The sliding phase transition in ferroelectric van der Waals bilayers. (arXiv:2208.00442v1 [cond-mat.mes-hall])

2022-08-02T04:30:22+00:00August 2nd, 2022|Categories: Publications|Tags: |

We address the sliding thermodynamics of van der Waals-bonded bilayers by the continuum elasticity theory. We attribute the robustness of the ferroelectricity recently observed in h-BN and WTe2 bilayers to large monolayer in-plane stiffness. We compute the electric susceptibility and specific heat in the mean-field self-consistent phonon approximation. We compare critical temperatures and electric switching fields with the observations.

Published : "arXiv Mesoscale and Nanoscale Physics".

Orbital polarization and third-order anomalous Hall effect in WTe2. (arXiv:2207.08045v1 [cond-mat.mes-hall])

2022-07-19T04:30:21+00:00July 19th, 2022|Categories: Publications|Tags: |

The anomalous Hall effect (AHE) has been extended into the nonlinear regime, where the Hall voltage shows higher-order response to the applied current. Nevertheless, the microscopic mechanism of the nonlinear AHE remains unclear. Here we report the orbital polarization and its induced third-order AHE in few-layer WTe2 flakes. Through angle-dependent electric measurements, it is found that the third-order AHE is quite consistent with the electric field induced polarization of orbital magnetic moment caused by the Berry connection polarizability tensor, which is further directly detected by polar reflective magnetic circular dichroism spectroscopy. The microscopic mechanisms of third-order AHE are analyzed through the scaling law, that is, the opposite orbital magnetic moments (up or down) deflect to opposite directions driven by electric field induced Berry curvature, forming the intrinsic contribution; driven by the Magnus effect of the self-rotating Bloch electrons, the opposite orbital magnetic moments are scattered towards opposite transverse directions, resulting in the skew scattering.

Published : "arXiv Mesoscale and Nanoscale Physics".

Orbital polarization and third-order anomalous Hall effect in WTe2. (arXiv:2207.08045v1 [cond-mat.mes-hall])

2022-07-19T02:29:28+00:00July 19th, 2022|Categories: Publications|Tags: |

The anomalous Hall effect (AHE) has been extended into the nonlinear regime, where the Hall voltage shows higher-order response to the applied current. Nevertheless, the microscopic mechanism of the nonlinear AHE remains unclear. Here we report the orbital polarization and its induced third-order AHE in few-layer WTe2 flakes. Through angle-dependent electric measurements, it is found that the third-order AHE is quite consistent with the electric field induced polarization of orbital magnetic moment caused by the Berry connection polarizability tensor, which is further directly detected by polar reflective magnetic circular dichroism spectroscopy. The microscopic mechanisms of third-order AHE are analyzed through the scaling law, that is, the opposite orbital magnetic moments (up or down) deflect to opposite directions driven by electric field induced Berry curvature, forming the intrinsic contribution; driven by the Magnus effect of the self-rotating Bloch electrons, the opposite orbital magnetic moments are scattered towards opposite transverse directions, resulting in the skew scattering.

Published in: "arXiv Material Science".

Two Types of 3D Bulk Quantum Hall Effects in Multilayer WTe$_2$. (arXiv:2206.02253v1 [cond-mat.mes-hall])

2022-06-07T04:30:20+00:00June 7th, 2022|Categories: Publications|Tags: |

Interplay between the topological surface states and bulk states gives rise to diverse exotic transport phenomena in topological materials. The recently proposed Weyl orbit in topological semimetals in the presence of magnetic field is a remarkable example. This novel closed magnetic orbit consists of Fermi arcs on two spatially separated sample surfaces which are connected by the bulk chiral zero mode, which can contribute to transport. Here we report Shubnikov-de Haas (SdH) oscillation and its evolution into quantum Hall effect (QHE) in multilayered type-II Weyl semimetal WTe2. We observe both the three-dimensional (3D) QHE from bulk states by parallelly stacking of confined two-dimensional layers in the low magnetic field region and the 3D QHE in the quantized surface transport due to Weyl orbits in the high magnetic field region. Our study of the two types of novel QHEs controlled by magnetic field and our demonstration of the crossover between quantized bulk and surface transport provide an essential platform for the future quantized transport studies in topological semimetals.

Published : "arXiv Mesoscale and Nanoscale Physics".

Two Types of 3D Bulk Quantum Hall Effects in Multilayer WTe$_2$. (arXiv:2206.02253v1 [cond-mat.mes-hall])

2022-06-07T02:29:24+00:00June 7th, 2022|Categories: Publications|Tags: |

Interplay between the topological surface states and bulk states gives rise to diverse exotic transport phenomena in topological materials. The recently proposed Weyl orbit in topological semimetals in the presence of magnetic field is a remarkable example. This novel closed magnetic orbit consists of Fermi arcs on two spatially separated sample surfaces which are connected by the bulk chiral zero mode, which can contribute to transport. Here we report Shubnikov-de Haas (SdH) oscillation and its evolution into quantum Hall effect (QHE) in multilayered type-II Weyl semimetal WTe2. We observe both the three-dimensional (3D) QHE from bulk states by parallelly stacking of confined two-dimensional layers in the low magnetic field region and the 3D QHE in the quantized surface transport due to Weyl orbits in the high magnetic field region. Our study of the two types of novel QHEs controlled by magnetic field and our demonstration of the crossover between quantized bulk and surface transport provide an essential platform for the future quantized transport studies in topological semimetals.

Published in: "arXiv Material Science".

Electronic properties of the steps in bilayer Td-WTe2. (arXiv:2205.12417v1 [cond-mat.mes-hall])

2022-05-26T04:30:17+00:00May 26th, 2022|Categories: Publications|Tags: |

Monolayer WTe2 stripes are quantum spin Hall (QSH) insulators. Density functional theory was used for investigating the electronic properties of the stripes and steps in bilayer Td-WTe2. For the stripes oriented along the dimer chains of W atoms (x direction), the hybridization between the two layers suppresses the QSH states. However, the QSH nature can be recovered by forming a step, depending on the atomic structure of the step. Conversely, the stripes and steps along the y direction maintain the QSH states. These findings can expand the application range of the QSH states in WTe2.

Published : "arXiv Mesoscale and Nanoscale Physics".

Transparent Josephson Junctions in Higher-Order Topological Insulator WTe2 via Pd Diffusion. (arXiv:2205.06542v1 [cond-mat.mes-hall])

2022-05-16T04:30:25+00:00May 16th, 2022|Categories: Publications|Tags: |

Highly transparent superconducting contacts to a topological insulator (TI) remain a persistent challenge on the route to engineer topological superconductivity. Recently, the higher-order TI WTe$_2$ was shown to turn superconducting when placed on palladium (Pd) bottom contacts, demonstrating a promising material system in perusing this goal. Here, we report the diffusion of Pd into WTe$_2$ and the formation of superconducting PdTe$_x$ as the origin of observed superconductivity. We find an atomically sharp interface between the diffusion layer and its host crystal, forming state-of-the-art superconducting contacts to a TI. The diffusion is discovered to be non-uniform along the width of the WTe$_2$ crystal, with a greater extend along the edges compared to the bulk. The potential of this contacting method is highlighted in transport measurements on Josephson junctions by employing external superconducting leads.

Published : "arXiv Mesoscale and Nanoscale Physics".

Fermi surface and nested magnetic breakdown in WTe2. (arXiv:2204.09977v1 [cond-mat.mes-hall])

2022-04-22T04:30:17+00:00April 22nd, 2022|Categories: Publications|Tags: |

We report a detailed Shubnikov-de Haas (SdH) study on the Weyl type-II semimetal WTe2 in magnetic fields up to 29 T. By using the SdH results to guide our density functional theory calculations, we are able to accurately determine its Fermi surface by employing a moderate Hubbard U term, which is an essential step in explaining the unusual electronic properties of this much studied material. In addition to the fundamental orbits, we observe magnetic breakdown, which can consistently be explained within the model of a Russian-doll-nested Fermi surface of electron and hole pockets. The onset of magnetic breakdown in WTe2 is solely determined by impurity damping in contrast to magnetic breakdown scenarios in other metallic systems.

Published : "arXiv Mesoscale and Nanoscale Physics".

Visualizing the thermoelectric origin of photocurrent flow in anisotropic semimetals. (arXiv:2203.17176v1 [cond-mat.mtrl-sci])

2022-04-01T04:30:30+00:00April 1st, 2022|Categories: Publications|Tags: |

Photocurrent measurements are incisive probes of crystal symmetry, electronic band structure, and material interfaces. However, conventional scanning photocurrent microscopy (SPCM) convolves the processes for photocurrent generation and collection, which can obscure the intrinsic light-matter interaction. Here, by using ac magnetometry with a nitrogen-vacancy center spin ensemble, we demonstrate the high-sensitivity, sub-micron resolved imaging of vector photocurrent flow. Our imaging reveals that in anisotropic semimetals WTe2 and TaIrTe4, the photoexcited electron carriers propagate outward along the zigzag chains and inward perpendicular to the chains. This circulating pattern is explained by our theoretical modeling to emerge from an anisotropic photothermoelectric effect (APTE) caused by a direction-dependent thermopower. Through simultaneous SPCM and magnetic imaging, we directly visualize how local APTE photocurrents stimulate long-range photocurrents at symmetry-breaking edges and contacts. These results uniquely validate the Shockley-Ramo process for photocurrent collection in gapless materials and identify the overlooked APTE as the primary origin of robust photocurrents in anisotropic semimetal devices. Our work highlights quantum-enabled photocurrent flow microscopy as a clarifying perspective for complex optoelectronic phenomena.

Published : "arXiv Mesoscale and Nanoscale Physics".

Visualizing the thermoelectric origin of photocurrent flow in anisotropic semimetals. (arXiv:2203.17176v1 [cond-mat.mtrl-sci])

2022-04-01T02:29:22+00:00April 1st, 2022|Categories: Publications|Tags: |

Photocurrent measurements are incisive probes of crystal symmetry, electronic band structure, and material interfaces. However, conventional scanning photocurrent microscopy (SPCM) convolves the processes for photocurrent generation and collection, which can obscure the intrinsic light-matter interaction. Here, by using ac magnetometry with a nitrogen-vacancy center spin ensemble, we demonstrate the high-sensitivity, sub-micron resolved imaging of vector photocurrent flow. Our imaging reveals that in anisotropic semimetals WTe2 and TaIrTe4, the photoexcited electron carriers propagate outward along the zigzag chains and inward perpendicular to the chains. This circulating pattern is explained by our theoretical modeling to emerge from an anisotropic photothermoelectric effect (APTE) caused by a direction-dependent thermopower. Through simultaneous SPCM and magnetic imaging, we directly visualize how local APTE photocurrents stimulate long-range photocurrents at symmetry-breaking edges and contacts. These results uniquely validate the Shockley-Ramo process for photocurrent collection in gapless materials and identify the overlooked APTE as the primary origin of robust photocurrents in anisotropic semimetal devices. Our work highlights quantum-enabled photocurrent flow microscopy as a clarifying perspective for complex optoelectronic phenomena.

Published in: "arXiv Material Science".

Orbit-transfer torque driven field-free switching of perpendicular magnetization. (arXiv:2202.07840v1 [cond-mat.mtrl-sci])

2022-02-17T04:30:23+00:00February 17th, 2022|Categories: Publications|Tags: , |

The reversal of perpendicular magnetization (PM) by electric control is crucial for high-density integration of low-power magnetic random-access memory (MRAM). Although the spin-transfer torque (STT) and spin-orbit torque (SOT) technologies have been used to switch the magnetization of a free layer with perpendicular magnetic anisotropy, the former has limited endurance because of the high current density directly through the junction, while the latter requires an external magnetic field or unconventional configuration to break the symmetry. Here we propose and realize the orbit-transfer torque (OTT), that is, exerting torque on the magnetization using the orbital magnetic moments, and thus demonstrate a new strategy for current-driven PM reversal without external magnetic field. The perpendicular polarization of orbital magnetic moments is generated by a direct current in a few-layer WTe2 due to the existence of nonzero Berry curvature dipole, and the polarization direction can be switched by changing the current polarity. Guided by this principle, we construct the WTe2/Fe3GeTe2 heterostructures, where the OTT driven field-free deterministic switching of PM is achieved.

Published : "arXiv Mesoscale and Nanoscale Physics".

Orbit-transfer torque driven field-free switching of perpendicular magnetization. (arXiv:2202.07840v1 [cond-mat.mtrl-sci])

2022-02-17T02:29:25+00:00February 17th, 2022|Categories: Publications|Tags: , |

The reversal of perpendicular magnetization (PM) by electric control is crucial for high-density integration of low-power magnetic random-access memory (MRAM). Although the spin-transfer torque (STT) and spin-orbit torque (SOT) technologies have been used to switch the magnetization of a free layer with perpendicular magnetic anisotropy, the former has limited endurance because of the high current density directly through the junction, while the latter requires an external magnetic field or unconventional configuration to break the symmetry. Here we propose and realize the orbit-transfer torque (OTT), that is, exerting torque on the magnetization using the orbital magnetic moments, and thus demonstrate a new strategy for current-driven PM reversal without external magnetic field. The perpendicular polarization of orbital magnetic moments is generated by a direct current in a few-layer WTe2 due to the existence of nonzero Berry curvature dipole, and the polarization direction can be switched by changing the current polarity. Guided by this principle, we construct the WTe2/Fe3GeTe2 heterostructures, where the OTT driven field-free deterministic switching of PM is achieved.

Published in: "arXiv Material Science".

Enhancing Perpendicular Magnetic Anisotropy in Garnet Ferrimagnet by Interfacing with Few-Layer WTe2. (arXiv:2202.02834v1 [cond-mat.mtrl-sci])

2022-02-08T05:29:30+00:00February 8th, 2022|Categories: Publications|Tags: , |

Engineering magnetic anisotropy in a ferro- or ferrimagnetic (FM) thin film is crucial in spintronic device. One way to modify the magnetic anisotropy is through the surface of the FM thin film. Here, we report the emergence of a perpendicular magnetic anisotropy (PMA) induced by interfacial interactions in a heterostructure comprised of a garnet ferrimagnet, Y3Fe5O12 (YIG), and the low-symmetry, high spin orbit coupling (SOC) transition metal dichalcogenide, WTe2. At the same time, we also observed an enhancement in Gilbert damping in the WTe2 covered YIG area. Both the magnitude of interface-induced PMA and the Gilbert damping enhancement have no observable WTe2 thickness dependence down to single quadruple-layer, indicating that the interfacial interaction plays a critical role. The ability of WTe2 to enhance the PMA in FM thin film, combined with its previously reported capability to generate out-of-plane damping like spin torque, makes it desirable for magnetic memory applications.

Published in: "arXiv Material Science".

Direct observation of vortices in an electron fluid. (arXiv:2202.02798v1 [cond-mat.mes-hall])

2022-02-08T05:29:28+00:00February 8th, 2022|Categories: Publications|Tags: |

Vortices are the hallmarks of hydrodynamic flow. Recent studies indicate that strongly-interacting electrons in ultrapure conductors can display signatures of hydrodynamic behavior including negative nonlocal resistance, Poiseuille flow in narrow channels, and a violation of the Wiedemann-Franz law. Here we provide the first visualization of whirlpools in an electron fluid. By utilizing a nanoscale scanning superconducting quantum interference device on a tip (SQUID-on-tip) we image the current distribution in a circular chamber connected through a small aperture to an adjacent narrow current carrying strip in high-purity type-II Weyl semimetal WTe2. In this geometry, the Gurzhi momentum diffusion length and the size of the aperture determine the vortex stability phase diagram. We find that the vortices are present only for small apertures, whereas the flow is laminar (non-vortical) for larger apertures, consistent with the theoretical analysis of the hydrodynamic regime and in contrast to the expectations of ballistic transport in WTe2 at low temperatures. Moreover, near the vortical-to-laminar transition, we observe a single vortex in the chamber splitting into two vortices, a behavior that can occur only in the hydrodynamic regime and cannot be sustained by ballistic transport. These findings suggest a novel mechanism of hydrodynamic flow: instead of the commonly considered electron-electron scattering at the bulk, which becomes extremely weak at low temperatures, the spatial diffusion of charge carriers’ momenta is enabled by small-angle scattering at the planar surfaces of thin pure crystals. This surface-induced para-hydrodynamics opens new avenues for exploring and utilizing electron fluidics in high-mobility electron systems.

Published in: "arXiv Material Science".

Enhancing Perpendicular Magnetic Anisotropy in Garnet Ferrimagnet by Interfacing with Few-Layer WTe2. (arXiv:2202.02834v1 [cond-mat.mtrl-sci])

2022-02-08T04:30:19+00:00February 8th, 2022|Categories: Publications|Tags: , |

Engineering magnetic anisotropy in a ferro- or ferrimagnetic (FM) thin film is crucial in spintronic device. One way to modify the magnetic anisotropy is through the surface of the FM thin film. Here, we report the emergence of a perpendicular magnetic anisotropy (PMA) induced by interfacial interactions in a heterostructure comprised of a garnet ferrimagnet, Y3Fe5O12 (YIG), and the low-symmetry, high spin orbit coupling (SOC) transition metal dichalcogenide, WTe2. At the same time, we also observed an enhancement in Gilbert damping in the WTe2 covered YIG area. Both the magnitude of interface-induced PMA and the Gilbert damping enhancement have no observable WTe2 thickness dependence down to single quadruple-layer, indicating that the interfacial interaction plays a critical role. The ability of WTe2 to enhance the PMA in FM thin film, combined with its previously reported capability to generate out-of-plane damping like spin torque, makes it desirable for magnetic memory applications.

Published : "arXiv Mesoscale and Nanoscale Physics".

Direct observation of vortices in an electron fluid. (arXiv:2202.02798v1 [cond-mat.mes-hall])

2022-02-08T04:30:17+00:00February 8th, 2022|Categories: Publications|Tags: |

Vortices are the hallmarks of hydrodynamic flow. Recent studies indicate that strongly-interacting electrons in ultrapure conductors can display signatures of hydrodynamic behavior including negative nonlocal resistance, Poiseuille flow in narrow channels, and a violation of the Wiedemann-Franz law. Here we provide the first visualization of whirlpools in an electron fluid. By utilizing a nanoscale scanning superconducting quantum interference device on a tip (SQUID-on-tip) we image the current distribution in a circular chamber connected through a small aperture to an adjacent narrow current carrying strip in high-purity type-II Weyl semimetal WTe2. In this geometry, the Gurzhi momentum diffusion length and the size of the aperture determine the vortex stability phase diagram. We find that the vortices are present only for small apertures, whereas the flow is laminar (non-vortical) for larger apertures, consistent with the theoretical analysis of the hydrodynamic regime and in contrast to the expectations of ballistic transport in WTe2 at low temperatures. Moreover, near the vortical-to-laminar transition, we observe a single vortex in the chamber splitting into two vortices, a behavior that can occur only in the hydrodynamic regime and cannot be sustained by ballistic transport. These findings suggest a novel mechanism of hydrodynamic flow: instead of the commonly considered electron-electron scattering at the bulk, which becomes extremely weak at low temperatures, the spatial diffusion of charge carriers’ momenta is enabled by small-angle scattering at the planar surfaces of thin pure crystals. This surface-induced para-hydrodynamics opens new avenues for exploring and utilizing electron fluidics in high-mobility electron systems.

Published : "arXiv Mesoscale and Nanoscale Physics".

Giant second-order nonlinearity of chiral Bloch electrons in twisted bilayer graphene. (arXiv:2201.09274v1 [cond-mat.mes-hall])

2022-01-25T04:30:34+00:00January 25th, 2022|Categories: Publications|Tags: , , |

The moir’e flat bands in twisted bilayer graphene (TBG), with Coulomb interactions dominate over the kinetic energy, have been proven to be a wealthy platform for many strong-correlation phases, such as metal-insulator transition and superconductivity. The observations of ferromagnetism and quantum anomalous Hall effect demonstrate the nontrivial topological properties of these moir’e flat bands. Here, we report a giant nonlinear transport response in TBG without breaking time-reversal symmetry, in which a second harmonic transverse electric voltage drop is generated by a longitudinal charge current. The magnitude and the direction of the second-order nonlinearity can be effectively tuned by the gate voltage. The peak value of the second-order Hall conductivity close to the full filling of the moir’e band reaches 4.38 ${mu}mSV^{-1}$, four-order larger than those reported in WTe2. The observed effect can be understood from the skew-scatterings of electrons arising from the chirality of the Bloch wave functions in noncentrosymmetric crystals. Through temperature-dependent measurements, the scaling law of the second-order Hall conductivity suggests that the skew-scatterings contribution of the chiral Bloch electrons from dynamic disorders dominates the observed giant second-order nonlinearity in TBG. Our observations demonstrate the potential of TBG in studying nonlinear response and rectification applications.

Published : "arXiv Mesoscale and Nanoscale Physics".

Pseudo-hydrodynamic flow of quasiparticles in semimetal WTe2 at room temperature. (arXiv:2201.08331v1 [cond-mat.mes-hall])

2022-01-21T02:29:31+00:00January 21st, 2022|Categories: Publications|Tags: , |

Recently, much interest has emerged in fluid-like electric charge transport in various solid-state systems. The hydrodynamic behavior of the electronic fluid reveals itself as a decrease of the electrical resistance with increasing temperature (the Gurzhi effect) in narrow conducting channels, polynomial scaling of the resistance as a function of the channel width, substantial violation of the Wiedemann-Franz law supported by the emergence of the Poiseuille flow. Similarly to whirlpools in flowing water, the viscous electronic flow generates vortices, resulting in abnormal sign-changing electrical response driven by the backflow of electrical current. Experimentally, the presence of the hydrodynamic vortices was observed in low-temperature graphene as a negative voltage drop near the current-injecting contacts. However, the question of whether the long-ranged sign-changing electrical response can be produced by a mechanism other than hydrodynamics has not been addressed so far. Here we use polarization-sensitive laser microscopy to demonstrate the emergence of visually similar abnormal sign-alternating patterns in charge density in multilayer tungsten ditelluride at room temperature where this material does not exhibit true electronic hydrodynamics. We argue that this pseudo-hydrodynamic behavior appears due to a subtle interplay between the diffusive transport of electrons and holes. In particular, the sign-alternating charge accumulation in WTe2 is supported by the unexpected backflow of compressible neutral electron-hole current, which creates charge-neutral whirlpools in the bulk of this nearly compensated semimetal. We demonstrate that the exceptionally large spatial size of the charge domains is sustained by the long recombination time of electron-hole pairs.

Published in: "arXiv Material Science".

Comments on quantum oscillations in two-dimensional insulators induced by graphite gates. (arXiv:2112.07138v1 [cond-mat.mes-hall])

2021-12-15T04:30:31+00:00December 15th, 2021|Categories: Publications|Tags: , |

A recent Letter by Zhu et al [Phys. Rev. Lett. 127, 247702 (2021)] claimed a unified mechanism for quantum oscillations (QOs) in graphite-gated 2D devices based on studies of three cases (WTe2, MoTe$_2$/WSe$_2$ heterobilayers and bilayer graphene (BLG)). We find that not only are the claims of Zhu et al based on insufficient evidence in all three cases but also critical aspects are ignored. Their conclusions are hence unreliable.

Published : "arXiv Mesoscale and Nanoscale Physics".

Light-tunable charge density wave orders in MoTe2 and WTe2 single layers. (arXiv:2111.11920v1 [cond-mat.mtrl-sci])

2021-11-24T02:29:52+00:00November 24th, 2021|Categories: Publications|Tags: , |

By using constrained density functional theory modeling, we demonstrate that ultrafast optical pumping unveils hidden charge orders in group VI monolayer transition metal ditellurides. We show that irradiation of the insulating 2H phases stabilizes multiple transient charge density wave orders with light-tunable distortion, periodicity, electronic structure and bandgap. Moreover, optical pumping of the semimetallic 1T’ phases generates a transient charge ordered metallic phase composed of 2D diamond clusters. For each transient phase we identify the critical fluence at which it is observed and the specific optical and Raman fingerprints to directly compare with future ultrafast pump-probe experiments. Our work demonstrates that it is possible to stabilize charge density waves even in insulating 2D transition metal dichalcogenides by ultrafast irradiation.

Published in: "arXiv Material Science".

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