Showing 1–20 of 63 results
/ Date/ Name
Nov 1, 2021Characterization of Pedestal Burst Instabilities during I-mode to H-mode Transition in the EAST TokamakFeb 20, 2020Edge Temperature Ring Oscillation Modulated by Turbulence Transition for Sustaining Stationary Improved Energy Confinement PlasmasAug 14, 2013The simultaneous occurrence of superparamagnetism and superconductivity in nominal single crystalline (Ca1-xPrx)Fe2As2 with 0 <= x <= 0.13Nov 5, 2010Incommensurate spin-density wave and multiband superconductivity in Na$_{x}$FeAs as revealed by nuclear magnetic resonanceOct 3, 2019Decoupling of Lattice and Orbital Degrees of Freedom in an Iron-Pnictide SuperconductorFeb 4, 2009The Synthesis and Characterization of LiFeAs and NaFeAsFeb 27, 2009The superconductor KxSr(1-x)Fe2As2: Normal state and superconducting propertiesApr 6, 2010Evidence for multiple gaps in specific heat of LiFeAs crystalsJun 10, 2011The Unusual Superconducting State at 49 K in Electron-Doped CaFe2As2 at AmbientMay 5, 2016Tip Pressure Induced Incoherent Energy Gap in CaFe2As2Oct 27, 2012Experimental investigation of the electronic structure of Ca$_{0.83}$La$_{0.17}$Fe$_2$As$_2$Aug 24, 2012Anomalous hysteresis as an evidence for a magnetic field-induced chiral superconducting state in LiFeAsAug 30, 2013Why is the superconducting Tc so high in rare-earth-doped CaFe2As2?Jun 7, 2008Superconductivity up to 37 K in (A1-xSrx)Fe2As2 with A=K and CsJan 28, 2009Pressure shift of the superconducting T_c of LiFeAsJan 22, 2020Superconductivity in the regime of attractive interactions in the Tomonaga-Luttinger liquidAug 6, 2024Suppression of Edge Localized Modes in ITER Baseline Scenario in EAST using Edge Localized Magnetic PerturbationsFeb 12, 2016Evidence for Defect-induced Superconductivity up to 49 K in (Ca1-xRx)Fe2As2May 4, 2012Thermodynamic evidence for pressure-induced bulk superconductivity in the Fe-As pnictide superconductor CaFe2As2Oct 27, 2011High-pressure study of superconducting and non-superconducting single crystals of the same nominal composition Rb0.8Fe2Se2