2 research outputs found
Observation of light driven band structure via multi-band high harmonic spectroscopy
Intense light-matter interactions have revolutionized our ability to probe
and manipulate quantum systems at sub-femtosecond time scales, opening routes
to all-optical control of electronic currents in solids at petahertz rates.
Such control typically requires electric field amplitudes , when
the voltage drop across a lattice site becomes comparable to the characteristic
band gap energies. In this regime, intense light-matter interaction induces
significant modifications of electronic and optical properties, dramatically
modifying the crystal band structure. Yet, identifying and characterizing such
modifications remains an outstanding problem. As the oscillating electric field
changes within the driving field's cycle, does the band-structure follow, and
how can it be defined? Here we address this fundamental question, proposing
all-optical spectroscopy to probe laser-induced closing of the band-gap between
adjacent conduction bands. Our work reveals the link between nonlinear light
matter interactions in strongly driven crystals and the sub-cycle modifications
in their effective band structure
Evidence for two dimensional anisotropic Luttinger liquids at millikelvin temperatures
Abstract Interacting electrons in one dimension (1D) are governed by the Luttinger liquid (LL) theory in which excitations are fractionalized. Can a LL-like state emerge in a 2D system as a stable zero-temperature phase? This question is crucial in the study of non-Fermi liquids. A recent experiment identified twisted bilayer tungsten ditelluride (tWTe2) as a 2D host of LL-like physics at a few kelvins. Here we report evidence for a 2D anisotropic LL state down to 50 mK, spontaneously formed in tWTe2 with a twist angle of ~ 3o. While the system is metallic-like and nearly isotropic above 2 K, a dramatically enhanced electronic anisotropy develops in the millikelvin regime. In the anisotropic phase, we observe characteristics of a 2D LL phase including a power-law across-wire conductance and a zero-bias dip in the along-wire differential resistance. Our results represent a step forward in the search for stable LL physics beyond 1D