Search results for "CONDENSED MATTER"

showing 10 items of 13918 documents

Thermal, Pressure and Light Induced Spin Transition in the Two-Dimensional Coordination Polymer [Fe(pmd)2[Cu(CN)2]2]

2008

[EN] A complete structural, calorimetric, and magnetic characterisation of the 2D coordination spin crossover polymer {Fe(pmd)(2)[Cu(CN)(2)](2)} is reported. The crystal structure has been investigated below room temperature at 180 K and 90 K, and at 30 K after irradiating the sample at low temperature with green light ( lambda = 532 nm). The volume cell contraction through the thermal spin transition is only 18 angstrom(3) which is lower than the usually observed value of around 25-30 angstrom(3) while the average Fe-N bond distances decrease by the typical value of about 0.19 angstrom. The structural data of the irradiated state indicate that the high spin state is well induced since the …

chemistry.chemical_classificationSpin statesCondensed matter physicsCoordination polymerSpin transitionThermodynamicsCrystal structurePolymerInorganic Chemistrychemistry.chemical_compoundchemistrySpin crossoverFISICA APLICADAThermalIrradiation
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Pressure-induced cooperative spin transition in ironII 2D coordination polymers: room-temperature visible spectroscopic study.

2011

For the 2D coordination polymers [Fe(3-Fpy)(2)M(II)(CN)(4)] (M(II) = Ni, Pd, Pt), the pressure-induced spin crossover behavior has been investigated at 298 K by monitoring the distinct optical properties associated with each spin state. Cooperative first-order spin transition characterized by a piezohysteresis loop ca. 0.1 GPa wide was observed for the three derivatives. Application of the mean field regular solution theory has enabled estimation of the cooperative parameter, Γ(p), and the enthalpy, ΔH(HL)(p), associated with the spin transition for each derivative. These values, found in the intervals 6.8-7.9 and 18.6-20.8 kJ mol(-1), respectively, are consistent with those previously repo…

chemistry.chemical_classificationSpin statesCondensed matter physicsEnthalpySpin transitionElastic energyPolymerSurfaces Coatings and FilmschemistryMean field theorySpin crossoverMaterials ChemistryPhysical chemistryPhysical and Theoretical ChemistrySpin-½The journal of physical chemistry. B
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Anisotropic Effect after Stretching of the Spin-Crossover Compound [Fe(II)(2,6-bis-(benzimidazol-2′-yl)pyridine)2] (C1O4)2 in Polyvinylalcohol Polyme…

1999

Abstract [Fe(II)(2,6-bis-(benzimidazol-2′-yl)-pyridine)2](C1O4)2 diffused into a poly(vinyl)alcohol polymer matrix, exhibits an thermally induced spin-crossover. After stretching the matrix, the compound orients itself in the matrix. Polarised UV/VIS spectra measured parallel and perpendicular to the stretching direction allowed to calculate the distortion of the molecule in the matrix by means of semi-empirical PPP SCF-CI calculations.

chemistry.chemical_classificationSpin statesStereochemistryPolymerCondensed Matter Physicschemistry.chemical_compoundCrystallographyMatrix (mathematics)chemistrySpin crossoverPyridinePerpendicularMoleculePhysics::Chemical PhysicsAnisotropyMolecular Crystals and Liquid Crystals Science and Technology. Section A. Molecular Crystals and Liquid Crystals
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Experimental studies of the rheological behavior of a demixing biopolymeric sol

1995

Experimental data are presented concerning a large transient viscosity surge occurring in the course of spinodal demixing of agarose aqueous solutions. The study includes the effects of water perturbation by minor proportions of compatible cosolutes. Three observations are noteworthy. One concerns an upward or downward shift of the spinodal temperature, caused by cosolutes, which agrees with their expected modulation of solvent-induced forces. The second concerns the time of appearance of the viscosity surge. This is observed to follow a critical law, with an exponent independent of polymer concentration and solvent perturbation. The third concerns the inverse-power-law dependence of the vi…

chemistry.chemical_classificationSpinodalMaterials scienceAqueous solutionSpinodal decompositionPerturbation (astronomy)Concentration effectThermodynamicsPolymerCondensed Matter PhysicsCondensed Matter::Soft Condensed MatterRheologychemistryExponentInternational Journal of Thermophysics
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Structural study of NaNdGa4S8, a luminescent material with low-concentration quenching

1988

Abstract Single-crystal X-ray diffraction analysis and optical investigations of NaNdGa 4 S 8 show that Nd 3+ ions are essentially distributed in two of the three square antiprismatic sites of a CaGa 2 S 4 -type lattice. The NdS 8 polyhedra are isolated (minimum NdNd distance: 6.07 A) so the interactions responsible for concentration quenching of the luminescence are considerably reduced

chemistry.chemical_classificationSquare antiprismatic molecular geometryChemistryInorganic chemistryCrystal structureCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsIonInorganic ChemistryBond lengthCrystallographyMolecular geometryX-ray crystallographyMaterials ChemistryCeramics and CompositesPhysical and Theoretical ChemistryLuminescenceInorganic compoundJournal of Solid State Chemistry
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Discrete bond model (DBM) of sodium silicate glasses derived from XPS, Raman and NMR measurements

1993

In sodium silicate glasses, the fraction of differently bound Si species Q[i] (i = 0−4), depending on the number i of bridging oxygens bound to the quarternary silicon, is a function of stoichiometry and the Na/Si ratio. Sodium silicate glasses were investigated by high resolution X-ray photoelectron spectroscopy. To explain the differences in chemical shifts and linewidths of the O 1s signal of the bridging and the non-bridging oxygen as a function of alkali concentration, and extended glass model was developed. This new model takes into account the influence of the alkali concentration on the Q[i] distribution and on the appearance and concentrations of differently bound bridging oxygens …

chemistry.chemical_classificationStereochemistryChemical shiftBinding energyCondensed Matter PhysicsAlkali metalElectronic Optical and Magnetic Materialssymbols.namesakeCrystallographychemistryX-ray photoelectron spectroscopyChemical bondMaterials ChemistryCeramics and CompositessymbolsRaman spectroscopyInorganic compoundStoichiometryJournal of Non-Crystalline Solids
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Structure of 5,17-dimethyl-11,23-dioctylcalix[4]arene

1991

The title compound C46O4H60 crystallizes in the triclinic space group, P¯1, witha=11.584(2),b=16.261(2),c=11.172(1) A,α=103.15(8),β=95.68(1),γ=96.85(1)°. The structure was solved by direct methods, and refined by weighted full-matrix least squares toR=0.097. This is the second calix[4]arene with two different alkyl substituents atpara positions of the phenolic rings. The macrocycle adopts the cone conformation. Interactions CH3-π are established between two calixarenes related by a center of symmetry. Comparisons are made between the conformation of this molecule and that of symmetrically substituted calix[4]arenes.

chemistry.chemical_classificationStereochemistryChemistryGeneral ChemistryNuclear magnetic resonance spectroscopyCrystal structureTriclinic crystal systemCondensed Matter Physicschemistry.chemical_compoundCrystallographyStructural BiologyX-ray crystallographyCalixareneMoleculeSpectroscopyAlkylOrganometallic chemistryJournal of Crystallographic and Spectroscopic Research
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Postsynthetic Approach for the Rational Design of Chiral Ferroelectric Metal–Organic Frameworks

2017

International audience; Ferroelectrics (FEs) are materials of paramount importance with a wide diversity of applications. Herein, we propose a postsynthetic methodology for the smart implementation of ferroelectricity in chiral metal−organic frameworks (MOFs): following a single-crystal to single-crystal cation metathesis, the Ca2+ counterions of a preformed chiral MOF of formula Ca6II{CuII24[(S,S)-hismox]12(OH2)3}·212H2O (1), where hismox is a chiral ligand derived from the natural amino acid l-histidine, are replaced by CH3NH3+. The resulting compound, (CH3NH3)12{CuII24[(S,S)-hismox]12(OH2)3}·178H2O (2), retains the polar space group of 1 and is ferroelectric below 260 K. These results op…

chemistry.chemical_classificationStereochemistryChiral ligandRational design02 engineering and technologyGeneral Chemistry010402 general chemistry021001 nanoscience & nanotechnologyMetathesis01 natural sciencesBiochemistryFerroelectricityCatalysis0104 chemical sciencesCrystallographyColloid and Surface Chemistrychemistry[PHYS.COND.CM-MS]Physics [physics]/Condensed Matter [cond-mat]/Materials Science [cond-mat.mtrl-sci]Metal-organic frameworkCounterion0210 nano-technology
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Effect of Protonated Organic Cations and Anion−π Interactions on the Magnetic Behavior of Hexabromorhenate(IV) Salts

2015

Two novel Re-IV compounds of formula (Hbpym)(2)[(ReBr6)-Br-IV]center dot 4H(2)O (1) and (H(4)biim)[(ReBr6)-Br-IV]center dot 4H(2)O (2) [Hbpym(+) = 2,2'-bipyrimidinium cation and H(4)biim(2+) = 2,2'-biimidazolium dication] have been prepared and magnetostructurally characterized. 1 and 2 exhibit distinct crystal packing, and the presence of weak intermolecular contacts, such as Re-Br...B-rRe (1 and 2), Re-Br center dot center dot center dot(H2O)center dot center dot center dot BrRe (1 and 2), and Re-Br center dot center dot center dot pi center dot center dot center dot Br-Re (2), lead to different magnetic behaviors. While 1 is antiferromagnetic, 2 is a ferromagnetic compound and indeed the…

chemistry.chemical_classificationStereochemistryIntermolecular forceSalt (chemistry)ProtonationGeneral ChemistryCondensed Matter Physics3. Good healthDicationIonCrystalCrystallographychemistryFerromagnetismAntiferromagnetismCOMPLEXESGeneral Materials ScienceX-RAY-STRUCTURECrystal Growth & Design
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Radical cation salts based on BEDT-TTF and the paramagnetic anion [Cr(NCS)6]3−

1999

Abstract A new radical cation salt formulated as (ET)5.5[Cr(NCS)6] (ET = BEDT-TTF = bis(ethylene)dithiotetrathiafulvalene) has been synthesised and characterised by X-ray diffraction and magnetic measurements. The structure shows the presence of alternating layers of the ET units and mixed layers of anions and an isolated ET molecule. The magnetic susceptibility data in the temperature range 2–300 K show a Curie law with C = 1.771 cm3.K.mol−1 and Nα = 1.20.10−5 cm3.mol−1, in agreement with the presence of isolated Cr(III) without any contribution from the organic part.

chemistry.chemical_classificationStereochemistryMechanical EngineeringMetals and AlloysSalt (chemistry)Atmospheric temperature rangeCondensed Matter PhysicsMagnetic susceptibilityElectronic Optical and Magnetic MaterialsIonParamagnetismCurie's lawCrystallographychemistryRadical ionMechanics of MaterialsMaterials ChemistryMoleculeSynthetic Metals
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