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Magnetic-superconducting phase boundary of SmFeAsO 1 − x F x studied via muon spin rotation: Unified behavior in a pnictide familyNanoscopic coexistence of magnetism and superconductivity in YBa2Cu3O6+x detected by muon spin rotationMagnetic states of MnP: muon-spin rotation studies.Ferromagnetic Quantum Critical Point Avoided by the Appearance of Another Magnetic Phase in LaCrGe_{3} under Pressure.Relaxation dynamics in the frustratedCr9antiferromagnetic ring probed by NMRExchange interactions in Ca3Co2O6probed locally by NMRCoherent Manipulation of a Molecular Ln-Based Nuclear Qudit Coupled to an Electron QubitErratum: Evidence of Orbital Reconstruction at Interfaces in UltrathinLa0.67Sr0.33MnO3Films [Phys. Rev. Lett.100, 137401 (2008)]Evidence of Orbital Reconstruction at Interfaces in UltrathinLa0.67Sr0.33MnO3FilmsStrain-induced phase separation inLa0.7Sr0.3MnO3thin filmsSoft x-ray absorption and high-resolution powder x-ray diffraction study of superconducting CaxLa1−xBa1.75−xLa0.25+xCu3Oy systemEffect of the external pressure at the crossover between magnetism and superconductivity in LnFeAsO1−xFx (Ln = La0.7Y0.3, Ce) superconductorsEffect of external pressure on the magnetic properties of R CoAsO ( R =La, Pr, Sm): a μSR studyPoisoning effect of Mn inLaFe1−xMnxAsO0.89F0.11: Unveiling a quantum critical point in the phase diagram of iron-based superconductorsRole of in-plane and out-of-plane dilution in CeFeAsO: Charge doping versus disorderOnset of magnetism in optimally electron-dopedLFe1−xRuxAsO1−yFy(L=La, Nd, or Sm) superconductors aroundx=14Common effect of chemical and external pressures on the magnetic properties ofRCoPO (R=La, Pr)Phase separation at the magnetic-superconducting transition in La0.7Y0.3FeAsO1−xFxEffect of external pressure on the magnetic properties of LnFeAsO (Ln = La, Ce, Pr, Sm)ac susceptibility investigation of vortex dynamics in nearly optimally dopedRFeAsO1−xFxsuperconductors (R= La, Ce, Sm)Magnetic properties of spin-diluted iron pnictides fromμSR and NMR in LaFe1−xRuxAsOLong- to short-range magnetic order in fluorine-doped CeFeAsOCorrelated Trends of Coexisting Magnetism and Superconductivity in Optimally Electron-Doped OxypnictidesTuning of competing magnetic and superconducting phase volumes in LaFeAsO0.945F0.055by hydrostatic pressureVortex dynamics and irreversibility line in optimally doped SmFeAsO0.8F0.2from ac susceptibility and magnetization measurementsEvidence for impurity-induced frustration in La2CuO4Nanoscopic coexistence of magnetic and superconducting states within the FeAs layers ofCeFeAsO1−xFxNMR and high-resolution x-ray diffraction evidence for an alkali-metal fulleride with large interstitial clusters:Li12C60Observation of endohedral muonium in C61H2Magnetism ofMg1−xMnxO4spinels by SQUID magnetometry and muon spin rotation spectroscopyMagnetic order and spin dynamics in substituted spinel Mg1−xMn2+xO4Phase separation in superconducting EuBa2Cu3O6+xμSR studies of superconductivity in eutectically grown mixed ruthenates75As NQR signature of the isoelectronic nature of ruthenium for iron substitution in LaFe1−xRuxAsOIntrinsic Ferromagnetic Impurity Phases in SmFeAsO1−x F x Detected by μSRStripe disorder and dynamics in the hole-doped antiferromagnetic insulator La5/3Sr1/3CoO4Competing effects of Mn and Y doping on the low-energy excitations and phase diagram ofLa1−yYyFe1−xMnxAsO0.89F0.11iron-based superconductorsHigh-pressure magnetic state of MnP probed by means of muon-spin rotationMagnetic ground state and spin fluctuations in MnGe chiral magnet as studied by muon spin rotationMagnetic phase diagram ofLa2−xSrxCoO4revised using muon-spin relaxation
P50
Q27347501-999F66C0-EDDA-4AB9-ABE6-3EF578959EB1Q27349270-6DDF4B6B-E3B3-4E62-826C-BDEF8CB9A0CAQ38890479-B79D705B-29E2-4916-9E08-A9C2348D5D89Q53050897-F809EE39-92FA-4118-92B6-2253AC7883D3Q57665255-51ADD7E0-83AB-4B30-8FC0-959B928426FAQ57665276-BDBFBF8D-89D0-4A72-BD1F-4FA816C775ABQ57706400-BEF49323-E3AE-4D69-9406-26456731138AQ58199516-0FE258C1-BE97-4A82-A023-5423B0BEDB80Q58199530-7A230B53-153A-4345-B444-20D388057036Q58199574-CD206D5E-9FB1-4657-9B03-C13D24AFAD99Q58908944-6A76872C-79CF-4130-9FA0-B2770A295418Q59447109-B499D1CE-9AF2-4991-AA65-1A8A6C8EA131Q59447132-908123A6-92C6-4C7F-98D1-596B5768CD73Q59447137-9F45827B-9426-4A5D-A78E-50606DDE9771Q59447145-F48C3045-E2E7-4EE1-A61E-D72EC714E65AQ59447149-3FCEFBD9-E6CC-4AAC-AC3C-5B1740877FEEQ59447154-C1C172E5-C5DE-4841-87A0-56EB07E39ECAQ59447158-926B73D5-8FD2-4BAD-927A-6F9C366B7193Q59447162-FEC3B819-97A4-43F1-AFAB-7AB496EB508DQ59447167-A980C001-EC5B-41B9-A6C0-7AE2A0062359Q59447171-7B361C32-1E18-4EE4-B4A9-AB53C9BE2456Q59447175-0FA68B59-2E79-42FA-941F-2613FCBC6CB9Q59447179-00E871BC-D6DE-413D-BE98-11E75762CBA1Q59447182-EB2280CC-B539-420C-840F-AF152E7391C4Q59447189-48859058-97F2-4989-A66B-B0692485F32EQ59447193-165966F6-88E8-4F4D-90E6-A5A8BEB13161Q59447199-9227FBD1-8101-48E6-80B7-64933A3E4937Q60081793-C36B83F8-A682-4B65-B975-4F1C5C7A4D1EQ60081834-C8069DD9-34D0-444D-8F14-0437F6DD0A40Q60235860-FFCD4245-8092-4DBC-B396-D7E07F19E0E2Q60235889-ED47218D-0858-4C6B-B0CF-E65E671CBB46Q60235893-0BA6DBB8-CBEA-49AC-B158-B3E81DC69F6AQ60243203-939076B3-292C-4A9A-8811-8DB1C837819AQ60244124-A45E00A6-DDC5-4DDC-8440-A35B3911601DQ60244158-BBBF20FC-FCC1-4AB6-9BC3-700CE5448626Q60298284-1092EC4F-4E76-443B-BE78-10143D43A1FFQ60298285-821E9F94-1E3C-4BE7-8DCD-78C94B3CF054Q60298286-7CDFD194-E326-42B0-9E28-6C5D73BFE921Q60298287-C95844E4-7EE3-4F0A-988E-850A146D65CBQ60298289-306B0CC0-8E1A-4A54-90D6-40D81CF35856
P50
description
onderzoeker
@nl
researcher ORCID ID = 0000-0002-5015-0061
@en
name
R. De Renzi
@nl
Roberto De Renzi
@en
Roberto De Renzi
@es
type
label
R. De Renzi
@nl
Roberto De Renzi
@en
Roberto De Renzi
@es
altLabel
R. De Renzi
@en
prefLabel
R. De Renzi
@nl
Roberto De Renzi
@en
Roberto De Renzi
@es
P1053
F-9182-2011
P106
P1153
7004234833
P21
P31
P496
0000-0002-5015-0061