Search results for "Fermi"

showing 10 items of 1388 documents

Exploring the Potential of Short-Baseline Physics at Fermilab

2018

We study the capabilities of the short baseline neutrino program at Fermilab to probe the unitarity of the lepton mixing matrix. We find the sensitivity to be slightly better than the current one. Motivated by the future DUNE experiment, we have also analyzed the potential of an extra liquid Argon near detector in the LBNF beamline. Adding such a near detector to the DUNE setup will substantially improve the current sensitivity on non-unitarity. This would help to remove CP degeneracies due to the new complex phase present in the neutrino mixing matrix. We also study the sensitivity of our proposed setup to light sterile neutrinos for various configurations.

Sterile neutrinoParticle physicsmedicine.medical_specialtyPhysics::Instrumentation and DetectorsPontecorvo–Maki–Nakagawa–Sakata matrixFOS: Physical sciences01 natural sciencesPartícules (Física nuclear)High Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesmedicineMedical physicsFermilab010306 general physicsNeutrino oscillationBaseline (configuration management)PhysicsUnitarity010308 nuclear & particles physicsDetectorHigh Energy Physics::PhenomenologyHigh Energy Physics - PhenomenologyBeamlineHigh Energy Physics::ExperimentNeutrinoProceedings of The 20th International Workshop on Neutrinos — PoS(NuFACT2018)
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Detecting topology through dynamics in interacting fermionic wires

2020

We describe a protocol to read out the topological invariant of interacting 1D chiral models, based on measuring the mean chiral displacement of time-evolving bulk excitations. We present analytical calculations and numerical Matrix Product State simulations of interacting Su-Schrieffer-Heeger (SSH) chains, demonstrating how the mean chiral displacement allows to distinguish between topological insulator, trivial insulator and symmetry-broken phases. Finally, we provide an experimental blueprint for realizing a model displaying these three phases and describe how to detect those.

Strongly Correlated Electrons (cond-mat.str-el)business.industrymedia_common.quotation_subjectLibrary scienceFOS: Physical sciencesTopologyTopologiaCondensed Matter - Strongly Correlated ElectronsHospitalityDynamics (music)ExcellenceQuantum Gases (cond-mat.quant-gas):Física::Física de fluids::Física de gasos [Àrees temàtiques de la UPC]Center (algebra and category theory)ddc:530SociologyGasesFermionic wiresCondensed Matter - Quantum Gasesbusinessmedia_common
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Antiferromagnetism and the node structure of the superconducting order parameter of UPd Al

2000

The node structure of the superconducting order parameter of the heavy-fermion system is analyzed within the weak-coupling theory. A pairing interaction induced by the exchange of antiferromagnetic spin excitations is assumed as suggested by recent inelastic neutron scattering experiments and tunneling spectroscopy. The multi-sheeted Fermi surface is taken into account. Based on a model susceptibility for the simple antiferromagnetic structure of , line nodes result at the rim of the magnetic Brillouin zone.

SuperconductivityBrillouin zonePhysicsCondensed matter physicsPairingAntiferromagnetismCondensed Matter::Strongly Correlated ElectronsFermi surfaceCondensed Matter PhysicsMagnetic susceptibilityInelastic neutron scatteringElectronic Optical and Magnetic MaterialsSpin-½The European Physical Journal B
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Superconductivity in Nb21S8, a Phase with Metal Cluster Chains

1998

Phase pure samples of Nb21S8 are obtained by chemical transport and molten flux reactions in sealed niobium containers at 850−950 °C. In the temperature range from 5 to 290 K the electrical conductivity is found to be moderate metallic with a specific resistivity of 3.90 mΩ cm at 273 K. Magnetic susceptibility measurements give weak, almost temperature independent paramagnetism above ∼40 K. These metallic properties are compared with the structure of Nb21S8, which contains linear single and double chains of fused body centered niobium cubes, separated by S and additional Nb atoms. Both physical measurements consistently show a transition into the superconducting state below 4.1(5) and 3.7(2…

SuperconductivityCondensed matter physicsChemistryFermi levelNiobiumchemistry.chemical_elementGeneral ChemistryBiochemistryMagnetic susceptibilityCatalysissymbols.namesakeParamagnetismColloid and Surface ChemistryElectrical resistivity and conductivityPhase (matter)symbolsElectronic band structureJournal of the American Chemical Society
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Giant Negative Magnetoresistance in GdI2: Prediction and Realization

1999

The electronic structure of the layered d1 compound GdI2 has been examined systematically in view of its relation to other layered d1 systems including superconducting and isostructural 2H-TaS2 and 2H-NbSe2. A van Hove type instability is evident in suitable representations of the Fermi surface. The presence of the half-filled and magnetic 4f level should preclude the possibility of superconductivity. Instead GdI2 orders ferromagnetically at 290(5) K and displays large negative magnetoresistance ≈70% at 7 T close to room temperature. This finding provides support to the idea that materials can be searched rationally for interesting properties through high level electronic structure calculat…

SuperconductivityCondensed matter physicsMagnetoresistanceChemistryGiant magnetoresistanceFermi surfaceElectronic structureCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsInorganic ChemistryMaterials ChemistryCeramics and CompositesDensity of statesPhysical and Theoretical ChemistryMetal–insulator transitionElectronic band structureJournal of Solid State Chemistry
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Structure and superconductivity in LnNi2B2C: comparison of calculation and experiment

2001

Abstract The experimental relation between the superconducting transition temperature ( T c ) and lattice size for the lanthanide nickel borocarbides is clarified. The electronic density of states (DOS) at the Fermi energy is calculated by the LMTO method for selected non-magnetic lanthanides. The T c and the DOS are both shown to scale in the same way with a structural parameter that characterizes the bond angle in the NiB 4 tetrahedra. The results strongly support arguments that the suppression of superconductivity on going from smaller to larger lanthanides in the quaternary nickel borocarbides is structurally driven. A structure– T c relationship of this type is unusual for intermetalli…

SuperconductivityLanthanideCondensed matter physicsIntermetallicchemistry.chemical_elementFermi energyGeneral ChemistryCondensed Matter PhysicsCondensed Matter::Materials ScienceNickelMolecular geometryTight bindingchemistryCondensed Matter::SuperconductivityMaterials ChemistryTetrahedronCondensed Matter::Strongly Correlated ElectronsSolid State Communications
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Effect of pressure on superconductivity in NaAlSi

2012

The ternary superconductor NaAlSi, isostructural with LiFeAs, the ``111'' iron pnictide superconductor, is investigated under pressure. The structure remains stable up to 15 GPa. Resistivity and susceptibility measurements show an increase of ${T}_{c}$ up to 2 GPa, followed by a decrease until superconductivity disappears at 4.8 GPa. Band structure calculations show that pressure should have a negligible effect on the electronic structure and the Fermi surface and thus the disappearance of superconductivity under pressure must have a different origin. We compare the electronic structure of NaAlSi under pressure with that of nonsuperconducting isostructural NaAlGe.

SuperconductivityMaterials scienceCondensed matter physicsElectrical resistivity and conductivityFermi surfaceElectronic structureIsostructuralCondensed Matter PhysicsElectronic band structureTernary operationPnictogenElectronic Optical and Magnetic MaterialsPhysical Review B
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Microrefrigeration by NIS tunnel junctions

1996

By using a normal metal-insulator-superconductor (NIS) tunnel junction one can manipulate the Fermi-Dirac distribution of the electrons in the normal electrode. If the junction is biased close to the superconducting gap, Δ, only “hot electrons” above Fermi level can tunnel from the normal electrode to the superconductor. Thus, due to the decoupling of the conduction electrons from the lattice at low temperatures, there exists a possibility to decrease the electronic temperature by this method. Because of the symmetry with bias voltage, two NIS tunnel junctions in series can form an efficient microrefrigerator. Temperature can be measured with two additional junctions by considering the vari…

SuperconductivityMaterials scienceCondensed matter physicsFermi levelGeneral Physics and AstronomyBiasingElectronCondensed Matter::Mesoscopic Systems and Quantum Hall EffectThermal conductionsymbols.namesakeTunnel junctionCondensed Matter::SuperconductivityLattice (order)ElectrodesymbolsComputer Science::DatabasesCzechoslovak Journal of Physics
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Probing the superconducting state of UPd2Al3 thin films by tunneling spectroscopy

1997

Abstract Giaever-type planar cross junctions of thin films of the heavy fermion superconductor UPd2Al3 and counter-electrodes of Au, Ag and Al were prepared. Tunneling barriers consisting of the native oxide layer of UPd2Al3 and artificial barriers of AlOx and UOx were investigated. The junctions without artificial barrier show a lack of reproducebility. On some junctions a BCS-like tunneling conductivity with a ratio of 2Δ 0 /k B T c ⋍ 3.8 was observed. Using oxidized Al deposited at room temperature as a barrier no substantial increase of the junction resistance occured. With Uraniumoxide a much higher resistance was obtained, but an association of the bias dependent junction conductivity…

SuperconductivityMaterials scienceCondensed matter physicsOxideEnergy Engineering and Power TechnologyConductivityHeavy fermion superconductorCondensed Matter PhysicsElectronic Optical and Magnetic Materialschemistry.chemical_compoundchemistryDensity of statesElectrical and Electronic EngineeringThin filmSpectroscopyQuantum tunnellingPhysica C: Superconductivity
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Preparation of thin films of the heavy fermion superconductor UNi2Al3

2004

Abstract Thin films of the heavy fermion superconductor UNi 2 Al 3 were prepared by coevaporation of the elementary components in an MBE-system. We obtained textured (1 0 0)-oriented films of this hexagonal compound depositing on Al 2 O 3 substrates. Epitaxial growth was observed on (1 1 2)-oriented orthorhombical YAlO 3 substrates. However, due to pronounced strain the UNi 2 Al 3 (1 0 0)-axis is shortened by ≈2%. No superconductivity of the films was observed which can be associated with the high impurity concentration deduced from R ( T ) and XRD investigations.

SuperconductivityMaterials scienceCondensed matter physicsStrain (chemistry)ImpurityHexagonal crystal systemHeavy fermion superconductorThin filmCondensed Matter PhysicsEpitaxyElectronic Optical and Magnetic MaterialsJournal of Magnetism and Magnetic Materials
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