Metal‐Insulator Transitions
2003
2,273 citations recorded by the source corpus.
Subfields: Atomic and Molecular Physics, and Optics, Condensed Matter Physics, Materials Chemistry
View Paper: https://www.semanticscholar.org/paper/3dda8eb70ad380d35604ba2a09e61e3f4c5c074d
Citations in the corpus
- Direct Probing of the Mott Crossover in the SU(N) Fermi-Hubbard Model (2015, background): “It explains a wide range of observed phenomena such as metal-to-insulator transitions and magnetic order, and is believed to capture the essential physics of d-wave superfluidity in high-temperature superconductors [1,2].”
- The Casimir force between real materials: Experiment and theory (2009, background): “…and intrinsic semiconductors characterized by a band gap of different width, Mott-Hubbard dielectrics and doped semiconductors with doping concentration below the critical value) have a zero value of the dc conductivity at zero temperature [see, e.g., Mott (1990), Shklovskii, Efros (1984)].”
- Electrodynamics of correlated electron materials (2011, background): “A violation of the so-called Mott or Ioffe-Regel condition means that ρ(T ) exceeds the upper limit fixed by the common understanding of a metal for which the mean free path ` should be larger than the atomic distance d (Ioffe and Regel, 1960; Mott, 1990).”
- Nonlinear light–matter interaction at terahertz frequencies (2016, background): “Such rotation indeed modifies the Mn-O-Mn bond angles, thus affecting the spatial overlap of the orbital wave functions along these bonds and controlling the sign of the exchange interactions [47,48].”
- Electronic instabilities of kagome metals: Saddle points and Landau theory (2021, background): “Two dimensional correlated metals based on transition metal ions are a classic subject for many body physics [1, 2], displaying diverse electronic phenomena such as unconventional superconductivity [3–5], charge and spin order [6, 7], nematicity [8, 9], strange metallic behavior [10–12], and more.”
- One dimensional bosons: From condensed matter systems to ultracold gases (2011, background): “If the system is in contact with a bath, an instanton calculation (Nattermann et al., 2003) leads back to Mott’s variable range hopping (Mott, 1990) σ(T ) ∼ e−(T0/T ) 1/2 .”