about
Boron isotope effect in superconducting MgB2Super-heavy electron material as metallic refrigerant for adiabatic demagnetization coolingUltrafast observation of critical nematic fluctuations and giant magnetoelastic coupling in iron pnictides.Six closely related YbT2Zn20 (T = Fe, Co, Ru, Rh, Os, Ir) heavy fermion compounds with large local moment degeneracy.Strong cooperative coupling of pressure-induced magnetic order and nematicity in FeSe.Solidification and loss of hydrostaticity in liquid media used for pressure measurements.Tricritical wings and modulated magnetic phases in LaCrGe3 under pressure.Magnetic ordering in GdAgSb2.Thermoelectric power of RAgSb(2) (R = Y, La, Ce, and Dy) in zero and applied magnetic fields.Effect of spatial confinement on magnetic hyperthermia via dipolar interactions in Fe₃O₄ nanoparticles for biomedical applications.Polar Intermetallics Pr5 Co2 Ge3 and Pr7 Co2 Ge4 with Planar Hydrocarbon-Like Metal Clusters.Physical properties of SrSn(4) single crystals.Physical properties of CeGe2-x (x=0.24) single crystals.Superelasticity and cryogenic linear shape memory effects of CaFe2As2.Preserved entropy and fragile magnetism.A family of binary magnetic icosahedral quasicrystals based on rare earths and cadmium.Crystallographic, electronic, and magnetic studies of zeta(2)-GaM (M = Cr, Mn or Fe): trends in itinerant magnetism.Synthesis, Structure, and Complex Magnetism of MIr2In8 (M = Eu, Sr).Pauli paramagnetic effects on vortices in superconducting TmNi2B2C.Uniaxial strain control of spin-polarization in multicomponent nematic order of BaFe2As2.Ferromagnetic Quantum Critical Point Avoided by the Appearance of Another Magnetic Phase in LaCrGe_{3} under Pressure.Giant magnetic anisotropy and tunnelling of the magnetization in Li₂(Li(1-x)Fe(x))N.Origin of the Resistivity Anisotropy in the Nematic Phase of FeSe.Inelastic neutron scattering study of a nonmagnetic collapsed tetragonal phase in nonsuperconducting CaFe2As2: evidence of the impact of spin fluctuations on superconductivity in the iron-arsenide compounds.Coexistence of cluster spin glass and superconductivity in Ba(Fe(1-x)Co(x))2As2 for 0.060≤x≤0.071.Effect of Biaxial Strain on the Phase Transitions of Ca(Fe_{1-x}Co_{x})_{2}As_{2}.Hedgehog Spin-Vortex Crystal Antiferromagnetic Quantum Criticality in CaK(Fe_{1-x}Ni_{x})_{4}As_{4} Revealed by NMRDual nature of 3delectrons in YbT2Zn20(T = Co; Fe) evidenced by electron spin resonanceAnisotropy of SuperconductingMgB2as Seen in Electron Spin Resonance and Magnetization DataHydrostatic-pressure tuning of magnetic, nonmagnetic, and superconducting states in annealed Ca(Fe1−xCox)2As2Effects of Band Filling on Magnetic Structures: The Case ofRNi2Ge2The magnetic structures of DyNi2Ge2Pressure-induced collapsed-tetragonal phase inSrCo2As2Suppression of antiferromagnetic spin fluctuations in superconducting Cr0.8Ru0.2Competition between stripe and checkerboard magnetic instabilities in Mn-doped BaFe2As2Magnetic excitations in underdoped Ba(Fe1−xCox)2As2withx=0.047Magneto-optical studies of the uniform critical state in bulk MgB2Direct visualization of phase separation between superconducting and nematic domains in Co-doped CaFe2As2 close to a first-order phase transitionInfrared pseudogap in cuprate and pnictide high-temperature superconductorsMeasurements of elastoresistance under pressure by combining in-situ tunable quasi-uniaxial stress with hydrostatic pressure
P50
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P50
description
condensed matter experimental physicist at Ames Lab and Iowa State University
@en
natuurkundige
@nl
name
Sergey L. Bud'ko
@ast
Sergey L. Bud'ko
@en
Sergey L. Bud'ko
@es
Sergey L. Bud'ko
@nl
type
label
Sergey L. Bud'ko
@ast
Sergey L. Bud'ko
@en
Sergey L. Bud'ko
@es
Sergey L. Bud'ko
@nl
altLabel
Sergey Budko
@en
Serguei Bud'ko
@en
Serguei Budko
@en
prefLabel
Sergey L. Bud'ko
@ast
Sergey L. Bud'ko
@en
Sergey L. Bud'ko
@es
Sergey L. Bud'ko
@nl
P106
P31
P496
0000-0002-3603-5585