Search results for "Electron system"

showing 7 items of 17 documents

Pressure induced insulator/half-metal/metal transition in a strongly correlatedp-electron system

2012

Mixed-valent Rb${}_{4}$O${}_{6}$ provides an exceptional prototype material for studying the interplay between local correlations (Hubbard $U$) and electron kinetic energy ($W$) in the open $sp$-electron shell. Based on a first-principles calculation we show that depending on $U/W$ ratio, when tuned by external pressure, Rb${}_{4}$O${}_{6}$ exhibits a surprising sequence of phase transitions between strongly correlated antiferromagnetic insulator, ferromagnetic insulator ($U/W\phantom{\rule{-0.16em}{0ex}}\ensuremath{\gg}\phantom{\rule{-0.16em}{0ex}}1$), moderately correlated ferromagnetic half-metal ($U/W\phantom{\rule{-0.16em}{0ex}}\ensuremath{\sim}\phantom{\rule{-0.16em}{0ex}}1$), and fin…

PhysicsPhase transitionCondensed matter physicsCondensed Matter PhysicsElectron systemElectronic Optical and Magnetic MaterialsExternal pressureMetalFerromagnetismvisual_artvisual_art.visual_art_mediumAntiferromagnetismHalf-metalElectron kinetic energyPhysical Review B
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Role of excitons in double Raman resonances in GaAs quantum wells

1996

Raman scattering by longitudinal-optical phonons has been measured in GaAs-AlAs multiple quantum wells at high magnetic fields. Doubly resonant scattering processes are observed at photon energies corresponding to magneto-excitons with different principal quantum numbers for the incoming and outgoing channels. The existence of these initially forbidden scattering processes, their resonance energies, and their relative intensities are correctly reproduced by our theoretical description. The model takes into account the excitonic nature of the intermediate states, as well as scattering processes involving a nonzero in-plane phonon wave vector, which is required to allow inter-Landau level sca…

PhysicsPhonon scatteringCondensed matter physicsCondensed Matter::OtherScatteringScattering lengthCorrelated Electron Systems / High Field Magnet Laboratory (HFML)02 engineering and technologyCondensed Matter::Mesoscopic Systems and Quantum Hall Effect021001 nanoscience & nanotechnology01 natural sciencesScattering amplitudeCondensed Matter::Materials Sciencesymbols.namesakeX-ray Raman scattering0103 physical sciencesPrincipal quantum numbersymbolsScattering theoryAtomic physics010306 general physics0210 nano-technologyGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)Raman scatteringPhysical Review B
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New state of matter: heavy-fermion systems, quantum spin liquids, quasicrystals, cold gases, and high temperature superconductors

2018

We report on a new state of matter manifested by strongly correlated Fermi systems including various heavy-fermion (HF) metals, two-dimensional quantum liquids such as $\rm ^3He$ films, certain quasicrystals, and systems behaving as quantum spin liquids. Generically, these systems can be viewed as HF systems or HF compounds, in that they exhibit typical behavior of HF metals. At zero temperature, such systems can experience a so-called fermion-condensation quantum phase transition (FCQPT). Combining analytical considerations with arguments based entirely on experimental grounds we argue and demonstrate that the class of HF systems is characterized by universal scaling behavior of their ther…

Quantum phase transitionHigh-temperature superconductivityNon-Fermi liquid statesFOS: Physical sciencesQuantum phase transition01 natural sciencesNew state of matter010305 fluids & plasmaslaw.inventionQuantum spin liquidsSuperconductivity (cond-mat.supr-con)Condensed Matter - Strongly Correlated Electronslaw0103 physical sciencesGeneral Materials Science010306 general physicsQuantumSuperconductivityPhysicsFlat bandsCondensed matter physicsStrongly Correlated Electrons (cond-mat.str-el)Condensed Matter - SuperconductivityFermi surfaceStrongly correlated electron systemsFermionCondensed Matter PhysicsAtomic and Molecular Physics and OpticsHeavy fermionsHigh-Tc superconductivityCold gasesState of matterStrongly correlated materialQuasicrystals
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Protonation and rearrangement of the tricyclo[4.2.2.22,5]dodeca-3,7,9,11-tetraene scaffold

2006

The biplanemers 2a,b contain enol ether substructures, which permit facile protonations of the π electron system. The subsequent ether cleavage is characterized by rearrangements of the polycyclic scaffold of the carbenium ions or the electroneutral primary products. Apart from the expected products 3a and 5a, a series of unexpected ketones and diketones (4a′, 9b, 10b, 11b, and 12b) were obtained.

chemistry.chemical_classificationPrimary (chemistry)ChemistryStereochemistryOrganic ChemistryProtonationElectron systemBiochemistryMedicinal chemistryIonHydrolysisDrug DiscoveryEnol etherEther cleavageTetrahedron Letters
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ChemInform Abstract: Cycloaddition of Benzothiete and Electron-Deficient Nitriles.

2010

The o-quinoid 8π electron system 2, generated by thermal ring opening of benzothiete (1), enters regio-specific [8π + 2π] cycloaddition reactions with electron-deficient nitriles 3a-d, yielding the 4H-1,3-benzothiazines 4a-d. A competitive dimerization of 1 leads to 1,5-dibenzo[b,f]dithiocin (5). Depending on the nitrile further competitive or subsequent reactions (2 + 3b 7b, 2 + 3d 4d 8d) can occur. The cycloadducts 10e and 11e gained from 3e anticipate a primary cleavage of 3e to methylisothiocyanate 9e which reacts at the CN double bond as well as at the CS double bond.

chemistry.chemical_classificationchemistry.chemical_compoundDouble bondchemistryNitrileStereochemistryGeneral MedicineElectronCleavage (embryo)Electron systemRing (chemistry)Medicinal chemistryCycloadditionChemInform
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Cycloaddition of benzothiete and electron-deficient nitriles

1991

The o-quinoid 8π electron system 2, generated by thermal ring opening of benzothiete (1), enters regio-specific [8π + 2π] cycloaddition reactions with electron-deficient nitriles 3a-d, yielding the 4H-1,3-benzothiazines 4a-d. A competitive dimerization of 1 leads to 1,5-dibenzo[b,f]dithiocin (5). Depending on the nitrile further competitive or subsequent reactions (2 + 3b 7b, 2 + 3d 4d 8d) can occur. The cycloadducts 10e and 11e gained from 3e anticipate a primary cleavage of 3e to methylisothiocyanate 9e which reacts at the CN double bond as well as at the CS double bond.

chemistry.chemical_classificationchemistry.chemical_compoundNitrilechemistryDouble bondBicyclic moleculeOrganic ChemistryElectronCleavage (embryo)Electron systemRing (chemistry)Medicinal chemistryCycloadditionJournal of Heterocyclic Chemistry
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Magnetic quantum criticality in quasi-one-dimensional Heisenberg antiferromagnet Cu(C4H4N2)(NO3)2

2016

We analyze exciting recent measurements [Phys. Rev. Lett. 114 (2015) 037202] of the magnetization, differential susceptibility and specific heat on one dimensional Heisenberg antiferromagnet Cu(C4H4N2)(NO3)2 (CuPzN) subjected to strong magnetic fields. Using the mapping between magnons (bosons) in CuPzN and fermions, we demonstrate that magnetic field tunes the insulator towards quantum critical point related to so-called fermion condensation quantum phase transition (FCQPT) at which the resulting fermion effective mass diverges kinematically. We show that the FCQPT concept permits to reveal the scaling behavior of thermodynamic characteristics, describe the experimental results quantitativ…

non-fermi-liquid ground statesstrongly correlated electron systemsquasi-one-dimensional systemheavy fermionsspin chain modelsAnnalen Der Physik
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