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We study the emergence of non-Fermi liquid on heterostructure interfaces where there exists an infinite number of critical boson modes in two spatial dimensions for the magnetic fluctuations. At the interface, the interfacial Dzyaloshinskii-Moriya interaction naturally emerges in the magnetic interactions due to the absence of the inversion symmetry. The interfacial Dzyaloshinskii-Moriya interaction gives rise to a degenerate contour for the low-energy bosonic modes in the momentum space, which simultaneously becomes critical approaching the magnetic phase transition. The presence of the critical boson contour leads to a divergence in the dynamical magnetic susceptibility. The itinerant electrons are scattered by the critical boson contour and develop non-Fermi liquid behaviors. With a self-consistent renormalization calculation, we uncover a prominent non-Fermi liquid behavior in the resistivity with a characteristic temperature scaling power. These results set another possibility for the boson-fermion coupled problems and the fermion criticality.
At certain quantum critical points in metals an entire Fermi surface may disappear. A crucial question is the nature of the electronic excitations at the critical point. Here we provide arguments showing that at such quantum critical points the Fermi
Heavy electron metals on the verge of a quantum phase transition to magnetism show a number of unusual non-fermi liquid properties which are poorly understood. This article discusses in a general way various theoretical aspects of this phase transiti
We construct examples of translationally invariant solvable models of strongly-correlated metals, composed of lattices of Sachdev-Ye-Kitaev dots with identical local interactions. These models display crossovers as a function of temperature into regi
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