Magneto-Optics of the Incompressible Fermi Liquid and the Wigner Solid

1992 ◽  
pp. 262-269
Author(s):  
N. J. Pulsford ◽  
I. V. Kukushkin
Keyword(s):  
Fermi Liquid ◽  
Wigner Solid

Magnetooptics of the incompressible Fermi liquid and of the Wigner solid

1992 ◽  
Vol 263 (1-3) ◽  
pp. 30-38 ◽  
Author(s):  
I.V. Kukushkin ◽  
N.J. Pulsford ◽  
K. von Klitzing ◽  
K. Ploog ◽  
V.B. Timofeev
Keyword(s):  
Fermi Liquid ◽  
Wigner Solid

Wigner solid versus incompressible Fermi liquid: phase diagram derived from time-resolved photoluminescence

1993 ◽  
Vol 184 (1-4) ◽  
pp. 38-42 ◽  
Author(s):  
I.V. Kukushkin ◽  
N.J. Pulsford ◽  
K. von Klitzing ◽  
R. Haug ◽  
K. Ploog ◽  
...  
Keyword(s):  
Phase Diagram ◽  
Liquid Phase ◽  
Fermi Liquid ◽  
Time Resolved ◽  
Wigner Solid ◽  
Time Resolved Photoluminescence

scholarly journals From the Fermi Liquid towards the Wigner Solid in Two Dimensions

2002 ◽  
pp. 263-307 ◽  
Author(s):  
Jean-Louis Pichard ◽  
Giuliano Benenti ◽  
Georgios Katomeris ◽  
Franck Selva ◽  
Xavier Waintal
Keyword(s):  
Fermi Liquid ◽  
Two Dimensions ◽  
Wigner Solid

Evidence for a threshold force for displacement transverse to current for 2-D Wigner solid in a disorder field

1999 ◽  
Vol 09 (PR10) ◽  
pp. Pr10-231-Pr10-231
Author(s):  
Perrucho ◽  
Gaal ◽  
B. Sas ◽  
C. Mellor ◽  
Harris ◽  
...  
Keyword(s):  
Wigner Solid ◽  
Threshold Force

scholarly journals Propagation of shear stress in strongly interacting metallic Fermi liquids enhances transmission of terahertz radiation

2021 ◽  
Vol 11 (1) ◽  
Author(s):  
D. Valentinis ◽  
J. Zaanen ◽  
D. van der Marel
Keyword(s):  
Shear Stress ◽  
Terahertz Radiation ◽  
Fermi Liquid ◽  
Zero Sound ◽  
Strongly Correlated Electron ◽  
Correlated Electron Systems ◽  
Correlated Electron ◽  
Collisionless Regime ◽  
Propagating Shear ◽  
Mass Enhancement

AbstractA highlight of Fermi-liquid phenomenology, as explored in neutral $$^3$$ 3 He, is the observation that in the collisionless regime shear stress propagates as if one is dealing with the transverse phonon of a solid. The existence of this “transverse zero sound” requires that the quasiparticle mass enhancement exceeds a critical value. Could such a propagating shear stress also exist in strongly correlated electron systems? Despite some noticeable differences with the neutral case in the Galilean continuum, we arrive at the verdict that transverse zero sound should be generic for mass enhancement higher than 3. We present an experimental setup that should be exquisitely sensitive in this regard: the transmission of terahertz radiation through a thin slab of heavy-fermion material will be strongly enhanced at low temperature and accompanied by giant oscillations, which reflect the interference between light itself and the “material photon” being the actual manifestation of transverse zero sound in the charged Fermi liquid.

scholarly journals Deformation of the Fermi surface of a spinless two-dimensional electron gas in presence of an anisotropic Coulomb interaction potential

2021 ◽  
Vol 11 (1) ◽  
Author(s):  
Orion Ciftja
Keyword(s):  
Fermi Surface ◽  
Coulomb Interaction ◽  
Interaction Potential ◽  
Fermi Liquid ◽  
Energy State ◽  
Electron Gas ◽  
Two Dimensional ◽  
Dimensional Electron ◽  
Two Dimensional Electron Gas ◽  
Dimensional Electron Gas

AbstractWe consider the stability of the circular Fermi surface of a two-dimensional electron gas system against an elliptical deformation induced by an anisotropic Coulomb interaction potential. We use the jellium approximation for the neutralizing background and treat the electrons as fully spin-polarized (spinless) particles with a constant isotropic (effective) mass. The anisotropic Coulomb interaction potential considered in this work is inspired from studies of two-dimensional electron gas systems in the quantum Hall regime. We use a Hartree–Fock procedure to obtain analytical results for two special Fermi liquid quantum electronic phases. The first one corresponds to a system with circular Fermi surface while the second one corresponds to a liquid anisotropic phase with a specific elliptical deformation of the Fermi surface that gives rise to the lowest possible potential energy of the system. The results obtained suggest that, for the most general situations, neither of these two Fermi liquid phases represent the lowest energy state of the system within the framework of the family of states considered in this work. The lowest energy phase is one with an optimal elliptical deformation whose specific value is determined by a complex interplay of many factors including the density of the system.

Sign in / Sign up

Export Citation Format

Share Document