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11 relations: Critical field, Crystal structure, Cuprate superconductor, Fulde–Ferrell–Larkin–Ovchinnikov phase, Heavy fermion material, Heavy fermion superconductor, Inelastic neutron scattering, Quantum critical point, Scanning tunneling microscope, Scanning tunneling spectroscopy, Single crystal.
Critical field
Superconductivity is characterized both by perfect conductivity (zero resistance) and by the expulsion of magnetic fields (the Meissner effect).
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Crystal structure
In crystallography, crystal structure is a description of the ordered arrangement of atoms, ions or molecules in a crystalline material.
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Cuprate superconductor
Interest in cuprates sharply increased in 1986 with the discovery of high-temperature superconductivity in the Non-stoichiometric cuprate lanthanum barium copper oxide La2−xBaxCuO4.
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Fulde–Ferrell–Larkin–Ovchinnikov phase
The Fulde–Ferrell–Larkin–Ovchinnikov (FFLO) phase can arise in a superconductor in large magnetic field.
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Heavy fermion material
In solid-state physics, heavy fermion materials are a specific type of intermetallic compound, containing elements with 4f or 5f electrons in unfilled electron bands.
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Heavy fermion superconductor
Heavy fermion superconductors are a type of unconventional superconductor.
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Inelastic neutron scattering
Inelastic neutron scattering is an experimental technique commonly used in condensed matter research to study atomic and molecular motion as well as magnetic and crystal field excitations.
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Quantum critical point
A quantum critical point is a point in the phase diagram of a material where a continuous phase transition takes place at absolute zero.
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Scanning tunneling microscope
A scanning tunneling microscope (STM) is an instrument for imaging surfaces at the atomic level.
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Scanning tunneling spectroscopy
Scanning tunneling spectroscopy (STS), an extension of scanning tunneling microscopy (STM), is used to provide information about the density of electrons in a sample as a function of their energy.
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Single crystal
A single crystal or monocrystalline solid is a material in which the crystal lattice of the entire sample is continuous and unbroken to the edges of the sample, with no grain boundaries.
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