0000000001309203

AUTHOR

Marco Evangelisti

showing 18 related works from this author

Fragmenting gadolinium: Mononuclear polyoxometalate-based magnetic coolers for ultra-low temperatures

2012

The polyoxometalate clusters with formula [Gd(W 5O 18) 2] 9- and [Gd(P 5W 30O 110)] 12- each carry a single magnetic ion of gadolinium, which is the most widespread element among magnetic refrigerant materials. In an adiabatic demagnetization, the lowest attainable temperature is limited by the presence of magnetic interactions that bring about magnetic order below a critical temperature. We demonstrate that this limitation can be overcome by chemically engineering the molecules in such a way to effectively screen all magnetic interactions, suggesting their use as ultra-low-temperature coolers. © 2012 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.

Materials scienceMolecular nanomagnetsEntropyMechanical EngineeringGadoliniumchemistry.chemical_elementGadoliniumNanotechnologyTungsten CompoundsCold TemperatureMagneticschemistryMechanics of MaterialsPolyoxometalateMagnetic refrigerationmedia_common.cataloged_instanceGeneral Materials ScienceEuropean unionmedia_common
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Tunable crossover between one- and three-dimensional magnetic dynamics inCoIIsingle-chain magnets organized by halogen bonding

2016

Low-temperature magnetometry, ac susceptibility, and calorimetry have been employed to study Co-based single-chain magnets (SCMs) organized through halogen bonding. Magnetic hysteresis and maxima in the dc and ac susceptibilities, respectively, confirm the SCM behavior of the system. Several characteristic magnetic relaxation regimes are observed at different temperatures, which can be associated with both intra- and interchain exchange interactions. Remarkably, tweaking the rate at which an external magnetic field is swept along the axis of the chains enables a controlled transition between the one- and three-dimensional dynamics. Experiments on an isostructural Co-based SCM system crystal…

Halogen bondMaterials scienceMagnetometerNanotechnology02 engineering and technologyCalorimetry021001 nanoscience & nanotechnologyMagnetic hysteresis01 natural sciencesMagnetic fieldlaw.inventionChemical physicslawMagnet0103 physical sciencesHalogenCondensed Matter::Strongly Correlated ElectronsIsostructural010306 general physics0210 nano-technologyPhysical Review B
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A [Cr2Ni] coordination polymer: slow relaxation of magnetization in quasi-one-dimensional ferromagnetic chains

2018

The reaction of [Cr3IIIO(OAc)6(H2O)3]NO3·AcOH with 2-hydroxynaphthaldehyde, 2-amino-isobutyric acid and NiCl2·6H2O in MeOH, under basic and solvothermal conditions, led to the formation of the quasi-1D coordination polymer {[CrIII2NiII(L)4(MeOH)2]}n (where L = the dianion of the Schiff base between 2-hydroxynaphthaldehyde and 2-amino-isobutyric acid), which behaves as a ferromagnetic chain, displaying slow relaxation of magnetization.

Materials scienceCoordination polymer010402 general chemistry01 natural sciencesCatalysisMETAL-ORGANIC FRAMEWORKSchemistry.chemical_compoundMagnetizationChain (algebraic topology)SYSTEMSNANO-MAGNETSABSORPTIONMaterials ChemistryFIELDANTIFERROMAGNETSANISOTROPYMOSSBAUER RELAXATIONSchiff base010405 organic chemistryNONLINEAR EXCITATIONSMetals and AlloysGeneral ChemistrySINGLE-MOLECULE MAGNETS0104 chemical sciencesSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsCrystallographychemistryFerromagnetismCeramics and CompositesRelaxation (physics)Quasi one dimensional
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A quantum spin liquid candidate isolated in a two-dimensional CoIIRhIII bimetallic oxalate network

2023

A quantum spin liquid (QSL) is an elusive state of matter characterized by the absence of long-range magnetic order, even at zero temperature, and by the presence of exotic quasiparticle excitations. In spite of their relevance for quantum communication, topological quantum computation and the understanding of strongly correlated systems, like high-temperature superconductors, the unequivocal experimental identification of materials behaving as QSLs remains challenging. Here, we present a novel 2D heterometallic oxalate complex formed by high-spin Co(II) ions alternating with diamagnetic Rh(III) in a honeycomb lattice. This complex meets the key requirements to become a QSL: a spin ½ ground…

General ChemistryChemical Science
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Electronic and magnetic properties of Mn 12 molecular magnets on sulfonate and carboxylic acid prefunctionalized gold surfaces

2012

Structural, electronic, and magnetic properties of [Mn 12O 12(bet) 16(EtOH) 4](PF 6) 14·4CH 3CN·H 2O (in short Mn 12bet, bet = betaine = +N(CH 3) 3-CH 2-COO -) single-molecule magnets (SMMs) deposited on previously functionalized gold surfaces have been investigated. Self-assembled monolayers (SAMs) either of sodium mercaptoethanesulfonate (MES) or mercaptopropionic acid (MPA) are used as functionalization to avoid the direct interaction between the Mn 12bet molecules and the Au surface with the aim of preserving the main functional properties of the molecules. Scanning tunneling microscopy (STM) and X-ray photoemission spectroscopy (XPS) analysis show deposited Mn 12bet SMMs well-isolated …

X-ray absorption spectroscopyAbsorption spectroscopyPhotoemission spectroscopyXMCDElectronic Optical and Magnetic MaterialInorganic chemistrySurfaces Coatings and Filmsurface layerSurfaces Coatings and FilmsElectronic Optical and Magnetic Materialslaw.inventionchemistry.chemical_compoundCrystallographyEnergy (all)General EnergySulfonatechemistryX-ray photoelectron spectroscopylawOxidation stateMonolayerPhysical and Theoretical ChemistryScanning tunneling microscopeMolecular magnets; XMCD; surface layerMolecular magnetsJournal of Physical Chemistry C
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Gd-based single-ion magnets with tunable magnetic anisotropy: Molecular design of spin qubits

2012

et al.

PhysicsMagnetic anisotropyPhysics and Astronomy (all)Condensed matter physicsPulsed EPRPolyoxometalateIsotropyGeneral Physics and AstronomyFigure of meritMoleculeQuantum tunnellingIon
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Two C3-symmetric Dy3 III complexes with triple di-μ-methoxo-μ-phenoxo bridges, magnetic ground state, and single-molecule magnetic behavior

2014

Two series of isostructural C3-symmetric Ln3 complexes Ln3·[BPh4] and Ln3·0. 33[Ln(NO3)6] (in which LnIII=Gd and Dy) have been prepared from an amino-bis(phenol) ligand. X-ray studies reveal that LnIII ions are connected by one μ2-phenoxo and two μ3-methoxo bridges, thus leading to a hexagonal bipyramidal Ln3O5 bridging core in which LnIII ions exhibit a biaugmented trigonal-prismatic geometry. Magnetic susceptibility studies and ab initio complete active space self-consistent field (CASSCF) calculations indicate that the magnetic coupling between the DyIII ions, which possess a high axial anisotropy in the ground state, is very weakly antiferromagnetic and mainly dipolar in nature. To redu…

LanthanideGadoliniumab initio calculationsOrganic Chemistrychemistry.chemical_elementGadoliniumGeneral ChemistryCatalysisCrystallographychemistryComputational chemistryAb initio quantum chemistry methodsMagnetic propertiesLanthanidesDysprosiumDysprosiumMoleculeGround stateta116Chemistry: A European Journal
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Layered gadolinium hydroxides for low-temperature magnetic cooling

2015

Layered gadolinium hydroxides have revealed to be excellent candidates for cryogenic magnetic refrigeration. These materials behave as pure 2D magnetic systems with a Heisenberg-Ising critical crossover, induced by dipolar interactions. This 2D character and the possibility offered by these materials to be delaminated open the possibility of rapid heat dissipation upon substrate deposition.

Materials scienceGadoliniumMetals and Alloyschemistry.chemical_elementNanotechnologyGeneral ChemistrySubstrate (electronics)Thermal management of electronic devices and systems7. Clean energyCatalysisSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsChemistryDipoleChemical engineeringchemistryMaterials ChemistryCeramics and CompositesMagnetic refrigerationDeposition (phase transition)Chemical Communications
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Single-molecule magnet behavior and magnetocaloric effect in ferromagnetically coupled LnIII-NiII-NiII-LnIII (LnIII = DyIII and GdIII) linear complex…

2014

New types of linear tetranuclear LnIII-NiII-NiII-LnIII (LnIII = Dy (1), Gd (2)) complexes have been prepared using the multidentate ligand N,N′-bis(3-methoxysalicylidene)-1,3-diaminobenzene, which has two sets of NO and OO′ coordination pockets that are able to selectively accommodate NiII and LnIII ions, respectively. The X-ray structure analysis reveals that the NiII ions are bridged by phenylenediimine groups forming a 12-membered metallacycle in the central body of the complex, whereas the LnIII ions are located at both sides of the metallacycle and linked to the NiII ions by diphenoxo bridging groups. Phenylenediimine and diphenoxo bridging groups transmit ferromagnetic exchange intera…

Inorganic ChemistryCrystallographyChemistryMagnetic refrigerationSingle-molecule magnetPhysical and Theoretical Chemistryta116
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Lanthanoid single-ion magnets based on polyoxometalates with a 5-fold symmetry: The series [LnP5W30O110]12– (Ln3+ = Tb, Dy, Ho, Er, Tm, and Yb)

2012

A robust, stable and processable family of mononuclear lanthanoid complexes based on polyoxometalates (POMs) that exhibit single-molecule magnetic behavior is described here. Preyssler polyanions of general formula [LnP 5W 30O 110] 12- (Ln 3+ = Tb, Dy, Ho, Er, Tm, and Yb) have been characterized with static and dynamic magnetic measurements and heat capacity experiments. For the Dy and Ho derivatives, slow relaxation of the magnetization has been found. A simple interpretation of these properties is achieved by using crystal field theory. © 2012 American Chemical Society.

LanthanideMagnetic measurementsSingle ionCondensed matter physicsChemistryGeneral ChemistryBiochemistryHeat capacityCatalysisMagnetizationCrystallographyColloid and Surface ChemistryCrystal field theoryMagnet
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ChemInform Abstract: Lanthanoid Single-Ion Magnets Based on Polyoxometalates with a 5-Fold Symmetry: The Series [LnP5W30O110]12-(Ln3+: Tb, Dy, Ho, Er…

2013

The compounds K12LnP5W30O110 ·nH2O (Ln3+: Tb, Dy, Ho, Er, Tm, and Yb) are prepared from aqueous solutions of K12.5Na1.5 [NaP5W30O110] and LnCl3 (autoclave, 160 °C, 24 h) and characterized by static and dynamic magnetic measurements.

LanthanideAqueous solutionSeries (mathematics)Single ionFold (higher-order function)ChemistryMagnetPhysical chemistryGeneral MedicineSymmetry (physics)AutoclaveChemInform
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CCDC 969288: Experimental Crystal Structure Determination

2014

Related Article: Mikko M. Hänninen, Antonio J. Mota, Daniel Aravena, Eliseo Ruiz, Reijo Sillanpää, Agustín Camón, Marco Evangelisti, Enrique Colacio|2014|Chem.-Eur.J.|20|8410|doi:10.1002/chem.201402392

Space GroupCrystallographybis(mu3-methoxy)-tris(mu2-22'-(((2-(morpholin-4-yl)ethyl)ammonio)dimethanediyl)bis(6-methoxy-4-methylphenolato))-tris(nitrate)-tri-dysprosium tetraphenylborate methanol solvate monohydrateCrystal SystemCrystal StructureCell ParametersExperimental 3D Coordinates
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CCDC 969290: Experimental Crystal Structure Determination

2014

Related Article: Mikko M. Hänninen, Antonio J. Mota, Daniel Aravena, Eliseo Ruiz, Reijo Sillanpää, Agustín Camón, Marco Evangelisti, Enrique Colacio|2014|Chem.-Eur.J.|20|8410|doi:10.1002/chem.201402392

Space GroupCrystallographybis(mu~3~-Methoxo)-tris(mu~2~-22'-(((2-(morpholin-4-yl)ethyl)ammonio)dimethanediyl)bis(6-methoxy-4-methylphenolato))-tris(nitrato)-tri-gadolinium tetraphenylborate methanol solvateCrystal SystemCrystal StructureCell ParametersExperimental 3D Coordinates
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CCDC 969289: Experimental Crystal Structure Determination

2014

Related Article: Mikko M. Hänninen, Antonio J. Mota, Daniel Aravena, Eliseo Ruiz, Reijo Sillanpää, Agustín Camón, Marco Evangelisti, Enrique Colacio|2014|Chem.-Eur.J.|20|8410|doi:10.1002/chem.201402392

Space GroupCrystallographyCrystal SystemCrystal Structurebis(mu3-methoxy)-tris(mu2-22'-(((2-(morpholin-4-yl)ethyl)ammonio)dimethanediyl)bis(6-methoxy-4-methylphenolato))-tris(nitrato)-tri-dysprosium hexakis(nitrato)-dysprosium methanol solvate hexahydrateCell ParametersExperimental 3D Coordinates
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CCDC 1048590: Experimental Crystal Structure Determination

2015

Related Article: Carlos Meseguer, Silvia Titos-Padilla, Mikko M. Hänninen, R. Navarrete, A. J. Mota, Marco Evangelisti, José Ruiz, Enrique Colacio|2014|Inorg.Chem.|53|12092|doi:10.1021/ic501915j

bis(mu-22'-(13-phenylenebis(nitrilomethylylidene))bis(6-methoxyphenolato))-(mu-nitrato)-pentakis(nitrato)-bis(acetonitrile)-aqua-di-gadolinium-di-nickel acetonitrile solvateSpace GroupCrystallographyCrystal SystemCrystal StructureCell ParametersExperimental 3D Coordinates
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CCDC 1048589: Experimental Crystal Structure Determination

2015

Related Article: Carlos Meseguer, Silvia Titos-Padilla, Mikko M. Hänninen, R. Navarrete, A. J. Mota, Marco Evangelisti, José Ruiz, Enrique Colacio|2014|Inorg.Chem.|53|12092|doi:10.1021/ic501915j

Space GroupCrystallographyCrystal SystemCrystal StructureCell ParametersExperimental 3D Coordinatesbis(mu-22'-(13-phenylenebis(nitrilomethylylidene))bis(6-methoxyphenolato))-hexakis(nitrato)-bis(acetonitrile)-diaqua-di-dysprosium-di-nickel acetonitrile solvate
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CCDC 969291: Experimental Crystal Structure Determination

2014

Related Article: Mikko M. Hänninen, Antonio J. Mota, Daniel Aravena, Eliseo Ruiz, Reijo Sillanpää, Agustín Camón, Marco Evangelisti, Enrique Colacio|2014|Chem.-Eur.J.|20|8410|doi:10.1002/chem.201402392

Space GroupCrystallographybis(mu~3~-methoxy)-tris(mu~2~-22'-(((2-(morpholin-4-yl)ethyl)ammonio)dimethanediyl)bis(6-methoxy-4-methylphenolato))-tris(nitrato)-tri-gadolinium hexakis(nitrato)-gadolinium unknown solvateCrystal SystemCrystal StructureCell ParametersExperimental 3D Coordinates
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CCDC 1833818: Experimental Crystal Structure Determination

2018

Related Article: Eirini Fotopoulou, Jose Martínez-Lillo, Milosz Siczek, Tadeusz Lis, Vassilis Tangoulis, Marco Evangelisti, Euan K. Brechin, Constantinos J. Milios|2018|Chem.Commun.|54|6153|doi:10.1039/C8CC02583E

Space GroupCrystallographyCrystal Systemcatena-[tetrakis(mu-2-methyl-2-(((2-oxidonaphthalen-1-yl)methylidene)amino)propanoato)-bis(methanol)-di-chromium(iii)-nickel(ii)]Crystal StructureCell ParametersExperimental 3D Coordinates
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