| 1 | Gapless superconductivity from low-frequency electrodynamic response of two-dimensional granular composites | 2.5 | 2 | Citations (PDF) |
| 2 | Possible unconventional surface superconductivity in the half-Heusler compound YPtBi | 2.5 | 4 | Citations (PDF) |
| 3 | Spin-glass state in nickelate superconductors | 4.4 | 4 | Citations (PDF) |
| 4 | Vortex phase diagram of the kagome superconductor
CsV3Sb5 | 2.5 | 3 | Citations (PDF) |
| 5 | Thermal transport measurements through the charge density wave transition in
<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mi>CsV</mml:mi><mml:mn>3</mml:mn></mml:msub><mml:msub><mml:mi>Sb</mml:mi><mml:mn>5</mml:mn></mml:msub></mml:mrow></mml:math> | 2.5 | 3 | Citations (PDF) |
| 6 | Emergent tetragonality in a fundamentally orthorhombic material | 8.2 | 15 | Citations (PDF) |
| 7 | Nanoscale phase-slip domain walls in the charge density wave state of the Weyl semimetal candidate
NbTe4 | 2.5 | 13 | Citations (PDF) |
| 8 | Impact of disorder in the charge density wave state of Pd-intercalated
ErTe3
revealed by the electrodynamic response | 2.5 | 2 | Citations (PDF) |
| 9 | Emergent
Z2
symmetry near a charge density wave multicritical point | 2.5 | 6 | Citations (PDF) |
| 10 | Interplay between magnetism and superconductivity in
UTe2 | 2.5 | 44 | Citations (PDF) |
| 11 | Superconductor–insulator transitions in three-dimensional indium-oxide at high pressures | 1.6 | 2 | Citations (PDF) |
| 12 | Characterization of magnetic field noise in the ARIADNE source mass rotor | 2.5 | 14 | Citations (PDF) |
| 13 | Observation of broken inversion and chiral symmetries in the pseudogap phase in single- and double-layer bismuth-based cuprates | 2.5 | 8 | Citations (PDF) |
| 14 | Anomalous metals: From “failed superconductor” to “failed insulator” | 5.3 | 21 | Citations (PDF) |
| 15 | Universal Bound to the Amplitude of the Vortex Nernst Signal in Superconductors | 5.8 | 17 | Citations (PDF) |
| 16 | Robust anomalous metallic states and vestiges of self-duality in two-dimensional granular In-InOx composites | 4.4 | 15 | Citations (PDF) |
| 17 | Nanoscale Turing patterns in a bismuth monolayer | 10.8 | 76 | Citations (PDF) |
| 18 | Superconductor–insulator transition in two-dimensional indium–indium-oxide composite | 5.3 | 14 | Citations (PDF) |
| 19 | Emergence of ferromagnetism through the metal-insulator transition in undoped indium tin oxide films | 1.8 | 3 | Citations (PDF) |
| 20 | Anomalous thermal transport and strong violation of Wiedemann-Franz law in the critical regime of a charge density wave transition | 2.5 | 9 | Citations (PDF) |
| 21 | A cantilever torque magnetometry method for the measurement of Hall conductivity of highly resistive samples | 1.1 | 8 | Citations (PDF) |
| 22 | Robust superconductivity intertwined with charge density wave and disorder in Pd-intercalated
ErTe3 | 2.5 | 16 | Citations (PDF) |
| 23 | Sample shape and boundary dependence of measured transverse thermal properties | 1.6 | 2 | Citations (PDF) |
| 24 | Thermalization and possible signatures of quantum chaos in complex crystalline materials | 5.3 | 23 | Citations (PDF) |
| 25 | Colloquium
: Anomalous metals: Failed superconductors | 29.4 | 199 | Citations (PDF) |
| 26 | A lower bound to the thermal diffusivity of insulators | 1.6 | 32 | Citations (PDF) |
| 27 | Disorder-induced suppression of charge density wave order: STM study of Pd-intercalated
ErTe3 | 2.5 | 34 | Citations (PDF) |
| 28 | Thermal diffusivity above the Mott-Ioffe-Regel limit | 2.5 | 27 | Citations (PDF) |
| 29 | Bursting at the seams: Rippled monolayer bismuth on NbSe
2 | 8.2 | 42 | Citations (PDF) |
| 30 | Polar Kerr Effect from Time-Reversal Symmetry Breaking in the Heavy-Fermion Superconductor
PrOs4Sb12 | 5.8 | 26 | Citations (PDF) |
| 31 | Temperature-induced inversion of the spin-photogalvanic effect in
WTe2
and
MoTe2 | 2.5 | 31 | Citations (PDF) |
| 32 | Two-stage proximity-induced gap opening in topological-insulator–insulating-ferromagnet
(BixSb1−x)2Te3
–
EuS
bilayers | 2.5 | 10 | Citations (PDF) |
| 33 | Polar Kerr effect studies of time reversal symmetry breaking states in heavy fermion superconductors | 0.9 | 8 | Citations (PDF) |
| 34 | Disorder enabled band structure engineering of a topological insulator surface | 11.0 | 41 | Citations (PDF) |
| 35 | Anomalous thermal diffusivity in underdoped YBa
2
Cu
3
O
6+x | 5.3 | 82 | Citations (PDF) |
| 36 | Particle-hole symmetry reveals failed superconductivity in the metallic phase of two-dimensional superconducting films | 8.2 | 63 | Citations (PDF) |
| 37 | Superconductor to weak-insulator transitions in disordered tantalum nitride films | 2.5 | 23 | Citations (PDF) |
| 38 | Self-duality and a Hall-insulator phase near the superconductor-to-insulator transition in indium-oxide films | 5.3 | 42 | Citations (PDF) |
| 39 | Evidence for broken time-reversal symmetry in the superconducting phase ofURu2Si2 | 2.5 | 116 | Citations (PDF) |
| 40 | Notes on constraints for the observation of Polar Kerr Effect in complex materials | 2.2 | 17 | Citations (PDF) |
| 41 | A scanning, all-fiber Sagnac interferometer for high resolution magneto-optic measurements at 820 nm | 1.1 | 21 | Citations (PDF) |
| 42 | Pulsed laser deposition of high-quality thin films of the insulating ferromagnet EuS | 2.4 | 14 | Citations (PDF) |
| 43 | Evidence of Chiral Order in the Charge-Ordered Phase of SuperconductingLa1.875Ba0.125Cuo4Single Crystals Using Polar Kerr-Effect Measurements | 5.8 | 49 | Citations (PDF) |
| 44 | Emerging weak localization effects on a topological insulator–insulating ferromagnet (Bi2Se3-EuS) interface | 2.5 | 122 | Citations (PDF) |
| 45 | Kerr effect as evidence of gyrotropic order in the cuprates | 2.5 | 71 | Citations (PDF) |
| 46 | Observation of the ghost critical field for superconducting fluctuations in a disordered TaN thin film | 2.5 | 20 | Citations (PDF) |
| 47 | Weak localization effects as evidence for bulk quantization in Bi2Se3thin films | 2.5 | 50 | Citations (PDF) |
| 48 | High quality ultrathin Bi2Se3 films on CaF2 and CaF2/Si by molecular beam epitaxy with a radio frequency cracker cell | 2.4 | 27 | Citations (PDF) |
| 49 | Magneto-Optical Measurements of a Cascade of Transitions in SuperconductingLa1.875Ba0.125CuO4Single Crystals | 5.8 | 48 | Citations (PDF) |
| 50 | Hall conductivity dominated by fluctuations near the superconducting transition in disordered thin films | 2.5 | 27 | Citations (PDF) |
| 51 | Charge and spin collective modes in a quasi-one-dimensional model of Sr2RuO4 | 2.5 | 32 | Citations (PDF) |
| 52 | Weak antilocalization and disorder-enhanced electron interactions in annealed films of the phase-change compound GeSb2Te4 | 2.5 | 70 | Citations (PDF) |
| 53 | STM Imaging of Impurity Resonances onBi2Se3 | 5.8 | 96 | Citations (PDF) |
| 54 | Thin-film synthesis of the high-Tc oxide superconductor YBa2Cu3O7 by electron-beam codeposition | 1.9 | 28 | Citations (PDF) |
| 55 | Microstructure and Properties of Mixed Yba2Cu3O7-X and Y2Ba4Cu8O16 Thin Films | 0.1 | 0 | Citations (PDF) |
| 56 | Microstructural interaction of Y2Ba4Cu8O16 stacking faults within YBa2Cu3O7−x | 1.9 | 9 | Citations (PDF) |
| 57 | STM imaging of a bound state along a step on the surface of the topological insulator Bi2Te3 | 2.5 | 40 | Citations (PDF) |
| 58 | Hidden Quasi-One-Dimensional Superconductivity inSr2RuO4 | 5.8 | 181 | Citations (PDF) |
| 59 | STM Imaging of Electronic Waves on the Surface ofBi2Te3: Topologically Protected Surface States and Hexagonal Warping Effects | 5.8 | 507 | Citations (PDF) |
| 60 | Critical thickness for itinerant ferromagnetism in ultrathin films ofSrRuO3 | 2.5 | 194 | Citations (PDF) |
| 61 | Inverse Proximity Effect in Superconductor-Ferromagnet Bilayer Structures | 5.8 | 100 | Citations (PDF) |
| 62 | Search for time-reversal symmetry breaking in unconventional superconductors | 2.2 | 2 | Citations (PDF) |
| 63 | Polar Kerr effect as probe for time-reversal symmetry breaking in unconventional superconductors | 1.9 | 144 | Citations (PDF) |
| 64 | Polar Kerr-Effect Measurements of the High-TemperatureYBa2Cu3O6+xSuperconductor: Evidence for Broken Symmetry near the Pseudogap Temperature | 5.8 | 362 | Citations (PDF) |
| 65 | New apparatus for detecting micron-scale deviations from Newtonian gravity | 3.5 | 26 | Citations (PDF) |
| 66 | Improved constraints on non-Newtonian forces at 10 microns | 3.5 | 197 | Citations (PDF) |
| 67 | Preparation and properties of amorphousMgB2∕MgOsuperstructures: Model disordered superconductor | 2.5 | 5 | Citations (PDF) |
| 68 | Approach to a superconductor-to-Bose-insulator transition in disordered films | 2.5 | 101 | Citations (PDF) |
| 69 | STM Studies ofTbTe3: Evidence for a Fully Incommensurate Charge Density Wave | 5.8 | 81 | Citations (PDF) |
| 70 | High Resolution Polar Kerr Effect Measurements ofSr2RuO4: Evidence for Broken Time-Reversal Symmetry in the Superconducting State | 5.8 | 552 | Citations (PDF) |
| 71 | Modified Sagnac interferometer for high-sensitivity magneto-optic measurements at cryogenic temperatures | 2.4 | 91 | Citations (PDF) |
| 72 | STM studies of near-optimal doped Bi2Sr2CaCu2O8+δ | 4.2 | 11 | Citations (PDF) |
| 73 | Feedback control and characterization of a microcantilever using optical radiation pressure | 2.4 | 37 | Citations (PDF) |
| 74 | Inferring effective interactions from the local density of states: Application to STM data fromBi2Sr2CaCu2O8+δ | 2.5 | 7 | Citations (PDF) |
| 75 | Gap-Inhomogeneity-Induced Electronic States in SuperconductingBi2Sr2CaCu2O8+δ | 5.8 | 102 | Citations (PDF) |
| 76 | Distinguishing patterns of charge order: Stripes or checkerboards | 2.5 | 119 | Citations (PDF) |
| 77 | Superconductivity in the insulating phase above the field-tuned superconductor–insulator transition in disordered indium oxide films | 0.9 | 98 | Citations (PDF) |
| 78 | Possible Field-Tuned Superconductor-Insulator Transition in High-TcSuperconductors: Implications for Pairing at High Magnetic Fields | 5.8 | 90 | Citations (PDF) |
| 79 | Constraints on Yukawa-type deviations from Newtonian gravity at 20 microns | 3.5 | 107 | Citations (PDF) |
| 80 | Periodic coherence-peak height modulations in superconductingBi2Sr2CaCu2O8+δ | 2.5 | 61 | Citations (PDF) |
| 81 | Periodic density-of-states modulations in superconductingBi2Sr2CaCu2O8+δ | 2.5 | 314 | Citations (PDF) |
| 82 | How to detect fluctuating stripes in the high-temperature superconductors | 29.4 | 1,293 | Citations (PDF) |
| 83 | Coexistence of periodic modulation of quasiparticle states and superconductivity in Bi2Sr2CaCu2O8+ | 5.3 | 106 | Citations (PDF) |
| 84 | New Experimental Constraints on Non-Newtonian Forces below100 μm | 5.8 | 215 | Citations (PDF) |
| 85 | Superconductor-insulator transition in a capacitively coupled dissipative environment | 2.5 | 45 | Citations (PDF) |
| 86 | Bulk magnetic properties and phase diagram of Li-dopedLa2CuO4:Common magnetic response of hole-dopedCuO2planes | 2.5 | 18 | Citations (PDF) |
| 87 | Simple microcalorimeter for measuring microgram samples at low temperatures | 1.1 | 14 | Citations (PDF) |
| 88 | Domain-wall resistivity in SrRuO3: the influence of domain walls spacing | 2.1 | 4 | Citations (PDF) |
| 89 | Negative deviations from Matthiessen's rule for SrRuO
3
and CaRuO
3 | 1.4 | 12 | Citations (PDF) |
| 90 | Inherent inhomogeneities in tunneling spectra ofBi2Sr2CaCu2O8−xcrystals in the superconducting state | 2.5 | 240 | Citations (PDF) |
| 91 | Microcantilever studies of angular field dependence of vortex dynamics inBi2Sr2CaCu2O8−x | 2.5 | 4 | Citations (PDF) |
| 92 | Effects of dissipation on quantum phase transitions | 2.5 | 99 | Citations (PDF) |
| 93 | True superconductivity in a two-dimensional superconducting-insulating system | 2.5 | 70 | Citations (PDF) |
| 94 | Thermal conductivity of pure and Mg-dopedCuGeO3in the incommensurate phase | 2.5 | 18 | Citations (PDF) |
| 95 | Magnetic resistivity inSrRuO3and the ferromagnetic phase transition | 2.5 | 38 | Citations (PDF) |
| 96 | Extraordinary Hall effect in SrRuO3 | 2.2 | 5 | Citations (PDF) |
| 97 | Thermal conductivity of Cu1−xMgxGeO3 | 2.2 | 3 | Citations (PDF) |
| 98 | Extraordinary Hall effect inSrRuO3 | 2.5 | 50 | Citations (PDF) |
| 99 | Temperature- and magnetic-field-dependent thermal conductivity of pure and Zn-dopedBi2Sr2CaCu2O8+δsingle crystals | 2.5 | 49 | Citations (PDF) |
| 100 | Kleinet al.Reply: | 5.8 | 7 | Citations (PDF) |
| 101 | Specific heat of Zn-dopedYBa2Cu3O6.95:Possible evidence for Kondo screening in the superconducting state | 2.5 | 34 | Citations (PDF) |
| 102 | Magnetization and resistivity measurements of the first-order vortex phase transition in(La1−xSrx)2CuO4 | 2.5 | 47 | Citations (PDF) |
| 103 | Domain Wall Resistivity inSrRuO3 | 5.8 | 89 | Citations (PDF) |
| 104 | Impurity-Induced Bound Excitations on the Surface ofBi2Sr2CaCu2O8 | 5.8 | 171 | Citations (PDF) |
| 105 | Temperature-dependent local exchange splitting inSrRuO3 | 2.5 | 39 | Citations (PDF) |
| 106 | Dissipation Effects on the Superconductor-Insulator Transition in 2D Superconductors | 5.8 | 207 | Citations (PDF) |
| 107 | Lorentz transmission electron microscope study of ferromagnetic domain walls in SrRuO3: Statics, dynamics, and crystal structure correlation | 1.6 | 88 | Citations (PDF) |
| 108 | Is CaRuO3 a non-Fermi liquid metal? | 2.2 | 14 | Citations (PDF) |
| 109 | Title is missing! | 0.7 | 3 | Citations (PDF) |
| 110 | Possible non-Fermi-liquid behavior ofCaRuO3 | 2.5 | 110 | Citations (PDF) |
| 111 | Large magnetoresistance of single-crystal films of ferromagnetic SrRuO3 | 2.1 | 24 | Citations (PDF) |
| 112 | Non-Fermi-Liquid Behavior ofSrRuO3: Evidence from Infrared Conductivity | 5.8 | 216 | Citations (PDF) |
| 113 | Observation of quantum oscillations in the electrical resistivity ofSrRuO3 | 2.5 | 98 | Citations (PDF) |
| 114 | Transport through Quantum Melts | 5.8 | 146 | Citations (PDF) |
| 115 | Thermal conductivity of the spin-Peierls compoundCuGeO3 | 2.5 | 80 | Citations (PDF) |
| 116 | Current-induced ordering of vortices in two-dimensional amorphousMo77Ge23films as a function of film thickness and magnetic field | 2.5 | 11 | Citations (PDF) |
| 117 | Magnetic and Crystalline Microstructure of SrRuO 3 Thin Films | 0.1 | 3 | Citations (PDF) |
| 118 | Temperature and doping dependence of the Bi-Sr-Ca-Cu-O electronic structure and fluctuation effects | 2.5 | 62 | Citations (PDF) |
| 119 | Specific heat ofYBa2Cu3O7−δ | 2.5 | 164 | Citations (PDF) |
| 120 | Unconventional Electronic Structure Evolution with Hole Doping inBi2Sr2CaCu2O8+δ: Angle-Resolved Photoemission Results | 5.8 | 607 | Citations (PDF) |
| 121 | Evolution of the Pseudogap State of High-TcSuperconductors with Doping | 5.8 | 143 | Citations (PDF) |
| 122 | Transport and magnetization in the badly metallic itinerant ferromagnet | 1.6 | 182 | Citations (PDF) |
| 123 | Field-DrivenTopologicalGlass Transition in a Model Flux Line Lattice | 5.8 | 70 | Citations (PDF) |
| 124 | Vortex Dynamics in Two-Dimensional Amorphous Mo77Ge23Films | 5.8 | 128 | Citations (PDF) |
| 125 | Anomalous Spin Scattering Effects in the Badly Metallic Itinerant FerromagnetSrRuO3 | 5.8 | 299 | Citations (PDF) |
| 126 | Lock-in transition in Bi2Sr2CaCu2O8+δ observed through 10GHz dissipation | 0.4 | 2 | Citations (PDF) |
| 127 | Growth and annealing of (Bi1−xPbx)2Sr2CaCu2O8+δ single crystals | 0.9 | 17 | Citations (PDF) |
| 128 | Proximity junctions on Bi2Sr2CaCu2O8 single crystals | 0.9 | 23 | Citations (PDF) |
| 129 | Evolution of the electronic structure with doping in Bi2Sr2CaCu2O8+δ - Angle resolved photoemission results | 1.5 | 3 | Citations (PDF) |
| 130 | Vortex Dynamics in Two-Dimensional AmorphousMo77Ge23Films | 5.8 | 3 | Citations (PDF) |
| 131 | Dynamical Phase Transition in a Driven Disordered Vortex Lattice | 5.8 | 136 | Citations (PDF) |
| 132 | Observation of Quantum Dissipation in the Vortex State of a Highly Disordered Superconducting Thin Film | 5.8 | 193 | Citations (PDF) |
| 133 | Rapid suppression of the superconducting gap in overdopedBi2Sr2CaCu2O8+δ | 2.5 | 36 | Citations (PDF) |
| 134 | Magnetization jumps and irreversibility inBi2Sr2CaCu2O8 | 2.5 | 50 | Citations (PDF) |
| 135 | Symmetry of the magneto-optic response of the Sagnac interferometer | 1.6 | 15 | Citations (PDF) |
| 136 | Analysis of the lock-in transition inBi2Sr2CaCu2O8+δsingle crystals through microwave dissipation | 2.5 | 27 | Citations (PDF) |
| 137 | Magnetic field dependence of the density of states of YBa2Cu3O6.95: Implications for the vortex structure | 0.0 | 4 | Citations (PDF) |
| 138 | Proposed thermodynamic method to determine the vortex mass in layered superconductors | 0.7 | 10 | Citations (PDF) |
| 139 | Specific heat of YBa2Cu3O7 − δ single crystals: Implications for the vortex structure | 4.2 | 10 | Citations (PDF) |
| 140 | Irreversible properties of micrometer-thick, superconducting MoGe/Ge multilayers as a function of anisotropy | 2.5 | 2 | Citations (PDF) |
| 141 | Superconducting-Insulating Transition in Two-Dimensionala-MoGe Thin Films | 5.8 | 354 | Citations (PDF) |
| 142 | Perpendicular magnetic anisotropy and strong magneto‐optic properties of SrRuO3 epitaxial films | 2.4 | 114 | Citations (PDF) |
| 143 | Correlation of Vortex Motion in High-TcSuperconductors | 5.8 | 12 | Citations (PDF) |
| 144 | HIGH RESOLUTION MAGNETO-OPTICS USING THE SAGNAC EFFECT | 0.3 | 0 | Citations (PDF) |
| 145 | Magneto-optic measurements with a sagnac interferometer | 0.5 | 9 | Citations (PDF) |
| 146 | Dynamic characteristics of the anomalous second peak in the magnetization curves of Bi-Sr-Ca-Cu-O | 2.5 | 154 | Citations (PDF) |
| 147 | Competition between pinning and melting in the two-dimensional vortex lattice | 2.5 | 12 | Citations (PDF) |
| 148 | Thermally assisted vortex motion in coupled two-dimensional superconductors | 2.5 | 9 | Citations (PDF) |
| 149 | Angular dependence of the critical currents inMo77Ge23/Ge multilayers | 2.5 | 12 | Citations (PDF) |
| 150 | Vortex lattice melting, pinning and kinetics | 0.7 | 8 | Citations (PDF) |
| 151 | Studies of two-dimensional MoGe superconductors in a magnetic field | 2.2 | 8 | Citations (PDF) |
| 152 | Spatially resolved vacuum tunneling spectroscopy on Bi2Sr2CaCu2O8 by STM at 4.8K | 2.2 | 17 | Citations (PDF) |
| 153 | Hc2 of Y1Ba2Cu3O7-δ thin films from conductivity fluctuations | 2.2 | 1 | Citations (PDF) |
| 154 | Evidence for the quasi-two dimensional behavior of the vortex structure in Bi2Sr2CaCu2O8 single crystals | 2.2 | 0 | Citations (PDF) |
| 155 | Resistive and thermodynamic transitions of a two-dimensional superconductor in a magnetic field | 0.9 | 4 | Citations (PDF) |
| 156 | Deoxygenation and oxygen annealing of Bi2Sr2CaCu2O8+δ single observed in situ by 17O NMR | 0.9 | 2 | Citations (PDF) |
| 157 | Vortex decoupling crossover in Bi2Sr2CaCu2O8 | 0.9 | 33 | Citations (PDF) |
| 158 | Microwave absorption in the mixed state of Bi2Sr2CaCu2Oδ+gd single crystals | 0.9 | 3 | Citations (PDF) |
| 159 | Magnetic field dependence of the electronic specific heat in YBa2Cu3O6.95 single crystals | 0.9 | 2 | Citations (PDF) |
| 160 | Normal modes and specific heat of an undamped three-dimensional lattice of pancake vortices in thin superconducting multilayers | 0.9 | 1 | Citations (PDF) |
| 161 | Angular dependence of the critical currents in magnetic fields of superconducting/insulating Mo77Ge23/Ge multilayers | 0.9 | 0 | Citations (PDF) |
| 162 | Anomalous temperature dependence of vortex elastic properties in the flux-flow regime ofMo77Ge23/Ge multilayer superconductors | 2.5 | 15 | Citations (PDF) |
| 163 | Magnetic Field Dependence of the Density of States of YBa2Cu3O6.95as Determined from the Specific Heat | 5.8 | 347 | Citations (PDF) |
| 164 | High‐resolution magneto‐optic measurements with a Sagnac interferometer (invited) | 1.6 | 44 | Citations (PDF) |
| 165 | Thermal diffusivity of Bi2Sr2CaCu2O8 single crystals | 0.9 | 9 | Citations (PDF) |
| 166 | Photothermal microscope for high‐Tc superconductors and charge density waves | 1.1 | 16 | Citations (PDF) |
| 167 | Anomalously large gap anisotropy in thea-bplane ofBi2Sr2CaCu2O8+δ | 5.8 | 874 | Citations (PDF) |
| 168 | Search for characteristic lengthscales of the magnetic field distribution at the surface of superconducting Bi2Sr2CaCu2O8+δ single crystals | 4.9 | 2 | Citations (PDF) |
| 169 | Vortex-antivortex crystallization in thin superconducting and superfluid films | 5.8 | 59 | Citations (PDF) |
| 170 | Observation of Kosterlitz-Thouless-type melting of the disordered vortex lattice in thin films ofa-MoGe | 5.8 | 48 | Citations (PDF) |
| 171 | Effects of columnar pins on flux line dynamics | 5.8 | 11 | Citations (PDF) |
| 172 | Collective vortex motion ina-MoGe superconducting thin films | 5.8 | 58 | Citations (PDF) |
| 173 | Key features in the measured band structure ofBi2Sr2CaCu2O8+δ: Flat bands atEFand Fermi surface nesting | 5.8 | 497 | Citations (PDF) |
| 174 | Microwave penetration depth measurements onBi2Sr2CaCu2O8single crystals andYBa2Cu3O7−δthin films | 5.8 | 142 | Citations (PDF) |
| 175 | Loss of interplane correlation inBi2Sr2CaCu2O8single crystals | 2.5 | 17 | Citations (PDF) |
| 176 | High Energy Resolution Arpes Measurements of the Normal and Superconducting States of Bi2Sr2CaCu2O8+δ | 0.1 | 1 | Citations (PDF) |
| 177 | Superconducting interlayer decoupling and softening of the flux line structure in BSCCO single crystals | 2.4 | 6 | Citations (PDF) |
| 178 | Two-step transition towards the reversibility region inBi2Sr2CaCu2O8−δsingle crystals | 2.5 | 18 | Citations (PDF) |
| 179 | Measurement of the spontaneous polar Kerr effect inYBa2Cu3O7andBi2Sr2CaCu2O8 | 5.8 | 59 | Citations (PDF) |
| 180 | Nature of the high-binding-energy dip in the low-temperature photoemission spectra ofBi2Sr2CaCu2O8+δ | 2.5 | 32 | Citations (PDF) |
| 181 | Thermoelectric cooling at very low temperatures | 2.4 | 15 | Citations (PDF) |
| 182 | Test for nonreciprocal circular birefringence inBi2Sr2CaCu2O8 | 2.5 | 23 | Citations (PDF) |
| 183 | Specific heat of a superconducting multilayer: 2D fluctuations and 2D-0D crossover | 5.8 | 24 | Citations (PDF) |
| 184 | In situ growth of YBa2Cu3Ox thin films by reactive cosputtering | 1.5 | 6 | Citations (PDF) |
| 185 | Ca 3dunoccupied states inBi2Sr2CaCu2O8investigated by CaL2,3x-ray-absorption near-edge structure | 2.5 | 14 | Citations (PDF) |
| 186 | Superconducting transition, fluctuation, and vortex motion in a two-dimensional single-crystal Nb film | 2.5 | 77 | Citations (PDF) |
| 187 | Evidence fork-dependent, in-plane anisotropy of the superconducting gap inBi2Sr2CaCu2O8+δ | 2.5 | 72 | Citations (PDF) |
| 188 | Defect dependence of the irreversibility line inBi2Sr2CaCu2O8single crystals | 2.5 | 42 | Citations (PDF) |
| 189 | Optical tests for broken time-reversal symmetry in high-temperature superconductors | 1.7 | 0 | Citations (PDF) |
| 190 | SQUID picovoltometry of single crystalBi2Sr2CaCu2O8+δ: Observation of the crossover from high-temperature Arrhenius to low-temperature vortex-glass behavior | 5.8 | 179 | Citations (PDF) |
| 191 | Monte Carlo simulation of flux lattice melting in a model high-Tcsuperconductor | 5.8 | 160 | Citations (PDF) |
| 192 | Growth of Bi2Sr2CaCu2O8 single crystals using MgO crucibles | 1.7 | 37 | Citations (PDF) |
| 193 | Alteration in the superconducting properties of Bi/sub 2/Sr/sub 2/CaCu/sub 2/O/sub 8/ crystals due to proton irradiation | 1.6 | 4 | Citations (PDF) |
| 194 | O 1score levels inBi2Sr2CaCu2O8+δsingle crystals | 2.5 | 59 | Citations (PDF) |
| 195 | Observation of a commensurate array of flux chains in tilted flux lattices in Bi-Sr-Ca-Cu-O single crystals | 5.8 | 226 | Citations (PDF) |
| 196 | Observation of an hexatic vortex glass in flux lattices of the high-Tc superconductor Bi2.1Sr1.9Ca0.9Cu2O8+δ | 2.2 | 9 | Citations (PDF) |
| 197 | Inter- and intraplane softening of the vortex structure in Bi2.1Sr1.9Ca0.9Cu2O8+δ: a two-step transition | 0.9 | 38 | Citations (PDF) |
| 198 | Measurements of nonreciprocal optical effects on magnetic and superconducting materials using a fiber‐optic gyroscope (abstract) | 1.6 | 0 | Citations (PDF) |
| 199 | Enhancement of optical reflectivity of highTcsuperconducting films by ion milling | 2.4 | 0 | Citations (PDF) |
| 200 | Flux-lattice melting, anisotropy, and the role of interlayer coupling in Bi-Sr-Ca-Cu-O single crystals | 2.5 | 74 | Citations (PDF) |
| 201 | Superconducting transition temperature in a Nb/NbxSi1−xbilayer system | 2.5 | 10 | Citations (PDF) |
| 202 | Model system for vortex motion in coupled two-dimensional type-II superconductors | 5.8 | 73 | Citations (PDF) |
| 203 | Magnetic penetration depth and flux dynamics in single-crystalBi2Sr2CaCu2O8+δ | 5.8 | 65 | Citations (PDF) |
| 204 | In-plane dissipation maxima and vortex-line distortions in the resistive transitions of oxygen-doped Bi_{2}Sr_{2}CaCu_{2}O_{8+δ} single crystals | 5.8 | 22 | Citations (PDF) |
| 205 | The gold/high temperature superconductor interface; metallicity of the near surface region and a search for the proximity effect | 1.5 | 2 | Citations (PDF) |
| 206 | Search for a proximity effect induced gap in gold/highTcjunctions | 2.4 | 8 | Citations (PDF) |
| 207 | Translational and bond-orientational order in the vortex lattice of the high-TcsuperconductorBi2.1Sr1.9Ca0.9Cu2O8+δ | 5.8 | 117 | Citations (PDF) |
| 208 | Anomalous spectral weight transfer at the superconducting transition ofBi2Sr2CaCu2O8+δ | 5.8 | 252 | Citations (PDF) |
| 209 | Preparation of Optically Smooth Surfaces of High TcSuperconducting Films | 0.1 | 0 | Citations (PDF) |
| 210 | Percolative Properties of Al-Ge Composite thin Films | 0.1 | 0 | Citations (PDF) |
| 211 | Breakdown field in highly anisotropic superconductors | 2.1 | 26 | Citations (PDF) |
| 212 | Optical anisotropy ofBi2Sr2CaCu2O8 | 2.5 | 21 | Citations (PDF) |
| 213 | Test for nonreciprocal circular birefringence inYBa2Cu3O7thin films as evidence for broken time-reversal symmetry | 5.8 | 179 | Citations (PDF) |
| 214 | Angle-resolved-photoemission study ofBi2Sr2CaCu2O8+δ: Metallicity of the Bi-O plane | 5.8 | 141 | Citations (PDF) |
| 215 | Observation of a hexatic vortex glass in flux lattices of the high-TcsuperconductorBi2.1Sr1.9Ca0.9Cu2O8+δ | 5.8 | 156 | Citations (PDF) |
| 216 | Distribution of flux-pinning energies inYBa2Cu3O7−δandBi2Sr2CaCu2O8+δfrom flux noise | 5.8 | 130 | Citations (PDF) |
| 217 | Ferrariet al. reply | 5.8 | 1 | Citations (PDF) |
| 218 | Variation of Cu-O charge-transfer energies inYBa2Cu3O7−xthin films studied by photoemission spectroscopy | 2.5 | 28 | Citations (PDF) |
| 219 | Growth and properties of oxygen- and ion-dopedBi2Sr2CaCu2O8+δsingle crystals | 2.5 | 285 | Citations (PDF) |
| 220 | Flux motion in a two‐dimensional single‐crystal Nb film | 2.4 | 6 | Citations (PDF) |
| 221 | Interaction of overlayers of Al and Rb with single‐crystalline surfaces of Bi2Sr2CaCu2O8 | 1.6 | 7 | Citations (PDF) |
| 222 | Electronic structure of the gold/Bi2Sr2CaCu2O8and gold/EuBa2Cu3O7−δinterfaces as studied by photoemission spectroscopy | 2.4 | 24 | Citations (PDF) |
| 223 | Photoemission study of absorption mechanisms inBi2.0Sr1.8Ca0.8La0.3Cu2.1O8+δ,BaBiO3, andNd1.85Ce0.15CuO4 | 2.5 | 12 | Citations (PDF) |
| 224 | Photoelectron energy-loss study of theBi2CaSr2Cu2O8superconductor | 2.5 | 11 | Citations (PDF) |
| 225 | Energy dispersions of single-crystallineBi2.0Sr1.8Ca0.8La0.3Cu2.1O8+δsuperconductors determined using angle-resolved photoelectron spectroscopy | 2.5 | 8 | Citations (PDF) |
| 226 | Low-temperature specific heat of single-crystalBi2CaSr2Cu2O8andTl2Ca2Ba2Cu3O10 | 2.5 | 44 | Citations (PDF) |
| 227 | Valence-band states inBi2(Ca,Sr,La)3Cu2O8 | 2.5 | 24 | Citations (PDF) |
| 228 | Effect of electron-electron interaction on the thermoelectric power in disordered metallic systems | 2.5 | 18 | Citations (PDF) |
| 229 | Spectroscopic evidence of two‐dimensional character of the 90 K Bi2(Sr,La,Ca)3Cu2O8superconductors | 2.4 | 0 | Citations (PDF) |
| 230 | Electron tunneling and the energy gap inBi2Sr2CaCu2Ox | 2.5 | 101 | Citations (PDF) |
| 231 | Reaction of Rb and oxygen overlayers with single-crystallineBi2Sr2CaCu2O8+δsuperconductors | 2.5 | 59 | Citations (PDF) |
| 232 | Orthorhombic distortion and cation ordering inY2Ba4Cu8O16andEr2Ba4Cu8O16high-Tcthin films | 2.5 | 7 | Citations (PDF) |
| 233 | Resonance effects in Raman scattering in YBa2Cu3O7 | 1.6 | 25 | Citations (PDF) |
| 234 | Photothermal measurements of highTcsuperconductors | 2.4 | 34 | Citations (PDF) |
| 235 | Electronic structure of clean and Ag-covered single-crystallineBi2Sr2CuO6 | 2.5 | 10 | Citations (PDF) |
| 236 | Magnetic flux motion and its influence on transport properties of the high Tc oxide superconductors | 2.4 | 91 | Citations (PDF) |
| 237 | Symmetry of the oxygen hole states in Bi2Sr2CaCu2O8 investigated by XAS | 0.9 | 45 | Citations (PDF) |
| 238 | Electronic structure of the La1 + xBa2 − xCu3O7 + δ system studied by photoelectron spectroscopy | 2.0 | 9 | Citations (PDF) |
| 239 | Surface impedance studies of the high-T/sub c/ oxide superconductors | 1.0 | 25 | Citations (PDF) |
| 240 | Properties of high-T/sub c/ oxide fibers from laser heated pedestal growth | 1.0 | 2 | Citations (PDF) |
| 241 | In situ growth of superconducting YBaCuO using reactive electron-beam coevaporation | 1.0 | 77 | Citations (PDF) |
| 242 | Growth and properties of sputtered high-T/sub c/ oxide thin films | 1.0 | 24 | Citations (PDF) |
| 243 | Electronic structure of single crystalline Bi 2 (Sr,Ca,La) 3 Cu 2 O 8 | 0.9 | 2 | Citations (PDF) |
| 244 | Evidence for an intrinsic linear term in the T-dependence of the thermal conductivity of superconducting YBa 2 Cu 3 O 7 and Bi 2 Sr 2 CaCu 2 O 8 single crystals | 0.9 | 18 | Citations (PDF) |
| 245 | Orientation dependent resistive transition broadening in magnetic field of YBa 2 Cu 3 O 7−x thin films | 0.9 | 4 | Citations (PDF) |
| 246 | Vortex motion and time dependent magnetic responses in high T c superconductors | 0.9 | 19 | Citations (PDF) |
| 247 | The electronic structure of Bi2.0Sr1.8La0.3Ca0.8Cu2.1O8+δ superconductors studied using ultraviolet and X-ray photoelectron spectroscopy | 0.9 | 5 | Citations (PDF) |
| 248 | Photoemission study of the electronic structure (Pr0.2La0.8)(Ba1.875La0.125)Cu3O7−gd | 2.0 | 4 | Citations (PDF) |
| 249 | Systematic effects in thin film tunnel junctions of YBa2Cu3O7-δ | 2.0 | 36 | Citations (PDF) |
| 250 | Orthorhombic and tetragonal structures in the La(Ba2−yLay)Cu3O7−x system | 2.6 | 11 | Citations (PDF) |
| 251 | Measurements on thin-film high-Tc superconductors | 0.5 | 14 | Citations (PDF) |
| 252 | Orthorhombic and tetragonal structures in the La(La/Ba)2Cu3O9−δ system | 2.6 | 0 | Citations (PDF) |
| 253 | Analogy between Y2Ba4Cu8O16−x and Bi4Ca2Sr4Cu4O16+x | 0.9 | 19 | Citations (PDF) |
| 254 | Properties of films of high-Tc perovskite superconductors | 0.9 | 64 | Citations (PDF) |
| 255 | Fluctuation conductivity in inhomogeneous superconductors | 1.1 | 44 | Citations (PDF) |
| 256 | Upper critical field, fluctuation conductivity, and dimensionality ofYBa2Cu3O7−x | 2.5 | 426 | Citations (PDF) |
| 257 | Valence-band and core-level photoemission study of single-crystalBi2CaSr2Cu2O8superconductors | 2.5 | 34 | Citations (PDF) |
| 258 | Millimeter-wave surface resistance measurements in highly orientedYBa2Cu3O7−δthin films | 2.5 | 89 | Citations (PDF) |
| 259 | Optical anisotropy ofYBa2Cu3O7−x | 2.5 | 72 | Citations (PDF) |
| 260 | Thermodynamic fluctuations in the high-Tcperovskite superconductors | 2.5 | 126 | Citations (PDF) |
| 261 | Raman scattering spectra of superconductingBi2Sr2CaCu2O8single crystals | 2.5 | 55 | Citations (PDF) |
| 262 | Properties of Y-Ba-Cu-O thin films with ordered defect structure:Y2Ba4Cu8O20−x | 2.5 | 148 | Citations (PDF) |
| 263 | Ordered-defect structure in epitaxialYBa2Cu3O7−xthin films | 2.5 | 210 | Citations (PDF) |
| 264 | Scanning tunneling microscopy of thea‐bplanes of Bi2(Ca,Sr)3Cu2O8+δsingle crystal and thin film | 2.4 | 67 | Citations (PDF) |
| 265 | Two‐dimensional superstructure in the (001) plane of Bi2[Ca,Sr]3Cu2O8+δthin films | 2.4 | 31 | Citations (PDF) |
| 266 | Surface structure of Bi2Sr2CaCu2O8+δhigh‐temperature superconductors studied using low‐energy electron diffraction | 2.4 | 57 | Citations (PDF) |
| 267 | Site-selective doping and superconductivity in(La1−yPry)(Ba2−xLax)Cu3O7−δ | 2.5 | 40 | Citations (PDF) |
| 268 | Weakly coupled grain model of high‐frequency losses in highTcsuperconducting thin films | 2.4 | 239 | Citations (PDF) |
| 269 | Optical measurements on oriented thinYBa2Cu3O7−δfilms: Lack of evidence for excitonic superconductivity | 5.8 | 134 | Citations (PDF) |
| 270 | Electron-tunneling studies of thin films of high-Tcsuperconducting La-Sr-Cu-O | 2.5 | 72 | Citations (PDF) |
| 271 | Point-contact electron tunneling into the high-Tcsuperconductor Y-Ba-Cu-O | 2.5 | 84 | Citations (PDF) |
| 272 | Critical current densities and transport in superconducting YBa2Cu3O7−δ films made by electron beam coevaporation | 2.4 | 268 | Citations (PDF) |
| 273 | Onset of fractal growth: Statics and dynamics of diffusion-controlled polymerization | 2.5 | 45 | Citations (PDF) |
| 274 | Vibrational spectra and lattice instabilities in the high-Tcsuperconductors YBa2Cu3O7and GdBa2Cu3O7 | 2.5 | 12 | Citations (PDF) |
| 275 | Hc2spectroscopy of geometrical effects in La-S films | 2.5 | 7 | Citations (PDF) |
| 276 | Growth of highTcsuperconducting thin films using molecular beam epitaxy techniques | 2.4 | 129 | Citations (PDF) |
| 277 | Superconductivity and magnetism in the high-Tcsuperconductor YBaCuO | 5.8 | 119 | Citations (PDF) |
| 278 | Reactive magnetron sputtering of thin‐film superconductor YBa2Cu3O7−x | 2.4 | 136 | Citations (PDF) |
| 279 | Growth instability in diffusion controlled polymerization | 3.4 | 16 | Citations (PDF) |
| 280 | Elasticity of poly(diacetylene) gels: measurements by electric field coupling | 3.9 | 6 | Citations (PDF) |
| 281 | Calculated quasi‐eigenstates and quasi‐eigenenergies of quantum well superlattices in an applied electric field | 1.6 | 70 | Citations (PDF) |
| 282 | Reply to Comment on ‘‘Polydiacetylene macromolecules in solution: Electric field induced birefringence’’ | 2.2 | 9 | Citations (PDF) |
| 283 | Statics and Dynamics of the Diffusion-Limited Polymerization of the Conducting Polymer Polypyrrole | 5.8 | 58 | Citations (PDF) |
| 284 | Anderson localization and the theory of dirty superconductors. II | 2.5 | 84 | Citations (PDF) |
| 285 | Inhomogeneity effects on the magnetoresistance and the ghost critical field above Tcin thin mixture films of In-Ge | 1.4 | 25 | Citations (PDF) |
| 286 | Fractal eigendimensionalities for percolation clusters | 2.5 | 10 | Citations (PDF) |
| 287 | Anderson Localization and the Theory of Dirty Superconductors | 5.8 | 121 | Citations (PDF) |
| 288 | Conformation of polydiacetylene macromolecules in solution: Field induced birefringence and rotational diffusion constant | 2.2 | 55 | Citations (PDF) |
| 289 | Critical current of a percolating superconductor | 2.5 | 20 | Citations (PDF) |
| 290 | Electric Field Coupling to Slow Elastic Modes in Gels of Conjugated Polymers | 5.8 | 14 | Citations (PDF) |
| 291 | Comments on computer investigations of micrographs of metal films near their continuity threshold | 1.6 | 4 | Citations (PDF) |
| 292 | On the Fractal dimension and correlations in percolation theory | 0.8 | 11 | Citations (PDF) |
| 293 | Percolation scale effects in metal-insulator thin films | 0.8 | 23 | Citations (PDF) |
| 294 | Partial dimensional sequences and percolation | 0.8 | 5 | Citations (PDF) |
| 295 | Hall coefficient and conduction in a 2D percolation system | 2.3 | 43 | Citations (PDF) |
| 296 | Fluctuations of the mass of the infinite cluster at percolation | 2.3 | 6 | Citations (PDF) |
| 297 | 2D to 3D percolation crossover in the resistivity of co-evaporated Al-Ge mixture films | 1.5 | 11 | Citations (PDF) |
| 298 | Percolation Characteristics in Discontinuous Thin Films of Pb | 5.8 | 143 | Citations (PDF) |
| 299 | Localization in a one-dimensional disordered model | 2.0 | 5 | Citations (PDF) |
| 300 | Tc dependence of normal-state resistivity in granular superconductors | 0.7 | 3 | Citations (PDF) |
| 301 | Low Tc in non-granular Al-Ge thin films | 0.7 | 1 | Citations (PDF) |
| 302 | Dependence ofTcon the normal-state resistivity in granular superconductors | 2.5 | 35 | Citations (PDF) |
| 303 | The effect of crystallinity on the morphology of evaporated Al-Ge thin films | 2.3 | 24 | Citations (PDF) |
| 304 | Elastocaloric evidence for a multicomponent superconductor stabilized within the nematic state in Ba(Fe
1−
x
Co
x
)
2
As
2 | 5.3 | 6 | Citations (PDF) |
| 305 | Optical control of orbital magnetism in magic-angle twisted bilayer graphene | 10.8 | 2 | Citations (PDF) |
| 306 | High-resolution polar Kerr effect studies of
CsV
3
Sb
5
and
ScV
6
| 2.5 | 0 | Citations (PDF) |
