Universal signatures of Majorana-like quasiparticles in strongly correlated Landau-Fermi liquids.

Motivated by recent experiments in the Kitaev honeycomb lattice, Kondo insulators, and the 'Luttinger's theorem-violating' Fermi liquid phase of the underdoped cuprates, we extend the theoretical machinery of Landau-Fermi liquid theory to a system of itinerant, interacting Majorana-like particles. Building upon a previously introduced model of 'nearly self-conjugate' fermionic polarons, a Landau-Majorana kinetic equation is introduced to describe the collective modes and Fermi surface instabilities in a fluid of particles whose fermionic degrees of freedom obey the Majorana reality condition. At large screening, we show that the Landau-Majorana liquid harbors a Lifshitz transition for specific values of the driving frequency.

Unconventional Hund metal in a weak itinerant ferromagnet.

The physics of weak itinerant ferromagnets is challenging due to their small magnetic moments and the ambiguous role of local interactions governing their electronic properties, many of which violate Fermi-liquid theory. While magnetic fluctuations play an important role in the materials' unusual electronic states, the nature of these fluctuations and the paradigms through which they arise remain debated. Here we use inelastic neutron scattering to study magnetic fluctuations in the canonical weak itinerant ferromagnet MnSi.

Atypical behavior of collective modes in two-dimensional Fermi liquids.

Using the Landau kinetic equation to study the non-equilibrium behavior of interacting Fermi systems is one of the crowning achievements of Landau's Fermi liquid theory. While thorough study of transport modes has been done for standard three-dimensional Fermi liquids, an equally in-depth analysis for two dimensional Fermi liquids is lacking. In applying the Landau kinetic equation (LKE) to a two-dimensional Fermi liquid, we obtain unconventional behavior of the zero sound mode.

Consequences of the inherent density dependence in one dimensional Dirac materials.

Dirac materials are systems in which the dispersion is linear in the vicinity of the Dirac points. As a consequence of this linear dispersion, the Fermi velocity is independent of density and these systems exhibit unusual behavior and possess unique physical properties that are of considerable interest. In this work we study the ground state behavior of 1D Dirac materials in two ways.

Acoustic attenuation probe for Fermion superfluidity in ultracold-atom gases.

Dilute gas Bose-Einstein condensates (BEC's), currently used to cool fermionic atoms in atom traps, can also probe the superfluidity of these fermions. The damping rate of BEC-acoustic excitations (phonon modes), measured in the middle of the trap as a function of the phonon momentum, yields an unambiguous signature of BCS-like superfluidity, provides a measurement of the superfluid gap parameter, and gives an estimate of the size of the Cooper pairs in the BEC-BCS crossover regime. We also predict kinks in the momentum dependence of the damping rate which can reveal detailed information about the fermion quasiparticle dispersion relation.

Spin waves in quasiequilibrium spin systems.

Using the Landau Fermi liquid theory we discovered a new propagating transverse spin wave in a paramagnetic system which is driven slightly out of equilibrium without applying an external magnetic field. We find a gapless mode which describes the uniform precession of the magnetization in the absence of a magnetic field. We also find a gapped mode associated with the precession of the spin current around the internal field.

Coexistence of superconductivity and ferromagnetism in ferromagnetic metals.

We address the question of coexistence of superconductivity and ferromagnetism. Using a field theoretical approach we study a one-fermion effective model of a ferromagnetic superconductor in which the quasiparticles responsible for the ferromagnetism form the Cooper pairs as well. For the first time we solve self-consistently the mean-field equations for the superconducting gap and the spontaneous magnetization.

Atrial natriuretic peptide blocks the renal vasoconstrictor response to hypertonic saline in the dog.

The role of atrial natriuretic peptide to modulate the renal tubuloglomerular feedback response was examined in the dehydrated anesthetized dog using an infusion of hypertonic sodium chloride to increase renal plasma sodium concentration by 30 mEq/l as the stimulus to activate the tubuloglomerular feedback. Two sequential infusions of hypertonic sodium chloride into the renal artery for 10 min were separated by 90 min, and various interventions were introduced before the second hypertonic saline infusion. In the first group of dogs, the first infusion of hypertonic saline resulted in a significant decrease in renal blood flow from 234 +/- 36 to 199 +/- 31 ml/min, but when atriopeptin III (APIII) was infused into the renal artery at 3 x 10(-10) mol/min, the repeat infusion of hypertonic saline resulted in a significant increase in blood flow from 221 +/- 28 to 269 +/- 35 ml/min that was maintained throughout the 10 min of hypertonic saline.