human | Q5 |
P496 | ORCID iD | 0000-0002-7901-3562 |
P1053 | ResearcherID | I-3571-2013 |
P214 | VIAF ID | 77425236 |
P10832 | WorldCat Entities ID | E39PBJcWph7CbpGFfgMC3CR3Qq |
P69 | educated at | Saint Petersburg State University | Q27621 |
University of Potsdam | Q153012 | ||
P108 | employer | Helmholtz-Zentrum Berlin | Q314578 |
P735 | given name | Andrei | Q19850904 |
Andrei | Q19850904 | ||
P106 | occupation | researcher | Q1650915 |
P21 | sex or gender | male | Q6581097 |
Q34932143 | (pi, pi) electronic order in iron arsenide superconductors. |
Q57631702 | Absence of giant spin splitting in the two-dimensional electron liquid at the surface ofSrTiO3(001) |
Q57631719 | Angle-resolved and core-level photoemission study of interfacing the topological insulatorBi1.5Sb0.5Te1.7Se1.3with Ag, Nb, and Fe |
Q57987262 | Angle-resolved photoelectron spectroscopy of geometrically nonuniform surfaces |
Q57631728 | Anisotropic effect of warping on the lifetime broadening of topological surface states in angle-resolved photoemission fromBi2Te3 |
Q37659855 | Anisotropic two-dimensional electron gas at SrTiO3(110). |
Q57987214 | Atmospheric stability and doping protection of noble-metal intercalated graphene on Ni(111) |
Q57631725 | Atomic structure ofBi2Se3andBi2Te3(111) surfaces probed by photoelectron diffraction and holography |
Q57987216 | Bilayer manganites reveal polarons in the midst of a metallic breakdown |
Q57631757 | Chemical vapour deposition of graphene on Ni(111) and Co(0001) and intercalation with Au to study Dirac-cone formation and Rashba splitting |
Q57631738 | Continuous wafer-scale graphene on cubic-SiC(001) |
Q57987222 | Correlated Electrons Step by Step: Itinerant-to-Localized Transition of Fe Impurities in Free-Electron Metal Hosts |
Q36973991 | Dirac cone protected by non-symmorphic symmetry and three-dimensional Dirac line node in ZrSiS |
Q57987186 | Dirac states with knobs on: Interplay of external parameters and the surface electronic properties of three-dimensional topological insulators |
Q57987226 | Droplet-like Fermi surfaces in the anti-ferromagnetic phase of EuFe2As2, an Fe-pnictide superconductor parent compound |
Q57987230 | Effect of noble-metal contacts on doping and band gap of graphene |
Q57631739 | Effect of structural modulation and thickness of a graphene overlayer on the binding energy of the Rashba-type surface state of Ir(111) |
Q57631748 | Effects of spin-dependent quasiparticle renormalization in Fe, Co, and Ni photoemission spectra:An experimental and theoretical study |
Q57987282 | Electron structure and elemental composition of thin films of europium deposited at room temperature on a Si(100)2 × 1 surface |
Q57631731 | Electronic and spin structure of the topological insulator Bi2Te2.4Se0.6 |
Q57987264 | Electronic structure of gold nanoclusters on oxidized Ni(755) surface |
Q47664836 | Evidence for magnetic Weyl fermions in a correlated metal. |
Q57987168 | Evolution of the remnant Fermi-surface state in the lightly doped correlated spin-orbit insulator Sr2−xLaxIrO4 |
Q57987256 | Experimental and theoretical study of the morphology of commensurate and incommensurate graphene layers on Ni single-crystal surfaces |
Q58485438 | Extremely flat band in bilayer graphene |
Q57987271 | Fabrication of patterned Au films as supporting templates for one-dimensional magnetic nanostructures |
Q57987245 | Fermi surface of Ba1−xKxFe2As2 as probed by angle-resolved photoemission |
Q57987234 | Formation of spectra of quantum well states in thin Al layers on W(110) |
Q42114221 | Giant Magnetic Band Gap in the Rashba-Split Surface State of Vanadium-Doped BiTeI: A Combined Photoemission and Ab Initio Study |
Q52844929 | Giant Rashba Splitting in Pb1-x Snx Te (111) Topological Crystalline Insulator Films Controlled by Bi Doping in the Bulk. |
Q52885944 | Giant Rashba splitting in graphene due to hybridization with gold. |
Q56030514 | Graphene grown on Co(0001) films and islands: Electronic structure and its precise magnetization dependence |
Q57631721 | Highly spin-polarized Dirac fermions at the graphene/Co interface |
Q52903309 | Imaging buried molecules: fullerenes under graphene. |
Q57631742 | Induced Rashba splitting of electronic states in monolayers of Au, Cu on a W(110) substrate |
Q57987197 | Induced spin–orbit splitting in graphene: the role of atomic number of the intercalated metal andπ–d hybridization |
Q57987191 | Insights from angle-resolved photoemission spectroscopy on the metallic states ofYbB6(001):E(k)dispersion, temporal changes, and spatial variation |
Q57631752 | Intact Dirac Cones at Broken Sublattice Symmetry: Photoemission Study of Graphene on Ni and Co |
Q57631743 | Intact Dirac cone of Bi2Te3covered with a monolayer Fe |
Q52889250 | Ir(111) surface state with giant Rashba splitting persists under graphene in air. |
Q52912355 | Is there a rashba effect in graphene on 3d ferromagnets? |
Q57987201 | Kondo Hybridization and the Origin of Metallic States at the (001) Surface ofSmB6 |
Q57987238 | Large spin-orbit splitting in light quantum films: Al/W(110) |
Q57631694 | Laser-induced persistent photovoltage on the surface of a ternary topological insulator at room temperature |
Q57987267 | Low-dimensional structures on carbon-terminated W(110): from metallic nanowires to molecular chains |
Q57987275 | Magic numbers in two-dimensional self-organization ofC60molecules |
Q57631753 | Minigap isotropy and broken chirality in graphene with periodic corrugation enhanced by cluster superlattices |
Q57987247 | Momentum dependence of the superconducting gap inBa1−xKxFe2As2 |
Q57987248 | Momentum-resolved superconducting gap in the bulk of Ba1−xKxFe2As2from combined ARPES and μSR measurements |
Q57631684 | Nanostructural origin of giant Rashba effect in intercalated graphene |
Q39418145 | Negligible surface reactivity of topological insulators Bi2Se3 and Bi2Te3 towards oxygen and water |
Q57987179 | Non-symmorphic band degeneracy at the Fermi level in ZrSiTe |
Q36605079 | Nonmagnetic band gap at the Dirac point of the magnetic topological insulator (Bi(1-x)Mn(x))2Se3 |
Q57987249 | Nonmonotonic pseudogap in high-Tccuprates |
Q39194968 | Observation of quantum-tunnelling-modulated spin texture in ultrathin topological insulator Bi2Se3 films |
Q57987239 | Observation of the Fermi surface, the band structure, and their diffraction replicas ofSr14−xCaxCu24O41by angle-resolved photoemission spectroscopy |
Q57987241 | Orbital character variation of the Fermi surface and doping dependent changes of the dimensionality inBaFe2−xCoxAs2from angle-resolved photoemission spectroscopy |
Q57987257 | Origin of Au nanostructures on tungsten surface carbides |
Q57987259 | Origin of Spin-Orbit Splitting for Monolayers of Au and Ag on W(110) and Mo(110) |
Q57987269 | Oxidation of Au on vicinal W(110): Role of step edges and facets |
Q57987284 | Photoemission from surface-localized structures on vicinal surfaces: Initial- or final-state superlattice effect? |
Q57631735 | Photoemission ofBi2Se3with Circularly Polarized Light: Probe of Spin Polarization or Means for Spin Manipulation? |
Q52935418 | Probing the ground state electronic structure of a correlated electron system by quantum well states: Ag/Ni(111). |
Q57631754 | Probing two topological surface bands of Sb2Te3by spin-polarized photoemission spectroscopy |
Q60150839 | Publisher’s Note: Correlated Electrons Step by Step: Itinerant-to-Localized Transition of Fe Impurities in Free-Electron Metal Hosts [Phys. Rev. Lett.104, 117601 (2010)] |
Q57631758 | Quantitative determination of spin-dependent quasiparticle lifetimes and electronic correlations in hcp cobalt |
Q52913712 | Quantum cavity for spin due to spin-orbit interaction at a metal boundary. |
Q57987250 | Quantum-size effects in the electronic structure of low-dimensional metallic systems |
Q57987289 | Quantum-well states and lateral superlattice effect in Ag and Au stripes on stepped W(1 4 5) |
Q57987276 | Quantum-well states in a thin Ag film on a Ni(111) substrate |
Q57631711 | Rashba splitting of 100 meV in Au-intercalated graphene on SiC |
Q52883699 | Reversal of the circular dichroism in angle-resolved photoemission from Bi2Te3. |
Q57631737 | Rotated domain network in graphene on cubic-SiC(001) |
Q57987291 | Self-organization of one-dimensional Au nanowires on a surface carbide and lateral electron quantization |
Q57631745 | Spin splitting of Dirac fermions in aligned and rotated graphene on Ir(111) |
Q57631716 | Spin splitting of Dirac fermions in graphene on Ni intercalated with alloy of Bi and Au |
Q57987210 | Spin-dependent avoided-crossing effect on quantum-well states in Al/W(110) |
Q57631746 | Spin-resolved photoemission andab initiotheory of graphene/SiC |
Q57631761 | Strength of Correlation Effects in the Electronic Structure of Iron |
Q57987193 | Strong electron pairing at the iron 3dxz,yzorbitals in hole-doped BaFe2As2superconductors revealed by angle-resolved photoemission spectroscopy |
Q57987279 | Structural and electronic properties of graphite layers grown on SiC(0001) |
Q57987217 | Structural stability of stepped nickel surfaces |
Q57987294 | Structure and quantum-size effects in a surface carbide:W(110)∕C−R(15×3) |
Q57987218 | Structure of graphene on the Ni(110) surface |
Q57631698 | Subpicosecond spin dynamics of excited states in the topological insulator Bi2Te3 |
Q57987243 | Substrate-induced spin-orbit splitting of quantum-well and interface states in Au, Ag, and Cu layers of different thicknesses on W(110) and Mo(110) surfaces |
Q57631700 | Suppression of electron scattering resonances in graphene by quantum dots |
Q57631713 | Surface Fermi arc connectivity in the type-II Weyl semimetal candidateWTe2 |
Q57987298 | Surface phonon and valence band dispersions in graphite overlayers formed by solid-state graphitization of6H−SiC(0001) |
Q44606306 | Tailoring the nature and strength of electron-phonon interactions in the SrTiO3(001) 2D electron liquid |
Q57987252 | Temperature and Doping-Dependent Renormalization Effects of the Low Energy Electronic Structure ofBa1−xKxFe2As2Single Crystals |
Q57631747 | The graphene/Au/Ni interface and its application in the construction of a graphene spin filter |
Q57987219 | The role of the covalent interaction in the formation of the electronic structure of Au- and Cu-intercalated graphene on Ni(111) |
Q57631686 | Tilted Dirac cone on W(110) protected by mirror symmetry |
Q51554306 | Tolerance of topological surface states towards magnetic moments: Fe on Bi2Se3. |
Q42379650 | Topological quantum phase transition from mirror to time reversal symmetry protected topological insulator. |
Q57987211 | Topology of spin polarization of the 5dstates on W(110) and Al/W(110) surfaces |
Q51797768 | Transport Gap Opening and High On-Off Current Ratio in Trilayer Graphene with Self-Aligned Nanodomain Boundaries. |
Q35917154 | Tunable Fermi level and hedgehog spin texture in gapped graphene |
Q57987299 | Two Alternative Ways for Formation of Mono‐atomic Carbon Layer on Ni(1 1 1): Organic‐Gas Cracking and Thermal Decomposition of Fullerenes in Thin Film |
Q57987253 | Two Energy Gaps and Fermi-Surface “Arcs” inNbSe2 |
Q57631714 | Ultrafast spin-polarization control of Dirac fermions in topological insulators |
Q57987184 | X-ray natural birefringence in reflection from graphene |
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