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Filming the formation and fluctuation of skyrmion domains by cryo-Lorentz transmission electron microscopyElectromagnon dispersion probed by inelastic X-ray scattering in LiCrO2.Hallmarks of Hunds coupling in the Mott insulator Ca2RuO4.Antiferromagnetic order induced by an applied magnetic field in a high-temperature superconductor.A new class of chiral materials hosting magnetic skyrmions beyond room temperatureDramatic pressure-driven enhancement of bulk skyrmion stability.Magnetodielectric detection of magnetic quadrupole order in Ba(TiO)Cu4(PO4)4 with Cu4O12 square cupolas.Neutral Aminyl Radicals Derived from Azoimidazolium Dyes.CAMEA--A novel multiplexing analyzer for neutron spectroscopy.Clean, cleaved surfaces of the photovoltaic perovskite.Dipolar antiferromagnetism and quantum criticality in LiErF₄.Charge-Stripe Order and Superconductivity in Ir1-xPtxTe2.Prototype of the novel CAMEA concept-A backend for neutron spectrometers.Robust metastable skyrmions and their triangular-square lattice structural transition in a high-temperature chiral magnet.Dinuclear clathrochelate complexes with pendent cyano groups as metalloligands.Superparamagnetic Nanoparticles as High Efficiency Magnetic Resonance Imaging T2 Contrast Agent.Correction to Superparamagnetic Nanoparticles as High Efficiency Magnetic Resonance Imaging T2 Contrast Agent.Spin dynamics of the 2D spin 1/2 quantum antiferromagnet copper deuteroformate tetradeuterate (CFTD).Origin of the Spin-Orbital Liquid State in a Nearly J=0 Iridate Ba_{3}ZnIr_{2}O_{9}.Néel-type skyrmion lattice with confined orientation in the polar magnetic semiconductor GaV4S8.Single-chip electron spin resonance detectors operating at 50GHz, 92GHz, and 146GHz.Chemical tunnel-splitting-engineering in a dysprosium-based molecular nanomagnet.Dimensional Reduction in Quantum Dipolar Antiferromagnets.Quantum Phase Transition of a Magnet in a Spin BathThree-dimensionality of field-induced magnetism in a high-temperature superconductor.Direct electric field control of the skyrmion phase in a magnetoelectric insulator.Collective Magnetic Excitations in the Spin LadderSr14Cu24O41Measured Using High-Resolution Resonant Inelastic X-Ray ScatteringNeutron Decoherence Imaging for Visualizing Bulk Magnetic Domain StructuresDisordered skyrmion phase stabilized by magnetic frustration in a chiral magnetPolarons and confinement of electronic motion to two dimensions in a layered manganiteMultiple- noncollinear magnetism in an itinerant hexagonal magnetSpin excitations in a single La2CuO4 layerDirect Observation of Magnon Fractionalization in the Quantum Spin LadderProbing multi-spinon excitations outside of the two-spinon continuum in the antiferromagnetic spin chain cuprate SrCuOScale-Free Antiferromagnetic Fluctuations in thes=1/2Kagome Antiferromagnet HerbertsmithiteDispersive Excitations in the High-Temperature SuperconductorLa2−xSrxCuO4The ${J}_{\mathrm{eff}}=\frac{1}{2}$ insulator Sr3Ir2O7studied by means of angle-resolved photoemission spectroscopyMagnetic-Field-Induced Soft-Mode Quantum Phase Transition in the High-Temperature SuperconductorLa1.855Sr0.145CuO4: An Inelastic Neutron-Scattering StudyMagnetic-Field-Induced Spin Excitations and Renormalized Spin Gap of the UnderdopedLa1.895Sr0.105CuO4SuperconductorStrain-engineering Mott-insulating LaCuO
P50
Q27319904-707C26A5-0C60-448C-9912-8A6413D2E7F0Q30369038-7E44200B-4F43-49ED-ACF3-C9EA21B3B041Q33654585-73FA405F-836D-4DB1-9EC9-D5D2323B25BFQ34109925-937877C2-A64D-4537-987F-6614B2438500Q35863483-5703D38C-C128-4960-9464-4C5DD870BA65Q36595494-949B1FCB-6F8F-4D94-9B79-0C8C2DD3231EQ37329832-EDDCBC34-CF4B-4BA2-BF44-30A2CC7AF86DQ39116732-CE720F01-5241-48EC-B12B-DAFF4E9F2855Q39870939-FB031FDF-135B-4360-A356-CAA545AA59ABQ42126670-1B7E7855-2D5D-472D-98DE-4EFED4F40D88Q46567443-79FED5BA-298E-4042-8CDD-5720BF563834Q47157314-B56A3CE8-7D26-4A6A-85AA-671444E650D4Q48042379-8691A900-38BF-4EF8-B222-61992E6F675DQ48265917-9A61EFFB-C755-4753-8ECB-D378C50CA2EAQ48311013-76A7BBC7-51E1-411D-A29B-70A528527607Q48344868-CCCED3F8-344A-420A-B166-E6B71549AC5FQ48587887-8AC35FE1-5E30-4440-8D2C-2ED30D4E011EQ49740512-1BA83238-9213-4F4A-BF7A-C26FCEB30D2BQ50689164-E13613AA-30A9-43CA-A631-2BA2E513A258Q50858633-79F6E508-8B3E-4879-9961-7DD2E6F51D5FQ51441013-F1190939-BCF2-4F7C-8D4D-7B66A578D873Q51732425-94EE9F42-ECC9-4E96-BDFF-A86E4DFA79B0Q52851829-8FD29E78-FDFA-4E5B-86D9-BC513FE8BEA1Q53585580-1DE09149-3BEE-4B31-8550-7098924E33CEQ53847474-03270DDD-E9BF-47D3-84B6-FF4EE8B881F1Q55664807-DC81C059-7A77-45BF-9D62-1BDA876BB896Q58199508-32340C16-3FBA-4B26-90CF-35B9854CBEB5Q58444526-574B08AC-27B1-446A-A51C-57F15161EC82Q58740474-20E7A467-616C-47D1-97DC-0637A40250D9Q58830138-96646279-8AFC-45BB-9A0F-2A0B2B926E48Q59136631-5A977BAA-9D87-412B-A056-F8AB68FD005AQ59348683-A2ACD658-02BC-45B0-9399-351ACCCC34B4Q59461906-25D7ACA8-B0BD-457B-ABD3-73CAD060E247Q60300803-2AA64173-A612-4E71-A8AF-BE6FC29F6993Q60962423-3951E9CB-75D3-4954-8C85-20E197559FD7Q62475713-D5DEDD35-99F2-4378-86A5-6EC4754D69F3Q62481308-990240F8-9954-46F5-A517-226701C260F5Q62481337-DF837282-69C2-40CC-96E4-7920BBFF5806Q62481356-9D74BA50-0BBB-4470-9445-C30E7A9ACB9CQ64258438-56DD5AE3-6011-4BFE-8A72-6EA1AE91FC83
P50
description
researcher
@en
name
Henrik M. Rønnow
@en
Rønnow HM
@nl
type
label
Henrik M. Rønnow
@en
Rønnow HM
@nl
altLabel
Rønnow HM
@en
prefLabel
Henrik M. Rønnow
@en
Rønnow HM
@nl
P106
P31
P496
0000-0002-8832-8865