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Anomalous magneto-elastic and charge doping effects in thallium-doped BaFe2As2.Epitaxial Growth of Intermetallic MnPt Films on Oxides and Large Exchange Bias.Pressure induced second-order structural transition in Sr₃Ir₂O₇.Full Electroresistance Modulation in a Mixed-Phase Metallic Alloy.Multi-layered Chalcogenides with potential for magnetism and superconductivityMetallicity of Ca 2 Cu 6 P 5 with single and double copper-pnictide layersCO-doping effects on the transport and magnetic properties of FeTeFerromagnetism: Epitaxial Growth of Intermetallic MnPt Films on Oxides and Large Exchange Bias (Adv. Mater. 1/2016)Doping effects of Sb in FeTe1−xSbx single crystalsEvolution of magnetism in single-crystalCa2Ru1−xIrxO4(0≤x≤0.65)Role of magnetism in superconductivity ofBaFe2As2: Study of5dAu-doped crystalsSuperconductivity in semimetallicBi3O2S3Novel Magnetism ofIr5+(5d4)Ions in the Double PerovskiteSr2YIrO6Doping effects of Co and Cu on superconductivity and magnetism in Fe1+yTe0.6Se0.4single crystalsEvolution of magnetism in the single-crystal honeycomb iridates(Na1−xLix)2IrO3First-order spin reorientation transition and specific-heat anomaly in CeFeO3Giant vertical magnetization shift induced by spin canting in a Co/Ca2Ru0.98Fe0.02FeO4heterostructureMagnetic field and pressure effects on magnetism of bond-frustrated ZnCr2S4Observation of superconductivity and anomalous electrical resistivity in single-crystal Ir3Te8Single crystal growth, transport, and electronic band structure of YCoGa5Superconductivity in Fe1.05Te:Oxsingle crystalsTuning theJeff=12insulating state via electron doping and pressure in the double-layered iridate Sr3Ir2O7Annealing effects on superconductivity and magnetism in Fe1+yTe1−xSx single crystalsAnnealing induced colossal magnetocapacitance and colossal magnetoresistance in In-doped CdCr2S4Magnetic field and external pressure effects on the spiral order of polycrystalline MnCr2O4Spin-orbit tuned metal-insulator transitions in single-crystal Sr2Ir1−xRhxO4(0≤x≤1)Coexistence of superconductivity and magnetism in KxFe2−ySe2−zSz(z=0,0.4)Magnetism and superconductivity in MxFe1+yTe1–zSez (M = Cr, Mn, Co, Ni, Cu, and Zn) single crystalsSuperconductivity and magnetism in FeSe thin films grown by metal–organic chemical vapor depositionCritical properties of the 3D-Heisenberg ferromagnet \chem{CdCr_{2}Se_{4}}Disorder-induced orbital glass state in FeCr2S4Inconsistent pressure effect on superconducting transition temperature and volume in Fe1+yTe1−xSexsingle crystalsPressure effects on superconductivity of Fe1+yTe1−xSx single crystalsSpin–lattice coupling studied by magnetic entropy and EPR in the systemPressure Effect on Superconductivity and Magnetism in α-FeSe xSulfur substitution and pressure effect on superconductivity of α-FeSeAnnealing effects on superconductivity in Rb0.81Fe1.72Se2 single crystalDependence of temperature-dependent electrical resistivity of SrIrO3 on hydrostatic pressure to 9.1 kbar
P50
Q36574398-01029B20-63F2-4502-A1AB-76076BCB917CQ44156120-69C234FF-4174-4756-AC2D-65A567778824Q45770026-DB965A88-0E71-4177-AF47-65061B8F2A56Q51435564-517E3395-F2E5-49E1-BBCE-EABEBAF9E492Q53405042-4CCE0D1D-5ED1-4291-8045-9FC611E24190Q53405746-61B9C8AD-F9C6-4DD9-8AAF-325F5F15D4A7Q53405772-758E54C6-59C4-44A6-8FB5-EEBEC8A7B467Q53405796-745C2CBA-899A-4CCB-BE33-2BCCB73C2DB4Q53405813-9EE67A67-8125-441C-8117-660BC29E883BQ53405820-B932112C-4838-4956-9E22-A563C610AA74Q53405824-B9EA6D3B-235E-4FCB-88DD-3EECA33643CCQ53405832-C09F87CA-AA46-4FD9-938E-7171A682EAA3Q53405839-5E8C25D2-16B2-4509-8A7D-E2799E96E64DQ53405895-8AB8C192-AC40-4177-BAC8-333758D5F1CBQ53405900-A3136E53-FC37-4B93-A051-C1B8D7E28D99Q53405904-E77989CF-E16C-48E7-84A1-46A892C7BFE9Q53405908-FA586D3C-DCFC-4792-B879-78AAB09EB512Q53405912-560FB038-B2AA-426F-BB10-E12758D46D83Q53405914-C463A6C0-F127-4C9C-92A4-49B563DD4C4EQ53405921-F3DBEDD0-05E8-43CF-ADD8-E04FCF14FE5FQ53405928-31BFED84-FBBD-4845-BE92-1400AB218252Q53405935-E1140E1E-4C77-409A-AD97-792B353F5161Q53405940-5A47B821-BB04-4E45-956B-C2C76FCD1615Q53405945-B3AED409-CFFA-490D-B12A-D404D17E99EEQ53405952-4E9B7AC8-5625-46BB-A8B3-BB1DA6E1FAC4Q53405956-3058367F-00F3-4F72-94D9-9B6B8A9A635DQ53405959-4AD3701C-BF7D-431A-BBEB-E4B5140A753FQ53405964-C5E6CD52-4E6D-4641-860E-22DB33D905B6Q53405971-6DBA194C-BE95-46CD-A2A8-E0A3E436306FQ53405976-F683A039-FC03-4B3E-A4F5-7124023332F7Q53405982-0A7556AA-8A02-4548-884C-72FE0B01698AQ53405986-D7175C39-8563-415E-A9FA-59E891912A9BQ53405990-7C4FD96C-4D6C-4392-B596-BEB55BD75428Q53405996-9167EAAC-92F7-4A46-8158-E9AFE8E37C84Q53405997-905DC2B5-1F32-4CB4-817E-C665C702DCE7Q53406005-37B47D3E-EC68-4931-A54B-8BB14FA1EB76Q54678283-2779A9BB-0310-4CEA-B618-6D9CB705557DQ54678291-2ABB609B-FEE7-4E7C-A0CE-17F269658ED1
P50
description
materials scientist
@en
name
Li Li
@ast
Li Li
@en
Li Li
@es
Li Li
@nl
Li Li
@sl
type
label
Li Li
@ast
Li Li
@en
Li Li
@es
Li Li
@nl
Li Li
@sl
prefLabel
Li Li
@ast
Li Li
@en
Li Li
@es
Li Li
@nl
Li Li
@sl
P108
P1053
G-6406-2013
P106
P31
P3829
P496
0000-0003-1683-8118