1,437 research outputs found
Spin degrees of freedom and flattening of the spectra of single-particle excitations in strongly correlated Fermi systems
The impact of long-range spin-spin correlations on the structure of a flat
portion in single-particle spectra , which emerges beyond the point,
where the Landau state loses its stability, is studied. We supplement the
well-known Nozieres model of a Fermi system with limited scalar long-range
forces by a similar long-range spin-dependent term and calculate the spectra
versus its strength . It is found that Nozieres results hold as long as
. However, with changing its sign, the spontaneous magnetization is
shown to arise at any nonzero . The increase of the strength is
demonstrated to result in shrinkage of the domain in momentum space, occupied
by the flat portion of , and, eventually, in its vanishing.Comment: 7 pages, 15 figure
Damping effects and the metal-insulator transition in the two-dimensional electron gas
The damping of single-particle degrees of freedom in strongly correlated
two-dimensional Fermi systems is analyzed. Suppression of the scattering
amplitude due to the damping effects is shown to play a key role in preserving
the validity of the Landau-Migdal quasiparticle picture in a region of a phase
transition, associated with the divergence of the quasiparticle effective mass.
The results of the analysis are applied to elucidate the behavior of the
conductivity of the two-dimensional dilute electron gas in the
density region where it undergoes a metal-insulator transition.Comment: 7 pages, 6 figures. Improved and slightly extended version: new
paragraph about Hall effect + new Fig.
Two Scenarios of the Quantum Critical Point
Two different scenarios of the quantum critical point (QCP), a
zero-temperature instability of the Landau state, related to the divergence of
the effective mass, are investigated. Flaws of the standard scenario of the
QCP, where this divergence is attributed to the occurrence of some second-order
phase transition, are demonstrated. Salient features of a different {\it
topological} scenario of the QCP, associated with the emergence of bifurcation
points in equation that ordinarily determines the Fermi
momentum, are analyzed. The topological scenario of the QCP is applied to
three-dimensional (3D) Fermi liquids with an attractive current-current
interaction.Comment: 6 pages, added new discussion and 2 figure
Mechanisms driving alteration of the Landau state in the vicinity of a second-order phase transition
The rearrangement of the Fermi surface of a homogeneous Fermi system upon
approach to a second-order phase transition is studied at zero temperature. The
analysis begins with an investigation of solutions of the equation
, a condition that ordinarily has the Fermi momentum as
a single root. The emergence of a bifurcation point in this equation is found
to trigger a qualitative alteration of the Landau state, well before the
collapse of the collective degree of freedom that is responsible for the
second-order transition. The competition between mechanisms that drive
rearrangement of the Landau quasiparticle distribution is explored, taking into
account the feedback of the rearrangement on the spectrum of critical
fluctuations. It is demonstrated that the transformation of the Landau state to
a new ground state may be viewed as a first-order phase transition.Comment: 16 pages, 10 figure
Rearrangement of the Fermi Surface of Dense Neutron Matter and Direct Urca Cooling of Neutron Stars
It is proposed that a rearrangement of single-particle degrees of freedom may
occur in a portion of the quantum fluid interior of a neutron star. Such a
rearrangement is associated with the pronounced softening of the spin-isospin
collective mode which, under increasing density, leads to pion condensation.
Arguments and estimates based on fundamental relations of many-body theory show
that one realization of this phenomenon could produce very rapid cooling of the
star via a direct nucelon Urca process displaying a dependence on
temperature.Comment: 8 pages, 2 figure
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