2019 Highly Selective and Catalytic Oxygenations of C-H and C=C Bonds by a Mononuclear Nonheme High-Spin Iron(III)-Alkylperoxo Species. Carbon 47-48 spindlin 1 Homo sapiens 95-99 31246329-0 2019 Highly Selective and Catalytic Oxygenations of C-H and C=C Bonds by a Mononuclear Nonheme High-Spin Iron(III)-Alkylperoxo Species. Carbon 47-48 spindlin 1 Homo sapiens 95-99 31352783-7 2019 Moreover, in polar solvents, the spin is shifted onto the donor substituent and away from the benzylic carbon. Carbon 103-109 spindlin 1 Homo sapiens 33-37 32917632-4 2020 Unexpectedly, we find good thermal contact throughout the nuclear spin bath, virtually independent of the hyperfine coupling strength, which we attribute to effective carbon-carbon interactions mediated by the electronic spin ensemble. Carbon 167-173 spindlin 1 Homo sapiens 66-70 32917632-4 2020 Unexpectedly, we find good thermal contact throughout the nuclear spin bath, virtually independent of the hyperfine coupling strength, which we attribute to effective carbon-carbon interactions mediated by the electronic spin ensemble. Carbon 167-173 spindlin 1 Homo sapiens 221-225 32917632-4 2020 Unexpectedly, we find good thermal contact throughout the nuclear spin bath, virtually independent of the hyperfine coupling strength, which we attribute to effective carbon-carbon interactions mediated by the electronic spin ensemble. Carbon 174-180 spindlin 1 Homo sapiens 66-70 32917632-4 2020 Unexpectedly, we find good thermal contact throughout the nuclear spin bath, virtually independent of the hyperfine coupling strength, which we attribute to effective carbon-carbon interactions mediated by the electronic spin ensemble. Carbon 174-180 spindlin 1 Homo sapiens 221-225 31427741-3 2019 Here, we show that coupling to a magnetic texture can induce both a strong spin-orbit coupling of 1.1 meV and a Zeeman effect in a carbon nanotube. Carbon 131-137 spindlin 1 Homo sapiens 75-79 30468954-2 2019 Spin-lattice relaxation rate (1/T1) of side chain carbon nuclei were remarkably high, because those nuclei possess higher degree of motional freedom. Carbon 50-56 spindlin 1 Homo sapiens 0-4 30984737-0 2019 Quantum Behavior of Spin-Orbit Inelastic Scattering of C-Atoms by D2 at Low Energy. Carbon 55-56 spindlin 1 Homo sapiens 20-24 30984737-2 2019 In particular, neutral carbon atoms are known to play a role in interstellar media, either as probes of physical conditions (ground state 3P j spin-orbit populations), or as cooling agent (collisional excitation followed by radiative decay). Carbon 23-29 spindlin 1 Homo sapiens 143-147 30984737-3 2019 This work aims at investigating the spin-orbit excitation of atomic carbon in its ground electronic state due to collisions with molecular deuterium, an isotopic variant of H2, the most abundant molecule in the interstellar medium. Carbon 68-74 spindlin 1 Homo sapiens 36-40 30984737-13 2019 The present data are compared with those obtained for the C-He and C-H2 collisional systems to get new insights into the dynamics of collision induced spin-orbit excitation/relaxation of atomic carbon. Carbon 194-200 spindlin 1 Homo sapiens 151-155 30855956-0 2019 Spin-Coupled Generalized Valence Bond Description of Group 14 Species: The Carbon, Silicon and Germanium Hydrides, XH n ( n = 1-4). Carbon 75-81 spindlin 1 Homo sapiens 0-4 29847722-1 2018 This paper describes a simple approach to the large-scale synthesis of colloidal Si nanocrystals and their processing into spin-on carbon-free nanocrystalline Si films. Carbon 131-137 spindlin 1 Homo sapiens 123-127 30260623-0 2018 Electrically Controllable Single-Point Covalent Functionalization of Spin-Cast Carbon-Nanotube Field-Effect Transistor Arrays. Carbon 79-85 spindlin 1 Homo sapiens 69-73 30102044-2 2018 Electron paramagnetic resonance spectra of the spin adduct and the adduct formed in the analogous reaction with selectively deuterated substrate identify the radical intermediate in this SmI2 reduction as a carbon-centered radical. Carbon 207-213 spindlin 1 Homo sapiens 47-51 28525951-6 2017 The distribution of spin up and spin down states at the bridge carbon atom plays a dominant role in the perfect spin filtering. Carbon 63-69 spindlin 1 Homo sapiens 20-24 30079190-0 2018 Modulating the oxygen reduction activity of heteroatom-doped carbon catalysts via the triple effect: charge, spin density and ligand effect. Carbon 61-67 spindlin 1 Homo sapiens 109-113 30079190-3 2018 The results of the DFT calculations indicate that the intrinsic catalytic activity and the ORR mechanism depend on the triple effect, that is, the charge, the spin density and the coordinate state (ligand effect) of the carbon sites. Carbon 220-226 spindlin 1 Homo sapiens 159-163 28525951-6 2017 The distribution of spin up and spin down states at the bridge carbon atom plays a dominant role in the perfect spin filtering. Carbon 63-69 spindlin 1 Homo sapiens 32-36 28525951-6 2017 The distribution of spin up and spin down states at the bridge carbon atom plays a dominant role in the perfect spin filtering. Carbon 63-69 spindlin 1 Homo sapiens 32-36 29039674-0 2017 Spin-Charge Separation in Finite Length Metallic Carbon Nanotubes. Carbon 49-55 spindlin 1 Homo sapiens 0-4 29039674-8 2017 Time evolution analysis of the charge and spin line densities evidences that the charge and spin density waves are elementary excitations of metallic carbon nanotubes. Carbon 150-156 spindlin 1 Homo sapiens 92-96 29039674-8 2017 Time evolution analysis of the charge and spin line densities evidences that the charge and spin density waves are elementary excitations of metallic carbon nanotubes. Carbon 150-156 spindlin 1 Homo sapiens 42-46 28393942-0 2017 Spin filtering with poly-T wrapped single wall carbon nanotubes. Carbon 47-53 spindlin 1 Homo sapiens 0-4 28972750-0 2017 Low-Valent, High-Spin Chromium-Catalyzed Cleavage of Aromatic Carbon-Nitrogen Bonds at Room Temperature: A Combined Experimental and Theoretical Study. Carbon 62-68 spindlin 1 Homo sapiens 17-21 28594639-0 2017 Spin-valley dynamics of electrically driven ambipolar carbon-nanotube quantum dots. Carbon 54-60 spindlin 1 Homo sapiens 0-4 28498696-0 2017 Hyperfine and Spin-Orbit Coupling Effects on Decay of Spin-Valley States in a Carbon Nanotube. Carbon 78-84 spindlin 1 Homo sapiens 14-18 28498696-0 2017 Hyperfine and Spin-Orbit Coupling Effects on Decay of Spin-Valley States in a Carbon Nanotube. Carbon 78-84 spindlin 1 Homo sapiens 54-58 28498696-1 2017 The decay of spin-valley states is studied in a suspended carbon nanotube double quantum dot via the leakage current in Pauli blockade and via dephasing and decoherence of a qubit. Carbon 58-64 spindlin 1 Homo sapiens 13-17 28294252-1 2017 Spin-orbit interaction in carbon nanotubes has been under debate for several years and a variety of theoretical calculations and experimental results have been published. Carbon 26-32 spindlin 1 Homo sapiens 0-4 28294252-0 2017 Spin-orbit coupling in nearly metallic chiral carbon nanotubes: a density-functional based study. Carbon 46-52 spindlin 1 Homo sapiens 0-4 27152812-1 2016 The small spin-orbit interaction of carbon atoms in graphene promises a long spin diffusion length and the potential to create a spin field-effect transistor. Carbon 36-42 spindlin 1 Homo sapiens 10-14 27419582-0 2016 Nonvortical Rashba Spin Structure on a Surface with C_{1h} Symmetry. Carbon 52-54 spindlin 1 Homo sapiens 19-23 27419582-4 2016 This novel nonvortical RB spin structure is confirmed as a general phenomenon originating from the C_{1h} symmetry of the surface. Carbon 99-101 spindlin 1 Homo sapiens 26-30 27152812-1 2016 The small spin-orbit interaction of carbon atoms in graphene promises a long spin diffusion length and the potential to create a spin field-effect transistor. Carbon 36-42 spindlin 1 Homo sapiens 77-81 27152812-1 2016 The small spin-orbit interaction of carbon atoms in graphene promises a long spin diffusion length and the potential to create a spin field-effect transistor. Carbon 36-42 spindlin 1 Homo sapiens 77-81 26447487-0 2015 Spin-orbit interaction in bent carbon nanotubes: resonant spin transitions. Carbon 31-37 spindlin 1 Homo sapiens 0-4 26824558-0 2016 Carbon Tetragons as Definitive Spin Switches in Narrow Zigzag Graphene Nanoribbons. Carbon 0-6 spindlin 1 Homo sapiens 31-35 26824558-2 2016 Here we use first-principles calculations to show that when narrow zigzag graphene nanoribbons are connected to form junctions or superlattices, properly placed square-shaped carbon tetragons not only serve as effective bundles of the two incoming spin edge channels, but also act as definitive topological spin switches for the two outgoing channels. Carbon 175-181 spindlin 1 Homo sapiens 248-252 26824558-2 2016 Here we use first-principles calculations to show that when narrow zigzag graphene nanoribbons are connected to form junctions or superlattices, properly placed square-shaped carbon tetragons not only serve as effective bundles of the two incoming spin edge channels, but also act as definitive topological spin switches for the two outgoing channels. Carbon 175-181 spindlin 1 Homo sapiens 307-311 26621579-6 2015 Based on thermoelastic modelling along an expected geotherm, the spin crossover in ferropericlase can contribute to 2% reduction in VP/VS in a pyrolite mineralogical model in mid lower-mantle. Carbon 143-151 spindlin 1 Homo sapiens 65-69 26491888-0 2015 Bimodal Latex Effect on Spin-Coated Thin Conductive Polymer-Single-Walled Carbon Nanotube Layers. Carbon 74-80 spindlin 1 Homo sapiens 24-28 26447487-0 2015 Spin-orbit interaction in bent carbon nanotubes: resonant spin transitions. Carbon 31-37 spindlin 1 Homo sapiens 58-62 26447487-1 2015 We develop an effective tight-binding Hamiltonian for spin-orbit (SO) interaction in bent carbon nanotubes (CNT) for the electrons forming the pi bonds between the nearest neighbor atoms. Carbon 90-96 spindlin 1 Homo sapiens 54-58 25899290-8 2015 Optimizations of the TEDOR pulse scheme in the case of a quadrupolar nucleus with a small quadrupole coupling constant show that it is most efficient when pulses are positioned on the spin-1/2 (carbon-13) nucleus. Carbon 194-200 spindlin 1 Homo sapiens 184-192 26344174-3 2015 In this work, the rapid and controllable spin-spray layer-by-layer (SSLbL) method is used to generate high quality networks of 1D nanomaterials: single-walled carbon nanotubes (SWNT) and vanadium pentoxide (V2O5) nanowires for anode and cathode electrodes, respectively. Carbon 159-165 spindlin 1 Homo sapiens 41-45 26371657-4 2015 The spin tune is deduced from the up-down asymmetry of deuteron-carbon scattering. Carbon 64-70 spindlin 1 Homo sapiens 4-8 24968260-8 2014 The spectra indicate a significant electron/spin density (rho ~ 0.1) on each meso-carbon atom. Carbon 82-88 spindlin 1 Homo sapiens 44-48 26261966-1 2015 Using density functional theory, a possible pathway of soot surface growth is studied in the low-temperature, postflame region in which spin-triplet polycyclic aromatic hydrocarbon (PAH) molecules with a small singlet-triplet energy gap react with unsaturated aliphatics such as acetylene via the carbon-addition-hydrogen-migration (CAHM) reaction. Carbon 174-180 spindlin 1 Homo sapiens 136-140 25353381-6 2014 The character and origin of the carbon-centered spin-adducts was confirmed using nitroso spin trapping agents. Carbon 32-38 spindlin 1 Homo sapiens 48-52 25353381-6 2014 The character and origin of the carbon-centered spin-adducts was confirmed using nitroso spin trapping agents. Carbon 32-38 spindlin 1 Homo sapiens 89-93 24737463-2 2014 Spin-trapping experiments indicate both an aryl-type radical and an oxidising radical, trapped as a carbon-centred radical, are formed from the protonated radical anion of SN30000. Carbon 100-106 spindlin 1 Homo sapiens 0-4 23644525-2 2013 Owing to their exceptionally long spin lifetimes, these carbon-based materials could also have an important impact on spintronics, where carrier spins play a key role in transmitting, processing and storing information. Carbon 56-62 spindlin 1 Homo sapiens 34-38 24116805-1 2013 Spin-orbit interaction provides a spin filtering effect in carbon nanotube based Cooper pair splitters that allows us to determine spin correlators directly from current measurements. Carbon 59-65 spindlin 1 Homo sapiens 0-4 24116805-1 2013 Spin-orbit interaction provides a spin filtering effect in carbon nanotube based Cooper pair splitters that allows us to determine spin correlators directly from current measurements. Carbon 59-65 spindlin 1 Homo sapiens 34-38 24116805-1 2013 Spin-orbit interaction provides a spin filtering effect in carbon nanotube based Cooper pair splitters that allows us to determine spin correlators directly from current measurements. Carbon 59-65 spindlin 1 Homo sapiens 131-135 24584481-5 2014 Our calculations together with a spin-dependent tight binding model ascribe the diffuse nature of the pi-bands to the multiple spin-split bands originated from the spin-injected carbon atoms residing only in the lower graphene layer. Carbon 178-184 spindlin 1 Homo sapiens 33-37 24584481-5 2014 Our calculations together with a spin-dependent tight binding model ascribe the diffuse nature of the pi-bands to the multiple spin-split bands originated from the spin-injected carbon atoms residing only in the lower graphene layer. Carbon 178-184 spindlin 1 Homo sapiens 127-131 24584481-5 2014 Our calculations together with a spin-dependent tight binding model ascribe the diffuse nature of the pi-bands to the multiple spin-split bands originated from the spin-injected carbon atoms residing only in the lower graphene layer. Carbon 178-184 spindlin 1 Homo sapiens 127-131 26276616-0 2014 Charge Separation in P3HT:SWCNT Blends Studied by EPR: Spin Signature of the Photoinduced Charged State in SWCNT. Carbon 26-31 spindlin 1 Homo sapiens 55-59 26290968-4 2012 These molecules undergo a thermally induced, fully reversible, gradual spin crossover with a transition temperature of T1/2 = 235(6) K and a transition width of DeltaT80 = 115(8) K. Our results show that by using a carbon-based substrate the spin-crossover behavior can be preserved even for molecules that are in direct contact with a solid surface. Carbon 215-221 spindlin 1 Homo sapiens 71-75 23742482-1 2013 Spin-orbit (de-)excitation of C(+)((2)P) by collisions with H2, a key process for astrochemistry, is investigated. Carbon 30-34 spindlin 1 Homo sapiens 0-4 23377456-0 2013 Strong spin-phonon coupling between a single-molecule magnet and a carbon nanotube nanoelectromechanical system. Carbon 67-73 spindlin 1 Homo sapiens 7-11 23377456-7 2013 Here, we provide the first experimental evidence for a strong spin-phonon coupling between a single molecule spin and a carbon nanotube resonator, ultimately enabling coherent spin manipulation and quantum entanglement. Carbon 120-126 spindlin 1 Homo sapiens 62-66 23377456-7 2013 Here, we provide the first experimental evidence for a strong spin-phonon coupling between a single molecule spin and a carbon nanotube resonator, ultimately enabling coherent spin manipulation and quantum entanglement. Carbon 120-126 spindlin 1 Homo sapiens 109-113 23377456-7 2013 Here, we provide the first experimental evidence for a strong spin-phonon coupling between a single molecule spin and a carbon nanotube resonator, ultimately enabling coherent spin manipulation and quantum entanglement. Carbon 120-126 spindlin 1 Homo sapiens 109-113 26290968-4 2012 These molecules undergo a thermally induced, fully reversible, gradual spin crossover with a transition temperature of T1/2 = 235(6) K and a transition width of DeltaT80 = 115(8) K. Our results show that by using a carbon-based substrate the spin-crossover behavior can be preserved even for molecules that are in direct contact with a solid surface. Carbon 215-221 spindlin 1 Homo sapiens 242-246 22874974-5 2012 In particular, the bromination on beta-pyrrole carbon atoms of the meso-substituted (oxo)manganese(V) corrole strikingly enhances the spin-orbit coupling interaction and results in the dramatic increase of reactivity. Carbon 47-53 spindlin 1 Homo sapiens 134-138 22979850-0 2012 Highly tunable spin-dependent electron transport through carbon atomic chains connecting two zigzag graphene nanoribbons. Carbon 57-63 spindlin 1 Homo sapiens 15-19 22975243-1 2012 The NMR hyperpolarization observed for freely rotating methyl groups by exerting a temperature jump from 4.2 K to 298 K can be transferred to spins which have a spin, spin coupling with the carbon of the methyl group. Carbon 190-196 spindlin 1 Homo sapiens 142-146 22975243-1 2012 The NMR hyperpolarization observed for freely rotating methyl groups by exerting a temperature jump from 4.2 K to 298 K can be transferred to spins which have a spin, spin coupling with the carbon of the methyl group. Carbon 190-196 spindlin 1 Homo sapiens 161-165 22979850-1 2012 Motivated by recent experiments of successfully carving out stable carbon atomic chains from graphene, we investigate a device structure of a carbon chain connecting two zigzag graphene nanoribbons with highly tunable spin-dependent transport properties. Carbon 67-73 spindlin 1 Homo sapiens 218-222 22979850-1 2012 Motivated by recent experiments of successfully carving out stable carbon atomic chains from graphene, we investigate a device structure of a carbon chain connecting two zigzag graphene nanoribbons with highly tunable spin-dependent transport properties. Carbon 142-148 spindlin 1 Homo sapiens 218-222 23003173-1 2012 We theoretically investigate the deflection-induced coupling of an electron spin to vibrational motion due to spin-orbit coupling in suspended carbon nanotube quantum dots. Carbon 143-149 spindlin 1 Homo sapiens 76-80 23003173-1 2012 We theoretically investigate the deflection-induced coupling of an electron spin to vibrational motion due to spin-orbit coupling in suspended carbon nanotube quantum dots. Carbon 143-149 spindlin 1 Homo sapiens 110-114 22680745-5 2012 Our results demonstrate a new approach for controlling spin-dependent transport in carbon nanotube double dot devices. Carbon 83-89 spindlin 1 Homo sapiens 55-59 22423853-6 2012 This leads to reduced electron spin-spin interaction and hence almost negligible intrinsic magnetism in the carbon-based PAHs and carbon nanographene fragments. Carbon 108-114 spindlin 1 Homo sapiens 31-35 22423853-6 2012 This leads to reduced electron spin-spin interaction and hence almost negligible intrinsic magnetism in the carbon-based PAHs and carbon nanographene fragments. Carbon 108-114 spindlin 1 Homo sapiens 36-40 22239772-4 2012 This paper makes a comparative assessment of the different approaches by applying them to potential energy surfaces for different spin states of the oxygen and carbon dimer. Carbon 160-166 spindlin 1 Homo sapiens 130-134 23198093-0 2012 Spin-based optomechanics with carbon nanotubes. Carbon 30-36 spindlin 1 Homo sapiens 0-4 23198093-1 2012 A simple scheme for determination of spin-orbit coupling strength in spinbased optomechanics with carbon nanotubes is introduced, under the control of a strong pump field and a weak signal field. Carbon 98-104 spindlin 1 Homo sapiens 37-41 21721654-0 2011 Spin transport properties of single metallocene molecules attached to single-walled carbon nanotubes via nickel adatoms. Carbon 84-90 spindlin 1 Homo sapiens 0-4 22088060-1 2011 The role of spin-orbit and rotational couplings in radiative association of C((3)P) and N((4)S) atoms is investigated. Carbon 76-77 spindlin 1 Homo sapiens 12-16 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. Carbon 155-161 spindlin 1 Homo sapiens 0-4 21721654-1 2011 The spin-dependent transport properties of single ferrocene, cobaltocene, and nickelocene molecules attached to the sidewall of a (4,4) armchair single-walled carbon nanotube via a Ni adatom are investigated by using a self-consistent ab initio approach that combines the non-equilibrium Green"s function formalism with the spin density functional theory. Carbon 159-165 spindlin 1 Homo sapiens 4-8 20136329-0 2010 Spin filter effect of manganese phthalocyanine contacted with single-walled carbon nanotube electrodes. Carbon 76-82 spindlin 1 Homo sapiens 0-4 20459188-0 2010 Erratum: "Spin filter effect of manganese phthalocyanine contacted with single-walled carbon nanotube electrodes" [J. Chem. Carbon 86-92 spindlin 1 Homo sapiens 10-14 21317495-0 2011 The effect of amine protonation on the electrical properties of spin-assembled single-walled carbon nanotube networks. Carbon 93-99 spindlin 1 Homo sapiens 64-68 20136329-1 2010 We present a theoretical study of the spin transport through a manganese phthalocyanine (MnPc) molecule sandwiched between two semi-infinite armchair single-walled carbon nanotube (SWCNT) electrodes. Carbon 164-170 spindlin 1 Homo sapiens 38-42 20136329-5 2010 The spin filter effect of MnPc is very robust regardless of whether the open ends of the SWCNT electrodes are terminated by hydrogen, fluorine, or carbon dimers, demonstrating its promising applications in future molecular spintronics. Carbon 147-153 spindlin 1 Homo sapiens 4-8 19275141-0 2009 Spin state splitting in carbon gasification models. Carbon 24-30 spindlin 1 Homo sapiens 0-4 20010828-6 2010 The electric modification of the spin polarization relies on discrete states in the Si with a Zeeman spin splitting, an approach that is also applicable to organic, carbon-based and other materials with weak spin-orbit interaction. Carbon 165-171 spindlin 1 Homo sapiens 33-37 20010828-6 2010 The electric modification of the spin polarization relies on discrete states in the Si with a Zeeman spin splitting, an approach that is also applicable to organic, carbon-based and other materials with weak spin-orbit interaction. Carbon 165-171 spindlin 1 Homo sapiens 101-105 20010828-6 2010 The electric modification of the spin polarization relies on discrete states in the Si with a Zeeman spin splitting, an approach that is also applicable to organic, carbon-based and other materials with weak spin-orbit interaction. Carbon 165-171 spindlin 1 Homo sapiens 101-105 19772319-2 2009 Spin trapping with 5,5"-dimethylpyrroline 1-N-oxide (DMPO) gave a composite spectrum of a carbon-centered radical and the well-known DMPO-OH adduct. Carbon 90-96 spindlin 1 Homo sapiens 0-4 19772319-4 2009 Furthermore, using the closely related spin trap 5-diethoxyphosphoryl-5-methylpyrroline N-oxide (DEPMPO), which is less prone to oxidation than DMPO, gave only a carbon-centered radical spectrum without any involvement of a (*)OH radical. Carbon 162-168 spindlin 1 Homo sapiens 39-43 19772319-5 2009 Reduction of a more soluble analogue of TPZ, in redox equilibrium with its 1-oxide derivative, led to spin trapping of both a carbon-centered radical and a nitrogen-centered radical by N-tert-butyl-alpha-phenylnitrone (PBN). Carbon 126-132 spindlin 1 Homo sapiens 102-106 20000481-2 2010 In the M = 2S + 1 = 13 (S is the total spin) ground state (GS) of Fe(6)-(C(6)H(6))(3) each benzene is bonded with one Fe atom, forming eta(6) coordinations with C-Fe contacts of 2.12-2.17 A; though the Fe(6) cluster structure is preserved, it presents more distortion than in bare Fe(6). Carbon 73-74 spindlin 1 Homo sapiens 39-43 19572757-5 2009 The first spin inversion, from the sextet state to the quartet state, makes the activation of the C-H bond energetically spontaneous. Carbon 98-99 spindlin 1 Homo sapiens 10-14 19385592-3 2009 The spin density distributions in the triplet state were found to be similar for bacteriochlorophyll a and bacteriochlorophyll b except for the presence of spin density on carbon 8(1) in bacteriochlorophyll b. Judging from a comparison with ENDOR experiments for the radical cation and anion, the triplet state in bacteriochlorophylls cannot be explained as being a simple HOMO-->LUMO excitation of Gouterman orbitals. Carbon 172-178 spindlin 1 Homo sapiens 156-160 17559287-2 2007 This three-terminal configuration allows the resistance to the source and drain electrodes to be individually measured, which we exploit to demonstrate that electrons were added to spin-degenerate states of the carbon nanotube. Carbon 211-217 spindlin 1 Homo sapiens 181-185 18518136-0 2008 Electrically tunable spin polarization in a carbon nanotube spin diode. Carbon 44-50 spindlin 1 Homo sapiens 21-25 18518136-0 2008 Electrically tunable spin polarization in a carbon nanotube spin diode. Carbon 44-50 spindlin 1 Homo sapiens 60-64 17706456-0 2008 Spin probe ESR studies of dynamics of single walled carbon nanotubes. Carbon 52-58 spindlin 1 Homo sapiens 0-4 17706456-1 2008 The highly sensitive technique of spin-probe Electron Spin Resonance (ESR) has been used to study dynamics of carbon nanotubes. Carbon 110-116 spindlin 1 Homo sapiens 34-38 17706456-1 2008 The highly sensitive technique of spin-probe Electron Spin Resonance (ESR) has been used to study dynamics of carbon nanotubes. Carbon 110-116 spindlin 1 Homo sapiens 54-58 17417840-0 2007 Spin-state selective carbon-detected HNCO with TROSY optimization in all dimensions and double echo-antiecho sensitivity enhancement in both indirect dimensions. Carbon 21-27 spindlin 1 Homo sapiens 0-4