From Quantum Paraelectric/Ferroelectric Perovskite Oxides to High Temperature Superconducting Copper Oxides -- In Honor of Professor K.A. Müller for His Lifework
From Quantum Paraelectric/Ferroelectric Perovskite Oxides to High Temperature Superconducting Copper Oxides -- In Honor of Professor K.A. Müller for His Lifework
English[eng]
ferroelastic||WO3||polarons||polaronic superconductivity||transition metal dichalcogenides||magnetic semiconductor spintronics||n/a||transition metal oxides||lattice–spin–charge landscapes||elasticity||superconductivity||cuprates||magnetic penetration depth||order parameter||superconducting gap structure||Kondo effect||spin relaxation rate||magnetic resonance||strontium titanate||quantum paraelectricity||quantum fluctuations||ferroelectricity||isotope exchange||external stress||polar metal||phase coexistence||magnetoelectric multiglass||Electron Paramagnetic Resonance (EPR)||ENDOR||Jahn-Teller||color centers||3d impurities||perovskite||SrTiO3||18O||isotope substitution||SrTiO3/LaAlO3||interface||heterostructure||tungsten oxide||phase separation||cuprate superconductors||electronic correlations||NMR||pseudogap||perovskite crystals||Pseudo-Jahn-Teller effect||multiferroicity||permittivity||flexoelectricity||polar nanoregions||orientational polarization||LSCO||anti-Jahn-Teller effect||first-principles calculation||Kamimura-Suwa model||spin-polarized band||Hund’s coupling spin-triplet and spin-singlet multiplets||high-temperature superconductivity||correlated Femi liquid||charge density wave||fluctuation||strange metal||coherence length||granular superconductivity||Mott transition||BCS–BEC cross-over||electron-phonon interaction||topological insulator||topological materials||transition metal dichalcogenide||helium atom scattering||perovskite oxides||phase transitions||high-temperature cuprate superconductors
English[eng]
ferroelastic||WO3||polarons||polaronic superconductivity||transition metal dichalcogenides||magnetic semiconductor spintronics||n/a||transition metal oxides||lattice–spin–charge landscapes||elasticity||superconductivity||cuprates||magnetic penetration depth||order parameter||superconducting gap structure||Kondo effect||spin relaxation rate||magnetic resonance||strontium titanate||quantum paraelectricity||quantum fluctuations||ferroelectricity||isotope exchange||external stress||polar metal||phase coexistence||magnetoelectric multiglass||Electron Paramagnetic Resonance (EPR)||ENDOR||Jahn-Teller||color centers||3d impurities||perovskite||SrTiO3||18O||isotope substitution||SrTiO3/LaAlO3||interface||heterostructure||tungsten oxide||phase separation||cuprate superconductors||electronic correlations||NMR||pseudogap||perovskite crystals||Pseudo-Jahn-Teller effect||multiferroicity||permittivity||flexoelectricity||polar nanoregions||orientational polarization||LSCO||anti-Jahn-Teller effect||first-principles calculation||Kamimura-Suwa model||spin-polarized band||Hund’s coupling spin-triplet and spin-singlet multiplets||high-temperature superconductivity||correlated Femi liquid||charge density wave||fluctuation||strange metal||coherence length||granular superconductivity||Mott transition||BCS–BEC cross-over||electron-phonon interaction||topological insulator||topological materials||transition metal dichalcogenide||helium atom scattering||perovskite oxides||phase transitions||high-temperature cuprate superconductors