Search results for "Valence electron"

showing 10 items of 56 documents

Near band edge and defect emissions in wurtzite Cd0.025Mg0.10Zn0.875O nanocrystals

2021

Abstract We report on near band edge and local defects emissions in Cd0·025Mg0·10Zn0·875O (CdMgZnO) nanoparticles (NPs) as a function of temperature, where a strong temperature-dependent near-infrared emission around 1.7 eV (~730 nm) has been observed. The NPs were synthesized by a modified sol-gel method and were annealed at 750 °C after growing. The crystallographic parameters have been determined by 2-dimensional synchrotron x-ray diffraction (XRD) and conventional XRD analysis, confirming their growth within the wurtzite phase with a preferred orientation along the (101) plane and an apparent crystallite size of 52.72 ± 0.18 nm. This apparent crystallite size is consistent with the near…

Materials sciencePhotoluminescenceBand gapOrganic ChemistryAnalytical chemistry02 engineering and technology010402 general chemistry021001 nanoscience & nanotechnology01 natural sciencesAtomic and Molecular Physics and Optics0104 chemical sciencesElectronic Optical and Magnetic MaterialsInorganic ChemistryCrystalliteElectrical and Electronic EngineeringPhysical and Theoretical Chemistry0210 nano-technologyValence electronSpectroscopyElectronic band structureHigh-resolution transmission electron microscopySpectroscopyWurtzite crystal structureOptical Materials
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Are AuPdTM (T = Sc, Y and M = Al, Ga, In), Heusler Compounds Superconductors without Inversion Symmetry?

2019

Heusler compounds with 2:1:1 stoichiometry either have a centrosymmetric Cu 2 MnAl structure or an Li 2 AgSb structure without a centre of inversion. The centrosymmetry is always lost in quaternary Heusler compounds with 1:1:1:1 stoichiometry and LiMgPdSn structure. This presents the possibility of realizing non-centrosymmetric superconductors in the family of Heusler compounds. The objective of this study is to search for and investigate such quaternary derivatives of Heusler compounds, particularly with respect to superconductivity. Several compounds were identified by carrying out calculations from first principles and superconductivity was observed in experiments conducted on AuPdScAl a…

Materials sciencePoint reflection02 engineering and technologyElectronic structureCentrosymmetry01 natural scienceslcsh:TechnologyArticlenon-centrosymmetric0103 physical sciencesGeneral Materials Science010306 general physicslcsh:Microscopylcsh:QC120-168.85Superconductivitylcsh:QH201-278.5lcsh:Tsuperconductivity021001 nanoscience & nanotechnologyelectronic structureCrystallographylcsh:TA1-2040lcsh:Descriptive and experimental mechanicslcsh:Electrical engineering. Electronics. Nuclear engineering0210 nano-technologyValence electronlcsh:Engineering (General). Civil engineering (General)Heusler compoundslcsh:TK1-9971StoichiometryMaterials
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Half-metallic compensated ferrimagnetism with a tunable compensation point over a wide temperature range in the Mn-Fe-V-Al Heusler system

2017

The cubic Heusler compound Mn1.5FeV0.5Al with the L21 Heusler structure is the first fully compensated half-metallic ferrimagnet with 24 valence electrons. The ferrimagnetic state can be tuned by changing the composition such that the compensation point appears at finite temperatures ranging from 0 K up to 226 K, while retaining half-metallicity in the system. In this paper, the structural, magnetic and transport properties of the Mn-Fe-V-Al system are discussed. Magnetic reversal and a change of sign of the anomalous Hall effect were observed at the compensation point, which gives rise to a sublattice spin-crossing. These materials present new possibilities for potential spintronic devices…

Materials scienceSpintronicsCondensed matter physicsGeneral Physics and Astronomy02 engineering and technologyengineering.materialAtmospheric temperature range021001 nanoscience & nanotechnologyHeusler compound01 natural scienceslcsh:QC1-999Compensation (engineering)Geomagnetic reversalCondensed Matter::Materials ScienceHall effectFerrimagnetism0103 physical sciencesengineeringCondensed Matter::Strongly Correlated Electrons010306 general physics0210 nano-technologyValence electronlcsh:PhysicsAIP Advances
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Isolation of a perfectly linear uranium(II) metallocene

2020

Reduction of the uranium(III) metallocene [(eta(5)-(C5Pr5)-Pr-i)(2)UI] (1) with potassium graphite produces the "second-generation" uranocene [(eta(5)-(C5Pr5)-Pr-i)(2)U] (2), which contains uranium in the formal divalent oxidation state. The geometry of 2 is that of a perfectly linear bis(cyclopentadienyl) sandwich complex, with the ground-state valence electron configuration of uranium(II) revealed by electronic spectroscopy and density functional theory to be 5f(3) 6d(1). Appreciable covalent contributions to the metal-ligand bonds were determined from a computational study of 2, including participation from the uranium 5f and 6d orbitals. Whereas three unpaired electrons in 2 occupy orbi…

Materials sciencemagneettiset ominaisuudetchemistry.chemical_elementorganometalliyhdisteet010402 general chemistry01 natural sciencesElectron spectroscopyCatalysisuraniumchemistry.chemical_compoundkemialliset sidoksetUranoceneCyclopentadienyl complex010405 organic chemistrychemical bondingGeneral MedicineGeneral ChemistryUraniummetalloceneselectronic structure0104 chemical sciencesCrystallographychemistryUnpaired electronuraaniDensity functional theorymagnetic propertiesQD0146Valence electronMetallocene
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15. Spectroscopic methods applied to zircon

2003

Natural and synthetic (pure and doped) zircon (ZrSiO4) have been studied with a variety of spectroscopic techniques. These techniques are based on different physical phenomena, for instance transitions between spin states of nuclei and electrons, energetic transitions of valence electrons, intra-molecular vibrations, or vibrations of atoms and molecular units in the lattice. All of the diverse spectroscopic techniques, however, have in common that they probe energy differences between a ground and excited states, mostly upon interaction of the mineral with incident radiation. Such interactions are not only determined by the excited elementary particles or molecules themselves but depend gre…

MetamictizationMaterials scienceValence (chemistry)Spin statesExcited stateElectronValence electronMolecular physicsZirconCharacterization (materials science)
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Measurement of the first ionization potential of lawrencium (element 103)

2015

Lawrencium, with atomic number 103, has an isotope with a half-life of 27 seconds; even so, its first ionization potential has now been measured on an atom-at-a-time scale and agrees well with state-of-the-art theoretical calculations that include relativistic effects. The most dramatic modern revision of Mendeleev's periodic table of elements came in 1944 when Glenn T. Seaborg placed a new series of elements, the actinides (atomic numbers 89–103), below the lanthanides. In this issue of Nature, Yuichiro Nagame and colleagues report the first measurement of one of the basic atomic properties of element 103 (lawrencium), namely its first ionization potential. Lawrencium is only accessible vi…

MultidisciplinaryChemistryPeriodic trendsAtomchemistry.chemical_elementTransactinide elementAtomic numberElectron configurationAtomic physicsRelativistic quantum chemistryValence electronChemical Physics and ChemistryLawrencium
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Chemical investigation of hassium (element 108).

2002

The periodic table provides a classification of the chemical properties of the elements. But for the heaviest elements, the transactinides, this role of the periodic table reaches its limits because increasingly strong relativistic effects on the valence electron shells can induce deviations from known trends in chemical properties. In the case of the first two transactinides, elements 104 and 105, relativistic effects do indeed influence their chemical properties, whereas elements 106 and 107 both behave as expected from their position within the periodic table. Here we report the chemical separation and characterization of only seven detected atoms of element 108 (hassium, Hs), which were…

MultidisciplinarychemistryGroup (periodic table)RutherfordiumAnalytical chemistryOsmium oxidechemistry.chemical_elementTransactinide elementNanotechnologyOsmiumValence electronRelativistic quantum chemistryHassiumNature
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Local suppression of collectivity in theN=80isotones at theZ=58subshell closure

2013

) transition strengths [1] and thenumber of nucleons in the valence shell. The global behaviorof these quantities between the major shells as a function ofthe nucleon number is well understood in the frameworks ofboth collective and microscopic models. One could expect thatthese general trends in the collective properties between themajorshellsaremodulated bythesubshellstructure.However,it is usually thought that the pairing correlations with anenergy scale of about 2 MeV, smear out and dissolve thesubshell structure as long as the separation energies betweenthe subshells are only about a few hundred keV.The recently observed evolution of the isovectorquadrupole-collective valence-shell exc…

Nuclear physicsMass numberPhysicsNuclear and High Energy PhysicsPairingNuclear TheoryPhysics::Atomic and Molecular ClustersClosure (topology)NucleonValence electronPhysical Review C
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Measurement of the first ionization potential of astatine by laser ionization spectroscopy

2013

The radioactive element astatine exists only in trace amounts in nature. Its properties can therefore only be explored by study of the minute quantities of artificially produced isotopes or by performing theoretical calculations. One of the most important properties influencing the chemical behaviour is the energy required to remove one electron from the valence shell, referred to as the ionization potential. Here we use laser spectroscopy to probe the optical spectrum of astatine near the ionization threshold. The observed series of Rydberg states enabled the first determination of the ionization potential of the astatine atom, 9.31751(8) eV. New ab initio calculations are performed to sup…

Other Fields of PhysicsGeneral Physics and Astronomychemistry.chemical_element7. Clean energy01 natural sciencesGeneral Biochemistry Genetics and Molecular BiologyArticlePhysics in GeneralAb initio quantum chemistry methodsCHEMISTRYIonization0103 physical sciencesAtomPhysics::Atomic and Molecular ClustersFACILITYPhysics::Atomic Physics010306 general physicsAstatineSpectroscopyPhysicsMultidisciplinary010308 nuclear & particles physicsGeneral ChemistryION-SOURCEIon source3. Good healthchemistry13. Climate actionIonization energyAtomic physicsValence electronNature Communications
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Optical phonons in theNaTiSi2O6oxide withS=12spin chains

2005

. The infrared-active phonon frequencies are obtained by Kramers-Kronig analy-sis of the reflectivity data. The assignment of the observed modes is done using lattice dynamical calculationsbased on the valence shell model. A phase transition at about 210 K is manifested through a dramatic changeof the mode frequency and broadening, and the appearance of new phonon modes. Analyzing the phononfrequency and damping vs temperature we have found that the phase transition leaves a fingerprint in thephonon dynamics of NaTiSi

Phase transitionMaterials scienceCondensed matter physicsPhononOxide02 engineering and technology021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciencesElectronic Optical and Magnetic Materialschemistry.chemical_compoundchemistryLattice (order)0103 physical sciences010306 general physics0210 nano-technologyValence electronPhysical Review B
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