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Insulating Phase sentence examples within twisted bilayer graphene
Magic-angle twisted bilayer graphene (MATBG)4–8 has recently emerged as a versatile platform that combines metallic, superconducting, magnetic and insulating phases in a single crystal9–14.
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An important nonperturbative finding is a remarkable fine-tuning effect of the precise lattice commensuration, where slight variations in the relative lattice periods may lead to a suppression of the correlated insulating phase, in qualitative agreement with the observed fragility of the correlated insulating phase in twisted bilayer graphene.
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Insulating Phase sentence examples within metal insulator transition
A systematic study of various metal-insulator transition (MIT) associated phases of VO2, including metallic R phase and insulating phases (T, M1, M2), is required to uncover the physics of MIT and trigger their promising applications.
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Vanadium dioxide (VO2) is a typical metal-insulator transition (MIT) material, which changes from room-temperature monoclinic insulating phase to high-temperature rutile metallic phase.
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Insulating Phase sentence examples within Topological Insulating Phase
Under different choices of gauge fields in either the Abelian or the non-Abelian regime, both weak and strong topological insulating phases are identified in the model.
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The realization of multifunctional two-dimensional (2D) materials is fundamentally intriguing, such as the combination of piezoelectricity with a topological insulating phase in Janus monolayer SrAlGaSe4.
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Insulating Phase sentence examples within Mott Insulating Phase
Our simulations reveal a magnetic phase transition from a ferromagnetic-order to a spin insulator inside the Mott insulating phase with two particles per site for quasi-balanced on-site inter- and intra-particle interactions, i.
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Above this interaction strength, a transition to the Mott insulating phase occurs, and the twisted boundary states disappear.
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Insulating Phase sentence examples within Hall Insulating Phase
This thesis also contains a brief overview of the current experimental situation surrounding this field of study as well as a short review of the Kane-Mele model as an example model featuring a quantum spin Hall insulating phase including spin-helical topological edge states.
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Our results are based on density functional theory and low-energy effective model calculations and strongly suggest that bilayers of TMDs are highly suitable platforms for direct observation of the orbital Hall insulating phase in two-dimensional materials.
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Insulating Phase sentence examples within Distinct Insulating Phase
We compute the time-averaged (annealed) conductance in the insulating regime and find three distinct insulating phases, separated by two transitions.
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We demonstrate that by tailoring the magnetization and interlayer electron hopping, a rich three-dimensional topological phase diagram can be established, including three types of topologically distinct insulating phases bridged by Weyl semimetals, and can be directly mapped to realistic materials such as MnBi2Te4/(Bi2Te3)n systems.
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Insulating Phase sentence examples within Correlated Insulating Phase
An important nonperturbative finding is a remarkable fine-tuning effect of the precise lattice commensuration, where slight variations in the relative lattice periods may lead to a suppression of the correlated insulating phase, in qualitative agreement with the observed fragility of the correlated insulating phase in twisted bilayer graphene.
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As the interaction strength increases, a sequence of different correlated insulating phases emerge, including a quantum valley Hall state with topological edge states, an intervalley-coherent insulator, and a valence bond solid.
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Insulating Phase sentence examples within Chern Insulating Phase
However, we also find several gapless Weyl points, separating the non-equivalent Chern insulating phases, tuned by the ratio of the interlayer coupling Jc and the third-neighbour Heisenberg interaction J3.
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Such an out-of-plane orbital magnetization allows the presence of a Chern insulating phase independent of the spin orientation in contrast to the spin-orbit coupling induced Chern insulator that disappears with in-plane ferromagnetism constrained by symmetry.
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Insulating Phase sentence examples within Trivial Insulating Phase
Different from its trivial insulating phase, this 2D topological state exhibits a finite longitudinal conductance at ~2e2/h when the Fermi level is aligned within the surface gap, indicating an emergent quantum spin Hall (QSH) state.
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As a direct application, we consider a holographic model which exhibits a topological quantum phase transition between a topologically trivial insulating phase and a gapless Weyl semimetal.
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Insulating Phase sentence examples within Antiferromagnetic Insulating Phase
7MnO3 films gives rise to a series of structural transformations ranging from the perovskite to the intermediate state and to the brownmillerite one, accompanied by tunable electronic performances from the antiferromagnetic insulating phase to the weak magnetic insulating one.
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Our two-band double exchange model Hamiltonian calculations show that the ‘Sr’ doping induces the ferromagnetic clusters in the antiferromagnetic insulating phase and in turn reduces the critical field.
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Insulating Phase sentence examples within Band Insulating Phase
We demonstrate that it undergoes reversible strain-induced topological phase transitions from a strong topological insulator phase with spin-polarized, quasi-one-dimensional topological surface states, to topologically trivial semimetal and band insulating phases.
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We also show the existence of a band insulating phase in the system for the case ∆ 6= 0,U = 0 and calculate the staggered charge density nB−nA as a function of the interaction for different values of the mass imbalance.
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Insulating Phase sentence examples within Original Insulating Phase
Ultrafast optical studies of this insulator-to-metal transition indicate that it is mediated by the formation of a transient metallic phase that retains the structure of the original insulating phase.
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Ultrafast optical studies of this insulator-to-metal transition indicate that it is mediated by the formation of a transient metallic phase that retains the structure of the original insulating phase.
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Insulating Phase sentence examples within Afm Insulating Phase
The magnetic results show that the CO-AFM insulating phase and the weak FM phase coexist at low temperature, and spin-glass effect was found in all films.
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Finally, an overall phase diagram in the U -δ plane is presented, which is composed of four regimes: the AFM insulator at half-filling, the AFM metal with the compressibility κ > 0 or κ < 0, and the paramagnetic metal, as well as three phase transitions: (i) From the AFM metal to the paramagnetic metal, (ii) between the AFM metal phases with positive and negative κ, and (iii) separating the AFM insulating phase at δ = 0 from the AFM metal phase for δ > 0.
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Insulating Phase sentence examples within Temperature Insulating Phase
We perform magnetic susceptibility and magnetic torque measurements on the organic κ -(BEDT-TTF) 2 Hg(SCN) 2 Br, which is recently suggested to host an exotic quantum dipole-liquid in its low-temperature insulating phase.
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16em}{0ex}}\text{K}$ from a high-temperature bad metallic phase ($\frac{1}{{\ensuremath{\rho}}_{\text{DC}}}\frac{d{\ensuremath{\rho}}_{\text{DC}}}{dT}l0$) with a high value of resistivity ${\ensuremath{\rho}}_{\text{DC}}\ensuremath{\approx}70 \mathrm{m}\mathrm{\ensuremath{\Omega}}$ cm at 300 K to a low temperature insulating phase.
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Insulating Phase sentence examples within insulating phase change
Electrically insulating phase change composite materials (PCCMs) with lightweight, good thermal management performance, high stability and high mechanical strength are strongly desired for lithium-ion battery (LIB) thermal management.
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The electronic band structure of the Pnma-CaF2 structure can be classified as an insulating phase with a wide bandgap, and the bandgap decreases under pressure above 70 GPa.
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In the insulating phase, the in-gap state is further pushed away from the conduction band edge under hydrostatic pressure, which increases the fundamental gap.
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The occurrence of superconducting and insulating phases is well-established in twisted graphene bilayers, and they have also been reported in other arrangements of graphene layers.
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Here, we directly image the three-dimensional superconducting state as it approaches an insulating phase and discover that signatures of a two-dimensional granular superconducting phase spontaneously emerge at the transition.
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The interplay between Coulomb repulsion, disorder and magnetic fields, drives the otherwise semi-metallic regime to insulating phases exhibiting different characters.
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In particular, interdiffusion at the interface between the cathode and the electrolyte during long-term operation leads to the formation of insulating phases, significantly reducing the cell performance.
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One of them is a phase-twisted superfluid that exists at low hopping strengths and reduces the domain of insulating phases.
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This indicates that the system is sitting exactly at the border between metallic and insulating phase.
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Ferromagnetism (FM) remains intact in the insulating phase of K2V6Cr2O16.
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In the spinful case, these modified equations enable us to demonstrate that in some region of the bare parameters values the phase diagram contains two massive phases, charge (CDW) and spin (SDW) density waves, which are separated by an insulating phase.
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The insulating phase changes into a metallic phase when the band gap is set to zero.
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In this system, non-volatile bi-polar RS (up to ∼2× 106%) takes place via electric field induced expansion/shrinkage of metallic phase domains, which are separated by an insulating phase domain.
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Local quasiparticle states around impurities provide essential insight into the mechanism of unconventional superconductivity, especially when the candidate materials are proximate to an antiferromagnetic Mott-insulating phase.
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Carbon substitution in boron nitride in the form of eight membered rings is found to be stable, and the variation of the substituted rings in the patterned hybrid o-MLs changes the structure from an insulating phase to a metallic phase.
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Firstly, The Dirac point exists on its band structure and mainly contributed by d orbits of Mo atoms, it will open the energy gap and enter the insulating phase when the spin–orbit coupling is added.
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However, formation of the YSZ–CGO solid solution with low ionic conductivity and the SrZrO 3 (SZO) insulating phase still happens during cell production and long-term operation, causing poor performance and degradation.
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Broad interest in quantum spin liquid (QSL) phases was triggered by the notion that they can be viewed as insulating phases with preexisting electron pairs, such that upon light doping they might automatically yield high temperature superconductivity.
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On the one hand, the hybrid MMs structure behave as a transmission device when VO2 board in its insulating phase and VO2 grating in its metallic phase.
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This insulating phase is adiabatically connected to a third-order topological insulator in the noninteracting limit, which features gapless modes around the corners of the pyrochlore lattice and is characterized by a \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${\mathbb {Z}}_{4}$$\end{document}Z4 spin-Berry phase.
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A new phenomenon of correlated plasmons was first observed in the insulating phase of the Sr1-xNb1-yO3+ family [T.
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Our study reveals that an insulating phase can be realized in the metallic cubic BaPbO3 in three ways in order to explore optoelectronic properties.
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In the weakly-coupled rungs situation, we find a smooth power-law localization whereas the strongly-coupled rungs limit produces a steep localization or insulating phase for various configurations of the two-peak random potential.
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While an insulating phase is found in the absence of Kac's rescaling, the latter leads to a new metallic phase that does not fall into the conventional Luttinger liquid paradigm.
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Many transition-metal dichalcogenides show competing metallic, superconducting, charge density waves (CDWs), or Mott-insulating phases.
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The combination of disorder and strong interactions makes it hard to understand the nature of doped silicon’s insulating phase.
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Combination of low-dimensionality and electron correlation is vital for exotic quantum phenomena such as the Mott-insulating phase and high-temperature superconductivity.
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In the strongly correlated limit, we construct an effective spin Hamiltonian on a honeycomb lattice that includes the Heisenberg interaction and nonsymmetric interactions such as a Dzyaloshinskii-Moriya interaction and a Kane-Mele coupling for the Mott-insulating phase at half-filling.
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The proposed device acts as a low-frequency broadband absorber if the vanadium dioxide is in the insulating phase, for which the Fermi energy level of graphene varies from to 0.
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For instance, the quantum spin Hall (QSH), the quantum anomalous Hall (QAH), and the three-dimensional (3D) topological insulator (TI) phase are insulating phases of matter that owe their nontrivial topology to an inverted band structure.
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We discuss possible origins of these sharp resistance peaks and we draw a stability diagram for the insulating phases in the $\ensuremath{\nu}\ensuremath{-}T$ phase space.
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While the system displays zero modes in the metallic phase apart from the nontrivial insulator phase, the metallic zero modes are not robust, as are the ones found in the insulating phase.
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The oxygen electrodes of the pristine and tested cells have been characterized by synchrotron X-ray micro-diffraction and micro-fluorescence to assess the relation between the material destabilization and the formation of insulating phases due to interlayer diffusion.
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1 ) is consistent with the theoretical one predicted by an analytical expression derived for the optimal rectification factor, as a function of the VO 2 emissivity in the metallic and insulating phases, sensor emissivity, and geometrical parameters.
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When VO2 is in the insulating phase, we observe an apparent resonance dip in the reflection spectrum, which is attributed to a hybrid mode originating from the gap plasmon in the dimers and localized surface plasmon (LSP) resonance excited at the edge of the nanodisks.
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By performing a summation of subsets of diagrams we are able to find the condition to the long-range correlations which leads to the phase boundary between superfluid and insulating phases.
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Remarkably, the isostructural Mott transition in Cr-doped V2O3 between paramagnetic metallic and insulating phase observed in bulk has been elusive in thin film compounds so far.
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Their key achievement is the observation of magnetoconductance oscillation of all films including superconducting, metallic and insulating phases, with a constant period of 0 = h/2e.
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