human | Q5 |
P2798 | Loop ID | 293480 |
P496 | ORCID iD | 0000-0002-5046-4829 |
P1053 | ResearcherID | G-6743-2012 |
P1153 | Scopus author ID | 7005507647 |
P69 | educated at | Moscow Institute of Physics and Technology | Q1367256 |
P108 | employer | Leibniz Institute for Solid State and Materials Research | Q835883 |
P106 | occupation | researcher | Q1650915 |
P21 | sex or gender | male | Q6581097 |
Q34932143 | (pi, pi) electronic order in iron arsenide superconductors. |
Q62647066 | About the relation between the quasiparticle Green’s function in cuprates obtained from ARPES data and the magnetic susceptibility |
Q62383003 | Absence of surface states for LiFeAs investigated using density functional calculations |
Q56813129 | An ARPES view on the high-T c problem: Phonons vs. spin-fluctuations |
Q36375074 | Angle-resolved photoemission spectroscopy at ultra-low temperatures |
Q62382936 | Angle-resolved photoemission spectroscopy of superconducting LiFeAs: Evidence for strong electron-phonon coupling |
Q62647068 | Anomalous Quasiparticle Renormalization inNa0.73CoO2: Role of Interorbital Interactions and Magnetic Correlations |
Q73477054 | Anomalous enhancement of the coupling to the magnetic resonance mode in underdoped Pb-Bi2212 |
Q62382892 | Anomalously enhanced photoemission from the Dirac point and other peculiarities in the self-energy of the surface-state quasiparticles in Bi2Se3 |
Q62383008 | Bridging Charge-Orbital Ordering and Fermi Surface Instabilities in Half-Doped Single-Layered ManganiteLa0.5Sr1.5MnO4 |
Q62680280 | Circular dichroism and bilayer splitting in the normal state of underdoped(Pb,Bi)2Sr2(CaxY1−x)Cu2O8+δand overdoped(Pb,Bi)2Sr2CaCu2O8+δ |
Q49256776 | Circular dichroism in angle-resolved photoemission spectra of under- and overdoped Pb-Bi2212. |
Q62383218 | Constituents of the Quasiparticle Spectrum Along the Nodal Direction of High-TcCuprates |
Q62382895 | Conventional superconductivity in SrPd2Ge2 |
Q62382779 | Crystal growth and electronic phase diagram of4d−dopedNa1−δFe1−xRhxAsin comparison to3d−dopedNa1−δFe1−xCoxAs |
Q62383221 | Current spinon-holon description of the one-dimensional charge-transfer insulatorSrCuO2: Angle-resolved photoemission measurements |
Q62644649 | Direct observation of the spin texture in SmB6 as evidence of the topological Kondo insulator |
Q27355455 | Doping dependence of the Fermi surface in ( B i , P b ) 2 Sr 2 CaCu 2 O 8 + δ |
Q79283529 | Doping dependence of the mass enhancement in (Pb,Bi)2Sr2CaCu2O8 at the antinodal point in the superconducting and normal states |
Q62383226 | Effect of Zn and Ni Impurities on the Quasiparticle Renormalization of Superconducting Bi-2212 |
Q37405763 | Effect of nematic ordering on electronic structure of FeSe |
Q62382855 | Electronic Band Structure of Ferro-Pnictide Superconductors from ARPES Experiment |
Q62382898 | Electronic Confinement and Ordering Instabilities in Colossal Magnetoresistive Bilayer Manganites |
Q62383096 | Electronic Structure and Nesting-Driven Enhancement of the RKKY Interaction at the Magnetic Ordering Propagation Vector inGd2PdSi3andTb2PdSi3 |
Q59348534 | Electronic Structure of the Dark Surface of the Weak Topological Insulator Bi14Rh3I9 |
Q62382856 | Electronic band structure and momentum dependence of the superconducting gap in Ca1−xNaxFe2As2from angle-resolved photoemission spectroscopy |
Q62382782 | Electronic structure of (Ca0.85La0.15)FeAs2 |
Q62383098 | Electronic structure ofCeCoIn5from angle-resolved photoemission spectroscopy |
Q62383101 | Electronic structure ofPr2−xCexCuO4studied via ARPES andLDA+DMFT+Σk |
Q62383022 | Electrons in cuprates: A consistent ARPES view |
Q62383106 | Erratum: Excitation energy map of high-energy dispersion anomalies in cuprates [Phys. Rev. B77, 212504 (2008)] |
Q61987275 | Evidence against a charge density wave on Bi(111) |
Q62567759 | Evidence for CuO conducting band splitting in the nodal direction ofBi2Sr2CaCu2O8+δ |
Q62383102 | Evidence for Fermi surface reconstruction in the static stripe phase of La1.8-xEu0.2SrxCuO4, x=1/8 |
Q62383158 | Excitation energy map of high-energy dispersion anomalies in cuprates |
Q53491498 | Experimental realization of a three-dimensional Dirac semimetal. |
Q59348519 | Experimental realization of type-II Weyl state in noncentrosymmetric TaIrTe4 |
Q62383162 | Fermi surface nesting in several transition metal dichalcogenides |
Q57987245 | Fermi surface of Ba1−xKxFe2As2 as probed by angle-resolved photoemission |
Q63484886 | High-energy electronic interaction in the 3d band of high-temperature iron-based superconductors |
Q36382299 | High-temperature superconductivity from fine-tuning of Fermi-surface singularities in iron oxypnictides |
Q62382904 | Hole doping in BaFe2As2: The case of Ba1−xNaxFe2As2single crystals |
Q62383167 | Hybridization effects inCeCoIn5observed by angle-resolved photoemission |
Q62382905 | Incommensurate magnetic fluctuations and Fermi surface topology in LiFeAs |
Q35635341 | Interaction-induced singular Fermi surface in a high-temperature oxypnictide superconductor |
Q62382789 | Isotropic multi-gap superconductivity in BaFe1.9Pt0.1As2from thermal transport and spectroscopic measurements |
Q74320786 | Joys and pitfalls of fermi surface mapping in Bi(2)Sr(2)CaCu(2)O(8+delta) using angle resolved photoemission |
Q62383254 | Kinks, Nodal Bilayer Splitting, and Interband Scattering inYBa2Cu3O6+x |
Q62383257 | Life of the nodal quasiparticles in Bi-2212 as seen by ARPES |
Q62383391 | Manifestation of the Magnetic Resonance Mode in the Nodal Quasiparticle Lifetime of the Superconducting Cuprates |
Q27440516 | Measuring the gap in angle-resolved photoemission experiments on cuprates |
Q80589764 | Momentum and energy dependence of the anomalous high-energy dispersion in the electronic structure of high temperature superconductors |
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 |
Q62382795 | Non-Fermi-liquid scattering rates and anomalous band dispersion in ferropnictides |
Q57987249 | Nonmonotonic pseudogap in high-Tccuprates |
Q57987239 | Observation of the Fermi surface, the band structure, and their diffraction replicas ofSr14−xCaxCu24O41by angle-resolved photoemission spectroscopy |
Q89010904 | Observation of the weak electronic correlations in KFeCoAs2 (3d 6): an isoelectronic to the parent compounds of 122 series of iron pnictides BaFe2As2 |
Q62382916 | One-Sign Order Parameter in Iron Based Superconductor |
Q62382797 | Orbital characters and electronic correlations in KCo2Se2 |
Q74639689 | Origin of the peak-dip-hump line shape in the superconducting-state (pi,0) photoemission spectra of Bi2Sr2CaCu2O8 |
Q62567769 | Origin of the shadow Fermi surface inBi-based cuprates |
Q62383286 | Parity of the Pairing Bosons in a High-TemperaturePb−Bi2Sr2CaCu2O8Bilayer Superconductor by Angle-Resolved Photoemission Spectroscopy |
Q61728053 | Photoemission and muon spin relaxation spectroscopy of the iron-based Rb0.77Fe1.61Se2superconductor: Crucial role of the cigar-shaped Fermi surface |
Q62382972 | Photoemission-induced gating of topological insulators |
Q62382974 | Propeller-Like Low Temperature Fermi Surface of Ba1-xKxFe2As2from Magnetotransport and Photoemission Measurements |
Q27350022 | Pseudogap and Charge Density Waves in Two Dimensions |
Q62382923 | Pseudogap in the chain states of YBa2Cu3O6.6 |
Q51872534 | Pseudogap-driven sign reversal of the Hall effect. |
Q62567677 | Quantitative comparison of single- and two-particle properties in the cuprates |
Q40276837 | Quasi one dimensional Dirac electrons on the surface of Ru₂Sn₃. |
Q62383182 | Relation between the one-particle spectral function and dynamic spin susceptibility of superconductingBi2Sr2CaCu2O8−δ |
Q60243189 | Renormalized band structure of Sr2RuO4: A quasiparticle tight-binding approach |
Q62382979 | Resistivity and Hall effect of LiFeAs: Evidence for electron-electron scattering |
Q62383068 | Single Crystal Growth and Characterization of Superconducting LiFeAs |
Q62382991 | Specific heat and angle-resolved photoemission spectroscopy study of the superconducting gaps in LiFeAs |
Q44415706 | Stacked topological insulator built from bismuth-based graphene sheet analogues |
Q62383135 | Strength of the spin-fluctuation-mediated pairing interaction in a high-temperature superconductor |
Q62383297 | Stripe Correlations inNa0.75CoO2 |
Q57987193 | Strong electron pairing at the iron 3dxz,yzorbitals in hole-doped BaFe2As2superconductors revealed by angle-resolved photoemission spectroscopy |
Q62382881 | Superconducting gap in LiFeAs from three-dimensional spin-fluctuation pairing calculations |
Q62382837 | Superconductivity from repulsion in LiFeAs: Novels-wave symmetry and potential time-reversal symmetry breaking |
Q62383074 | Superconductivity without Nesting in LiFeAs |
Q86854308 | Superconductivity: Fewer atoms, more information |
Q80523885 | Superconductors: time-reversal symmetry breaking? |
Q62382994 | Suppressed superconductivity in charge-doped Li(Fe1−xCox)As single crystals |
Q60243200 | Surface and bulk electronic structure of the unconventional superconductor Sr2RuO4: unusual splitting of theβband |
Q59348560 | TaIrTe4: A ternary type-II Weyl semimetal |
Q57987252 | Temperature and Doping-Dependent Renormalization Effects of the Low Energy Electronic Structure ofBa1−xKxFe2As2Single Crystals |
Q62383139 | Temperature-dependent Fermi surface of2H-TaSe2driven by competing density wave order fluctuations |
Q92321615 | Time-reversal symmetry breaking type-II Weyl state in YbMnBi2 |
Q57987253 | Two Energy Gaps and Fermi-Surface “Arcs” inNbSe2 |
Q62383315 | Unadulterated spectral function of low-energy quasiparticles inBi2Sr2CaCu2O8+δ |
Q62382841 | Unusual band renormalization in the simplest iron-based superconductorFeSe1−x |
Q62383001 | Van Hove singularity as a possible origin of the bandwidth renormalization in layered superconductors |
Q63957533 | Weak Superconducting Pairing and a Single Isotropic Energy Gap in Stoichiometric LiFeAs |
Q36427963 | Weak-coupling superconductivity in a strongly correlated iron pnictide |
Q62382935 | Weak-coupling superconductivity in electron-doped NaFe0.95Co0.05As revealed by ARPES |
Q62382885 | WhyTcof (CaFeAs)10Pt3.58As8is twice as high as (CaFe0.95Pt0.05As)10Pt3As8 |
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