PMID-sentid Pub_year Sent_text comp_official_name comp_offsetprotein_name organism prot_offset 18352430-2 2008 We create large spin-orbit splittings in a Au and Ag monolayer on W(110) and show that the size of the splitting does not depend on the atomic number of the Au or Ag overlayer but of the W substrate. Gold 43-45 spindlin 1 Homo sapiens 16-20 33136367-6 2020 Here, we report definitive observation of CISS-induced magnetoconductance in vertical heterojunctions of (Ga,Mn)As/AHPA-L molecules/Au, directly verifying spin filtering by the AHPA-L molecules via spin detection by the (Ga,Mn)As. Gold 132-134 spindlin 1 Homo sapiens 155-159 17915934-2 2007 For certain metal surfaces, such as the Au(111) surface, the experimentally observed spin-orbit coupling results in spin rotation lengths on the order of tens of nanometers, which is the typical length scale associated with quantum corral structures formed on metal surfaces. Gold 40-42 spindlin 1 Homo sapiens 85-89 17915934-2 2007 For certain metal surfaces, such as the Au(111) surface, the experimentally observed spin-orbit coupling results in spin rotation lengths on the order of tens of nanometers, which is the typical length scale associated with quantum corral structures formed on metal surfaces. Gold 40-42 spindlin 1 Homo sapiens 116-120 15053665-0 2004 Polydisperse composition of mixed monolayer-protected, spin-labeled Au nanoparticles. Gold 68-70 spindlin 1 Homo sapiens 55-59 14750677-0 2004 Spin-labelled Au nanoparticles. Gold 14-16 spindlin 1 Homo sapiens 0-4 14750677-1 2004 A series of Au nanoparticles functionalised with nitroxide spin labels has been prepared and studied by EPR spectroscopy. Gold 12-14 spindlin 1 Homo sapiens 59-63 33672227-0 2021 Spin-Orbit Coupling Effects in Au 4f Core-Level Electronic Structures in Supported Low-Dimensional Gold Nanoparticles. Gold 31-33 spindlin 1 Homo sapiens 0-4 33672227-2 2021 Herein, upon analyzing the Au 4f core-level spin-orbit components in many as-synthesized AuNP-based catalysts, we observed that like deviations in the Au 4f7/2 binding energy positions, both the Au 4f7/2-to-Au 4f5/2 peak intensity and linewidth ratios varied largely from the standard statistical bulk reference values. Gold 27-29 spindlin 1 Homo sapiens 44-48 33672227-2 2021 Herein, upon analyzing the Au 4f core-level spin-orbit components in many as-synthesized AuNP-based catalysts, we observed that like deviations in the Au 4f7/2 binding energy positions, both the Au 4f7/2-to-Au 4f5/2 peak intensity and linewidth ratios varied largely from the standard statistical bulk reference values. Gold 89-91 spindlin 1 Homo sapiens 44-48 33672227-2 2021 Herein, upon analyzing the Au 4f core-level spin-orbit components in many as-synthesized AuNP-based catalysts, we observed that like deviations in the Au 4f7/2 binding energy positions, both the Au 4f7/2-to-Au 4f5/2 peak intensity and linewidth ratios varied largely from the standard statistical bulk reference values. Gold 89-91 spindlin 1 Homo sapiens 44-48 33672227-2 2021 Herein, upon analyzing the Au 4f core-level spin-orbit components in many as-synthesized AuNP-based catalysts, we observed that like deviations in the Au 4f7/2 binding energy positions, both the Au 4f7/2-to-Au 4f5/2 peak intensity and linewidth ratios varied largely from the standard statistical bulk reference values. Gold 89-91 spindlin 1 Homo sapiens 44-48 33496295-4 2021 Layer-resolved DMI calculations revealed that the sign of the spin-orbit coupling (SOC) energy was changed for Au near the interface of Au/Fe under tensile stress, subsequently reversing the chirality of the i-DMI from left-handed to right-handed. Gold 111-113 spindlin 1 Homo sapiens 62-66 33496295-4 2021 Layer-resolved DMI calculations revealed that the sign of the spin-orbit coupling (SOC) energy was changed for Au near the interface of Au/Fe under tensile stress, subsequently reversing the chirality of the i-DMI from left-handed to right-handed. Gold 136-138 spindlin 1 Homo sapiens 62-66 33273540-0 2020 The impact of Fe atom on the spin-filter and spin thermoelectric properties of Au-Fe@C20-Au monomer and dimer systems. Gold 79-81 spindlin 1 Homo sapiens 29-33 33273540-0 2020 The impact of Fe atom on the spin-filter and spin thermoelectric properties of Au-Fe@C20-Au monomer and dimer systems. Gold 79-81 spindlin 1 Homo sapiens 45-49 33273540-0 2020 The impact of Fe atom on the spin-filter and spin thermoelectric properties of Au-Fe@C20-Au monomer and dimer systems. Gold 89-91 spindlin 1 Homo sapiens 29-33 33273540-0 2020 The impact of Fe atom on the spin-filter and spin thermoelectric properties of Au-Fe@C20-Au monomer and dimer systems. Gold 89-91 spindlin 1 Homo sapiens 45-49 33273540-4 2020 We suggest that the Au-(Fe@C20)2-Au system is a suitable junction for designing spin-filtering and spin thermoelectric devices and eventually it is a good candidate for spintronic applications. Gold 20-22 spindlin 1 Homo sapiens 80-84 33273540-4 2020 We suggest that the Au-(Fe@C20)2-Au system is a suitable junction for designing spin-filtering and spin thermoelectric devices and eventually it is a good candidate for spintronic applications. Gold 20-22 spindlin 1 Homo sapiens 99-103 17455490-8 2007 When the Au capping layer with a short spin-diffusion length replaces the Cu capping layer with a long spin-diffusion length, the reduction of the critical switching current is also observed. Gold 9-11 spindlin 1 Homo sapiens 39-43 17455490-8 2007 When the Au capping layer with a short spin-diffusion length replaces the Cu capping layer with a long spin-diffusion length, the reduction of the critical switching current is also observed. Gold 9-11 spindlin 1 Homo sapiens 103-107 15698224-3 2005 The hole transmission of a Ni(81)Fe(19)/Au/Co trilayer is clearly spin dependent, resulting in a surprisingly large current change by a factor of 2.3 in a magnetic field. Gold 40-42 spindlin 1 Homo sapiens 66-70 34623852-0 2021 Observation of Pure-Spin-Current Diodelike Effect at the Au/Pt Interface. Gold 57-59 spindlin 1 Homo sapiens 20-24 34623852-4 2021 Here we demonstrate asymmetric transport of pure-spin currents across an interface of dissimilar nonmagnetic materials Au/Pt. Gold 119-121 spindlin 1 Homo sapiens 49-53 34623852-5 2021 We exploit Py/Au/Pt/Co structures where spin pumping can generate pure-spin current from either Py or Co independently. Gold 14-16 spindlin 1 Homo sapiens 40-44 34623852-5 2021 We exploit Py/Au/Pt/Co structures where spin pumping can generate pure-spin current from either Py or Co independently. Gold 14-16 spindlin 1 Homo sapiens 71-75 34623852-6 2021 We find that the transmission of pure-spin current from Au into Pt is twice as efficient as transmission from Pt into Au. Gold 56-58 spindlin 1 Homo sapiens 38-42 34623852-7 2021 Experimental results are interpreted by extending conventional spin-pumping, spin-diffusion theory to include boundary conditions of reflected and transmitted spin current at the Au/Pt interface that are proportional to the established spin chemical potentials on either side of the interface. Gold 179-181 spindlin 1 Homo sapiens 63-67 34623852-7 2021 Experimental results are interpreted by extending conventional spin-pumping, spin-diffusion theory to include boundary conditions of reflected and transmitted spin current at the Au/Pt interface that are proportional to the established spin chemical potentials on either side of the interface. Gold 179-181 spindlin 1 Homo sapiens 77-81 34623852-7 2021 Experimental results are interpreted by extending conventional spin-pumping, spin-diffusion theory to include boundary conditions of reflected and transmitted spin current at the Au/Pt interface that are proportional to the established spin chemical potentials on either side of the interface. Gold 179-181 spindlin 1 Homo sapiens 159-163 34623852-7 2021 Experimental results are interpreted by extending conventional spin-pumping, spin-diffusion theory to include boundary conditions of reflected and transmitted spin current at the Au/Pt interface that are proportional to the established spin chemical potentials on either side of the interface. Gold 179-181 spindlin 1 Homo sapiens 236-240 33543525-0 2021 Hierarchical Spin-Crossover Cooperativity in Hybrid 1-D Chains of FeII-1,2,4-trizole Trimers Linked by [Au(CN)2]- Bridges. Gold 104-106 spindlin 1 Homo sapiens 13-17 33619343-0 2021 Broadband optical spin dependent reflection in self-assembled GaAs-based nanowires asymmetrically hybridized with Au. Gold 114-116 spindlin 1 Homo sapiens 18-22 32611013-5 2020 The latter is based on spin-polarized low-energy electron diffraction on an Au-passivated iridium crystal. Gold 76-78 spindlin 1 Homo sapiens 23-27 29365269-3 2018 Using angle- and spin-resolved photoemission spectroscopy, we show that the Dirac state in the Au-intercalated graphene on Co(0001) experiences giant splitting (up to 0.2 eV) while being by no means distorted due to interaction with the substrate. Gold 95-97 spindlin 1 Homo sapiens 17-21 32301607-5 2020 The complex [Au] exhibits an incomplete stepped spin transition as a function of the temperature with TSCO1 = 170 K and TSCO2 = 308 K for the two subsequent steps. Gold 13-15 spindlin 1 Homo sapiens 48-52 32031846-0 2020 Retraction: Neel Spin-Orbit Torque Driven Antiferromagnetic Resonance in Mn_{2}Au Probed by Time-Domain THz Spectroscopy [Phys. Gold 79-81 spindlin 1 Homo sapiens 17-21 30998264-6 2019 Temperature-dependent charge-transport measurements of an electrical device based on assemblies of these Au@SCO NPs also support this spin transition. Gold 105-107 spindlin 1 Homo sapiens 134-138 30776790-0 2019 Spin-orbit split two-dimensional states of BiTeI/Au(1 1 1) interfaces. Gold 49-51 spindlin 1 Homo sapiens 0-4 30776790-3 2019 We show that the resulting interface state that originates from the modified spin-orbit split surface state of the clean Au(1 1 1) surface resides at high energy above the Fermi level and acquires a large spin-splitting and reversal helicity as compared with the original surface state. Gold 121-123 spindlin 1 Homo sapiens 77-81 30776790-3 2019 We show that the resulting interface state that originates from the modified spin-orbit split surface state of the clean Au(1 1 1) surface resides at high energy above the Fermi level and acquires a large spin-splitting and reversal helicity as compared with the original surface state. Gold 121-123 spindlin 1 Homo sapiens 205-209 30776790-5 2019 In the I-Bi-Te/Au(1 1 1) interface, this state represents a Rashba system with strong spin-orbit interaction, where the outer branch of the spin-split state is mostly populated. Gold 15-17 spindlin 1 Homo sapiens 86-90 30776790-5 2019 In the I-Bi-Te/Au(1 1 1) interface, this state represents a Rashba system with strong spin-orbit interaction, where the outer branch of the spin-split state is mostly populated. Gold 15-17 spindlin 1 Homo sapiens 140-144 30312046-0 2018 Spin Structure of K Valleys in Single-Layer WS_{2} on Au(111). Gold 54-56 spindlin 1 Homo sapiens 0-4 30312046-1 2018 The spin structure of the valence and conduction bands at the K[over ] and K[over ]^{"} valleys of single-layer WS_{2} on Au(111) is determined by spin- and angle-resolved photoemission and inverse photoemission. Gold 124-126 spindlin 1 Homo sapiens 4-8 26212127-2 2015 Here we show that Au-intercalated graphene on Fe(110) displays a large (~230 meV) bandgap with out-of-plane hedgehog-type spin reorientation around the gapped Dirac point. Gold 18-20 spindlin 1 Homo sapiens 122-126 28731774-4 2017 Considering the calculated spin-dependent Fe/Au interface transmittance we conclude that a nonthermal spin-dependent Seebeck effect is responsible for the generation of ultrashort spin current pulses. Gold 45-47 spindlin 1 Homo sapiens 27-31 28731774-4 2017 Considering the calculated spin-dependent Fe/Au interface transmittance we conclude that a nonthermal spin-dependent Seebeck effect is responsible for the generation of ultrashort spin current pulses. Gold 45-47 spindlin 1 Homo sapiens 102-106 28731774-4 2017 Considering the calculated spin-dependent Fe/Au interface transmittance we conclude that a nonthermal spin-dependent Seebeck effect is responsible for the generation of ultrashort spin current pulses. Gold 45-47 spindlin 1 Homo sapiens 102-106 28731774-5 2017 The demonstrated rotation of spin polarization of hot electrons upon interaction with noncollinear magnetization at Au/Fe interfaces holds high potential for future spintronic devices. Gold 116-118 spindlin 1 Homo sapiens 29-33 25840475-2 2015 Measurements of the band structure of a Au(111) single crystal surface demonstrate an energy resolution of DeltaE=12 meV and a momentum resolution of Deltak =0.0049 A(-1), measured at the line-width of the spin-orbit split Shockley surface state. Gold 40-42 spindlin 1 Homo sapiens 206-210 25840475-4 2015 Spin resolution in the full momentum image is obtained by an imaging spin-filter based on low-energy electron diffraction at a Au passivated Ir(100) single crystal. Gold 127-129 spindlin 1 Homo sapiens 0-4 25840475-4 2015 Spin resolution in the full momentum image is obtained by an imaging spin-filter based on low-energy electron diffraction at a Au passivated Ir(100) single crystal. Gold 127-129 spindlin 1 Homo sapiens 69-73 26446292-4 2015 Pristine Si nanoterraces impose a strain on the neighboring Au-Si wires, which modifies both the band structure of metallic chains and the magnetic property of spin chains. Gold 60-62 spindlin 1 Homo sapiens 160-164 26974012-3 2016 In some cases--specifically, for Si(553)-Au and Si(557)-Au--a large fraction of the silicon atoms at the exposed edge of this strip are known to be spin-polarized and charge-ordered along the edge. Gold 56-58 spindlin 1 Homo sapiens 148-152 26974012-5 2016 Here, we demonstrate theoretically as well as experimentally that the closely related Si(775)-Au surface has--despite its very similar overall structure--zero spin polarization at its step edge. Gold 94-96 spindlin 1 Homo sapiens 159-163 26974012-7 2016 The model also predicts that unintentional defects and intentional dopants can create local spin moments at Si(hhk)-Au step edges. Gold 116-118 spindlin 1 Homo sapiens 92-96 26675052-4 2016 The molecular wire is built by trapping individual spin crossover Fe(II) complexes between one Au electrode and one ferromagnetic Ni electrode in an organic liquid medium. Gold 95-97 spindlin 1 Homo sapiens 51-55 26574362-2 2015 In this study, the recently observed qualitative differences between the platinum and gold compounds in the magnitude and the sign of spin-orbit-induced (SO) nuclear magnetic shielding at the vicinal light atom ((13)C, (15)N), sigma(SO)(LA), are explained by the contractions of 6s and 6p atomic orbitals in Au complexes, originating in the larger Au nuclear charge and stronger scalar relativistic effects in gold complexes. Gold 308-310 spindlin 1 Homo sapiens 134-138 26574362-2 2015 In this study, the recently observed qualitative differences between the platinum and gold compounds in the magnitude and the sign of spin-orbit-induced (SO) nuclear magnetic shielding at the vicinal light atom ((13)C, (15)N), sigma(SO)(LA), are explained by the contractions of 6s and 6p atomic orbitals in Au complexes, originating in the larger Au nuclear charge and stronger scalar relativistic effects in gold complexes. Gold 348-350 spindlin 1 Homo sapiens 134-138 26574362-3 2015 This leads to the chemical activation of metal 6s and 6p atomic orbitals in Au complexes and their larger participation in bonding with the ligand, which modulates the propagation of metal-induced SO effects on the NMR signal of the LA via the Spin-Orbit/Fermi Contact (SO/FC) mechanism. Gold 76-78 spindlin 1 Homo sapiens 244-248 24880311-1 2014 We investigate spin-dependent thermoelectronic transport properties of a single molecule magnet Mn(dmit)2 sandwiched between two Au electrodes using first-principles density functional theory combined with nonequilibrium Green"s function method. Gold 129-131 spindlin 1 Homo sapiens 15-19 24880311-2 2014 By applying a temperature difference between the two Au electrodes, spin-up and spin-down currents flowing in opposite directions can be induced due to asymmetric distribution of the spin-up and spin-down transmission spectra around the Fermi level. Gold 53-55 spindlin 1 Homo sapiens 68-72 24880311-2 2014 By applying a temperature difference between the two Au electrodes, spin-up and spin-down currents flowing in opposite directions can be induced due to asymmetric distribution of the spin-up and spin-down transmission spectra around the Fermi level. Gold 53-55 spindlin 1 Homo sapiens 80-84 24880311-2 2014 By applying a temperature difference between the two Au electrodes, spin-up and spin-down currents flowing in opposite directions can be induced due to asymmetric distribution of the spin-up and spin-down transmission spectra around the Fermi level. Gold 53-55 spindlin 1 Homo sapiens 80-84 24880311-2 2014 By applying a temperature difference between the two Au electrodes, spin-up and spin-down currents flowing in opposite directions can be induced due to asymmetric distribution of the spin-up and spin-down transmission spectra around the Fermi level. Gold 53-55 spindlin 1 Homo sapiens 80-84 24123564-0 2013 Spin-crossover complex on Au(111): structural and electronic differences between mono- and multilayers. Gold 26-28 spindlin 1 Homo sapiens 0-4 26282313-1 2013 Using X-ray absorption techniques, we show that temperature- and light-induced spin crossover properties are conserved for a submonolayer of the [Fe(H2B(pz)2)2(2,2"-bipy)] complex evaporated onto a Au(111) surface. Gold 198-200 spindlin 1 Homo sapiens 79-83 23249172-1 2013 We report on the unprecedented direct observation of spin-polarization transfer across colloidal magneto-plasmonic Au@Fe-oxide core@shell nanocrystal heterostructures. Gold 115-117 spindlin 1 Homo sapiens 53-57 23249172-0 2013 Spin-polarization transfer in colloidal magnetic-plasmonic Au/iron oxide hetero-nanocrystals. Gold 59-61 spindlin 1 Homo sapiens 0-4 23249172-4 2013 The angular to spin magnetic moment ratio, m(orb)/m(spin), for the Au 5d states, which was found to be equal to 0.38, appeared to be unusually large when compared to previous findings. Gold 67-69 spindlin 1 Homo sapiens 15-19 23249172-4 2013 The angular to spin magnetic moment ratio, m(orb)/m(spin), for the Au 5d states, which was found to be equal to 0.38, appeared to be unusually large when compared to previous findings. Gold 67-69 spindlin 1 Homo sapiens 52-56 21902353-2 2011 The spin mixing conductance was determined by comparing the Gilbert damping in bare YIG films with those covered by a Au/Fe/Au structure. Gold 118-120 spindlin 1 Homo sapiens 4-8 22642450-5 2012 Bis(phthalocyaninato)yttrium (YPc(2)) molecules deposited on an Au (111) surface keep their spin-1/2 magnetic moment due to the small molecule-substrate interaction. Gold 64-66 spindlin 1 Homo sapiens 92-98 21902353-2 2011 The spin mixing conductance was determined by comparing the Gilbert damping in bare YIG films with those covered by a Au/Fe/Au structure. Gold 124-126 spindlin 1 Homo sapiens 4-8 21902353-3 2011 The Fe layer in Au/Fe/Au acted as a spin sink as displayed by an increased Gilbert damping parameter alpha compared to that in the bare YIG. Gold 16-18 spindlin 1 Homo sapiens 36-40 21902353-3 2011 The Fe layer in Au/Fe/Au acted as a spin sink as displayed by an increased Gilbert damping parameter alpha compared to that in the bare YIG. Gold 22-24 spindlin 1 Homo sapiens 36-40 20482194-5 2010 A sign change of the spin Hall effect in Cu and Au hosts is obtained as a function of the impurity atom, and even light elements like Li can cause a strong effect. Gold 48-50 spindlin 1 Homo sapiens 21-25 21576768-1 2011 Substrate-induced spin-orbit splitting in graphene on Ni, Au and Ag(111) is examined on the basis of density-functional theory. Gold 58-60 spindlin 1 Homo sapiens 18-22 21364556-2 2011 Here, we switch on and off the molecular spin of a double-decker bis(phthalocyaninato)terbium(III) complex (TbPc2) adsorbed on an Au(111) surface by applying an electric current via a scanning tunnelling microscope. Gold 130-132 spindlin 1 Homo sapiens 41-45 20482209-1 2010 The influence of structural defects, in the form of step lattices, on the spin polarization of the spin-orbit split Shockley surface state of Au(111) has been investigated. Gold 142-144 spindlin 1 Homo sapiens 74-78 20482209-1 2010 The influence of structural defects, in the form of step lattices, on the spin polarization of the spin-orbit split Shockley surface state of Au(111) has been investigated. Gold 142-144 spindlin 1 Homo sapiens 99-103 20482209-5 2010 The spin texture shows in all cases spin polarization vectors tangential to the Fermi circles, with the same helicities as on Au(111). Gold 126-128 spindlin 1 Homo sapiens 4-8