Fucai Liu's research while affiliated with Yangtze Delta Region Institute of Tsinghua University and other places

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Publications (130)


Inverse-current quantum electro-oscillations in a charge density wave insulator
  • Article

June 2024

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19 Reads

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Ruiyang Jiang

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Linfeng Tu

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Quantum magneto-oscillations have long been a vital subject in condensed matter physics, with ubiquitous quantum phenomena and diverse underlying physical mechanisms. Here, we demonstrate the intrinsic and reproducible DC-current-driven quantum electro-oscillations with a periodicity in the inverse of the current (1/I), in quasi-one-dimensional charge-density-wave (CDW) insulator (TaSe4)2I and TaS3 nanowires. Such oscillations manifest in the nearly infinite Fröhlich conductivity region where the undamped CDW flow forms in a finite electric current, and finally disappear after the oscillation index n reaches 1. A systematic investigation on the effect of temperature and magnetic field establishes that the observed electro-oscillations are a coherent quantum phenomenon. We discuss the possibilities of the physical mechanisms, including the formation of sliding-driven inherent Floquet sidebands. Our results introduce a member in the family of quantum oscillations and shed light on plausible avenues to explore the physics and potential applications of coherent density-wave condensates.

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a) HAADF‐STEM image of CuCrP2S6 flakes. b) TEM image of CuCrP2S6 flakes. c) AFM image and corresponding height profile of CuCrP2S6 flakes. d,e) Atom‐resolved HAADF‐STEM images of CuCrP2S6 flakes. f) SAED pattern taken from CuCrP2S6 flakes. g) HAADF‐STEM image and corresponding elemental mapping images of CuCrP2S6 flakes.
a) XRD patterns of CuInP2S6, CuVP2S6, and CuCrP2S6 flakes. b) Cr K‐edge XANES spectra and c) Fourier transform spectra of Cr K‐edge EXAFS spectra of Cr foil, Cr2O3, and CuCrP2S6. WT plots of d) Cr foil, e) Cr2O3, and f) CuCrP2S6. g) Schematic diagram of the crystal structure of CuCrP2S6. h) EXAFS R‐space fitting profile of CuCrP2S6. i) Cu K‐edge XANES spectra and j) Fourier transform spectra of Cu K‐edge EXAFS spectra of Cu foil, Cu2O, CuO, and CuCrP2S6. WT plots of k) Cu foil, l) Cu2O, m) CuO, and n) CuCrP2S6. The XAFS data presented above are not phase‐corrected.
a) UV–vis–IR absorption spectra of CuInP2S6, CuVP2S6, and CuCrP2S6 flakes. UPS spectra of b) CuVP2S6 flakes and c) CuCrP2S6 flakes. d) Photocatalytic H2 evolution performance of CuInP2S6, CuVP2S6, and CuCrP2S6 flakes under simulated sunlight irradiation. e) PHE rates of CuVP2S6 and CuCrP2S6 samples with different morphologies under simulated sunlight irradiation. f) Comparison of PHE rates for different LMPSs including CuInP2S6, CuVP2S6, and CuCrP2S6 under simulated sunlight irradiation.[13,14,24] g) Photocatalytic H2 evolution performance of CuInP2S6, CuVP2S6, and CuCrP2S6 flakes under NIR light irradiation (λ > 780 nm). h) PHE rates of CuVP2S6 and CuCrP2S6 samples with different morphologies under NIR light irradiation (λ > 780 nm). i) Comparison of PHE rates for different materials including CuVP2S6 and CuCrP2S6 flakes under NIR light irradiation (λ > 780 nm).
KPFM potential images of a,b) CuVP2S6 flakes and d,e) CuCrP2S6 flakes in the dark (a,d) and under the light illumination (b,e). Surface potential profiles of c) CuVP2S6 flakes and f) CuCrP2S6 flakes in the dark and under the light illumination. 3D contour plots of femtosecond‐resolved TAS spectra for g) CuVP2S6 flakes and h) CuCrP2S6 flakes. i) Femtosecond‐resolved TAS kinetics probed at 500–600 nm for CuInP2S6, CuVP2S6, and CuCrP2S6 flakes.
Band structure and density of states for a) CuInP2S6, b) CuVP2S6, and c) CuCrP2S6. The charge differences of d) CuInP2S6, e) CuVP2S6, and f) CuCrP2S6 in the three selected areas related to the dotted‐line region. The three selected areas are the upper surface of P, the middle surface of metal, and the lower surface of P, respectively. Color codes in (d–f): yellow, lightcoral, turquoise, saddlebrown, violet, and royalbule spheres represent S, P, In, V, Cr, and Cu atoms, respectively. Red = electron deficiency; blue = electron surplus; green = 0.

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Black Ultrathin Single‐Crystalline Flakes of CuVP2S6 and CuCrP2S6 for Near‐Infrared‐Driven Photocatalytic Hydrogen Evolution
  • Article
  • Publisher preview available

June 2024

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52 Reads

Advanced Materials

Advanced Materials

The development of new near‐infrared‐responsive photocatalysts is a fascinating and challenging approach to acquire high photocatalytic hydrogen evolution (PHE) performance. Herein, near‐infrared‐responsive black CuVP2S6 and CuCrP2S6 flakes, as well as CuInP2S6 flakes, are designed and constructed for PHE. Atom‐resolved scanning transmission electron microscopy images and X‐ray absorption fine structure evidence the formation of ultrathin single‐crystalline sheet‐like structure of CuVP2S6 and CuCrP2S6. The synthetic CuVP2S6 and CuCrP2S6, with a narrow bandgap of ≈1.0 eV, shows the high light‐absorption edge exceeding 1100 nm. Moreover, through the femtosecond‐resolved transient absorption spectroscopy, CuCrP2S6 displays the efficient charge transfer and long charge lifetime (18318.1 ps), which is nearly 3 and 29 times longer than that of CuVP2S6 and CuInP2S6, respectively. In addition, CuCrP2S6, with the appropriate d‐band and p‐band, is thermodynamically favorable for the H⁺ adsorption and H2 desorption by contrast with CuVP2S6 and CuInP2S6. As a result, CuCrP2S6 exhibits high PHE rates of 9.12 and 0.66 mmol h⁻¹ g⁻¹ under simulated sunlight and near‐infrared light irradiation, respectively, far exceeding other layered metal phospho–sulfides. This work offers a distinctive perspective for the development of new near‐infrared‐responsive photocatalysts.

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Developing fatigue-resistant ferroelectrics using interlayer sliding switching

June 2024

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53 Reads

Science

Ferroelectric materials have switchable electrical polarization that is appealing for high density non-volatile memories. However, inevitable fatigue hinders practical applications of these materials. Fatigue-free ferroelectric switching could dramatically improve the endurance of devices. We report a fatigue-free ferroelectric system based on the sliding ferroelectricity of bilayer 3R-MoS 2 . The memory performance of this ferroelectric device does not show the “wake-up effect” at low cycles or a substantial “fatigue effect” after 10 ⁶ switching cycles under different pulse widths. The total stress time of device under an electric field is up to 10 ⁵ s, which is long relative to other devices. Our theoretical calculation uncovers that the fatigue-free feature of sliding ferroelectricity is due to the immobile charge defects in sliding ferroelectricity.


Neuromorphic circuits based on memristors: endowing robots with a human-like brain

June 2024

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9 Reads

Journal of Semiconductors

Robots are widely used, providing significant convenience in daily life and production. With the rapid development of artificial intelligence and neuromorphic computing in recent years, the realization of more intelligent robots through a profound intersection of neuroscience and robotics has received much attention. Neuromorphic circuits based on memristors used to construct hardware neural networks have proved to be a promising solution of shattering traditional control limitations in the field of robot control, showcasing characteristics that enhance robot intelligence, speed, and energy efficiency. Starting with introducing the working mechanism of memristors and peripheral circuit design, this review gives a comprehensive analysis on the biomimetic information processing and biomimetic driving operations achieved through the utilization of neuromorphic circuits in brain-like control. Four hardware neural network approaches, including digital-analog hybrid circuit design, novel device structure design, multi-regulation mechanism, and crossbar array, are summarized, which can well simulate the motor decision-making mechanism, multi-information integration and parallel control of brain at the hardware level. It will be definitely conductive to promote the application of memristor-based neuromorphic circuits in areas such as intelligent robotics, artificial intelligence, and neural computing. Finally, a conclusion and future prospects are discussed.




Magnetic field filtering of the boundary supercurrent in unconventional metal NiTe2-based Josephson junctions

March 2024

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53 Reads

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1 Citation

Nature Communications

Topological materials with boundary (surface/edge/hinge) states have attracted tremendous research interest. Additionally, unconventional (obstructed atomic) materials have recently drawn lots of attention owing to their obstructed boundary states. Experimentally, Josephson junctions (JJs) constructed on materials with boundary states produce the peculiar boundary supercurrent, which was utilized as a powerful diagnostic approach. Here, we report the observations of boundary supercurrent in NiTe 2 -based JJs. Particularly, applying an in-plane magnetic field along the Josephson current can rapidly suppress the bulk supercurrent and retain the nearly pure boundary supercurrent, namely the magnetic field filtering of supercurrent. Further systematic comparative analysis and theoretical calculations demonstrate the existence of unconventional nature and obstructed hinge states in NiTe 2 , which could produce hinge supercurrent that accounts for the observation. Our results reveal the probable hinge states in unconventional metal NiTe 2 , and demonstrate in-plane magnetic field as an efficient method to filter out the bulk contributions and thereby to highlight the hinge states hidden in topological/unconventional materials.


Synergistically Modulating Conductive Filaments in Ion‐Based Memristors for Enhanced Analog In‐Memory Computing

March 2024

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54 Reads

Memristors offer a promising solution to address the performance and energy challenges faced by conventional von Neumann computer systems. Yet, stochastic ion migration in conductive filament often leads to an undesired performance tradeoff between memory window, retention, and endurance. Herein, a robust memristor based on oxygen‐rich SnO2 nanoflowers switching medium, enabled by seed‐mediated wet chemistry, to overcome the ion migration issue for enhanced analog in‐memory computing is reported. Notably, the interplay between the oxygen vacancy (Vo) and Ag ions (Ag⁺) in the Ag/SnO2/p⁺⁺‐Si memristor can efficiently modulate the formation and abruption of conductive filaments, thereby resulting in a high on/off ratio (>106), long memory retention (10‐year extrapolation), and low switching variability (SV = 6.85%). Multiple synaptic functions, such as paired‐pulse facilitation, long‐term potentiation/depression, and spike‐time dependent plasticity, are demonstrated. Finally, facilitated by the symmetric analog weight updating and multiple conductance states, a high image recognition accuracy of ≥ 91.39% is achieved, substantiating its feasibility for analog in‐memory computing. This study highlights the significance of synergistically modulating conductive filaments in optimizing performance trade‐offs, balancing memory window, retention, and endurance, which demonstrates techniques for regulating ion migration, rendering them a promising approach for enabling cutting‐edge neuromorphic applications.




Citations (61)


... As a result, the obstructed edge states are always expected. Recently, the existence of SI-free unconventionality and obstructed hinge states is demonstrated in NiTe 2 bulk, and the magnetic field filtering of hinge supercurrent in NiTe 2 -based Josephson junctions is observed experimentally [50]. ...

Reference:

Majorana corner modes in unconventional monolayers of 1T-PtSe2 family
Magnetic field filtering of the boundary supercurrent in unconventional metal NiTe2-based Josephson junctions

Nature Communications

... The spontaneous polarization properties of ScAlN are closely related to the crystal structure and electronic structure of the material. [41][42][43][44][45] In the crystal structure of ScAlN, Sc and Al are located on separate lattice sites. The greater atomic radius of Sc results in a more noticeable ionic shift in the Sc-N bond, which increases the spontaneous polarization. ...

Nanostructured Materials and Architectures for Advanced Optoelectronic Synaptic Devices

... [1][2][3][4] However, the digital computers of Von Neumann architecture-based digital computer engineering are approaching their physical limits due to the manufacturing process of memristors. 5,6 To break through the limitations of the "Von Neumann architecture" which has slowed down our development in the field of data processing, we are developing electronic devices with functions similar to those of biological synapses. 4,[6][7][8] Making computers run as an advanced animal brain is an important direction for future computer development. ...

Mimicking neuroplasticity via ion migration in van der Waals layered copper indium thiophosphate
  • Citing Article
  • November 2023

... [1,2] Typically, the RS of memristors relies on the formation and rupture of conductive filaments in an amorphous medium, rendering data storage and processing in a single unit for energyefficient analog in-memory computing. [3,4,5] However, large-scale implementation of these devices has consistently suffered from material-level challenges. This is due to uncontrolled ion migration and stochastic filament location and morphology, [6] thereby leading to poor spatial and temporal variations and limited optimization window between memory window, retention, and endurance. ...

Integrated Optoelectronic Memory Array with Enhanced Broadband Si-based Lines for Advanced Visual Systems
  • Citing Article
  • November 2023

... At low reaction temperature of Se and low Ar flow rate, the partial vapor pressure of Se and metallic precursors can be modulated for preparing stoichiometric CuCrSe 2 . [38,39] We used atomic force microscopy (AFM) to check the thickness of CuCrSe 2 nanosheet. Figure 1e shows the ultrathin CuCrSe 2 with the thickness of 2 nm, which can be considered as a one-unit cell (1 u.c.) layer due to the lattice constant of c = 1.938 nm. ...

A Universal Strategy for Synthesis of 2D Ternary Transition Metal Phosphorous Chalcogenides
Advanced Materials

Advanced Materials

... [457][458][459] Memristors emerge as a promising solution, enabling enhanced circuit integration and lower power consumption. 460,461 Memristors, which serve as nonlinear passive bipolar elements, offer versatile electrical properties that can be utilized in various analog and digital computations within circuits. [461][462][463] However, the application of algorithms to memristor-based circuits is currently restricted, primarily owing to the significant differences between memristors and traditional electronic components. ...

Technology and Integration Roadmap for Optoelectronic Memristor
Advanced Materials

Advanced Materials

... This antiferromagnetic vdW class also provides a platform for tuning the 2D magnetism through doping [31,32], pressure [33,34], and strain [13], rendering these materials promising application potentials. Moreover, research on the atomic-thin sample reveals exotic physics, such as novel exciton behaviors in NiPS 3 [35,36] and magnon-phonon hybrid excitations, aka magnon polarons in FePS 3 [37,38] and FePSe 3 [39]. ...

Chirality selective magnon-phonon hybridization and magnon-induced chiral phonons in a layered zigzag antiferromagnet

Nature Communications

... 2 1 引言 铁电性是一种经典现象,其特征是特定材料的自发极化,可以通过外加电场逆转。这一特性 在信息 [1][2][3][4][5][6][7] 、能源 [8][9][10][11][12] 和传感技术 [13][14][15][16][17][18] 等各个领域具有广泛应用的巨大潜力。近期在二维材料中发 现的铁电性使器件得以向原子厚度小型化方向前进,从而进一步推动了该领域的发展 [19,20] 。值 得注意的是,对二维铁电性的研究最终明确,AB 堆垛的二元二维材料双层通过层间横向滑移能 实现可逆极化 [21] ,被称为滑移铁电性。由于其将二维铁电性扩展到更广泛的材料组成范围 [22][23][24][25] , 并引入了机械运动和电性能之间的新型耦合 [26][27][28][29][30] ,因此引起了人们浓厚的兴趣。然而,所有已报 道的滑移铁电体的实例所具有的固有电极化强度均较小。由于固有的弱层间范德华相互作用,其 电极化强度比体块材料低大约一个数量级。因此,如何有效地增强滑移铁电体的电极化仍然是一 个亟待解决的问题。 由于二维材料具有优异的力学性能, 弹性应变已被证明是调节其物理 [31][32][33][34][35][36][37][38][39] 和化学 [40][41][42][43][44][45] Page 2 of 15 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 3 vdW-DF2 方法考虑色散力修正 [56] ,采用 Berry 相法计算晶体的极化 [ [27] 。这种独特的反转机制引入了 ABA 堆垛的中间态, Page 5 of 15 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 Page 8 of 15 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 Page 9 of 15 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 Page 11 of 15 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 Page 12 of 15 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 Page 13 of 15 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 Page 14 of 15 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 15 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 ...

High-Performance Sliding Ferroelectric Transistor Based on Schottky Barrier Tuning
  • Citing Article
  • May 2023

Nano Letters

... Therefore, the occurrence of river capture between Shimian and Mianning assuming southward flow of the paleo-Dadu River from the Shimian to the Anning River has been suggested (Deng B et al., 2020;Yang R et al., 2020). However, the timing and events responsible for the capture of the Dadu River are still debated, and there are few constraints on when the capture occurred resulting in the current drainage system (Zheng Y et al., 2023). Clark MK et al. (2004) first suggested that the paleo-Dadu originally drained into the Anning River, then joined in the Yangtze River at Panzhihua. ...

Mid-Pleistocene drainage rearrangement of the Dadu River in response to plate convergence in southeastern Tibet
  • Citing Article
  • March 2023

Quaternary Research

... In 2003 the milestone value of the static piezoelectric constant (d 33 ∼ 416 pC/N) and dynamic piezoelectric constant (d 33 * ∼ 750 pm/V) was reported by Saito et al. [3] in the lead-free (K,Na)NbO 3 (KNN) textured ceramics. Recently, Liu et al. [32] achieved thermally stable high d 33 ∼ 330±33 pC/N and d 33 * ∼590±59 pm/V) in the rare-earth-doped KNN polycrystalline ceramics. A record high d 33 * ≈ 1250 pm/V was achieved under a small electric field of 20 kV/cm in the Sr-doped KNN ceramics synthesized by a conventional solid-state reaction process [33]. ...

(K,Na)NbO3-based lead-free ceramics with enhanced temperature-stable piezoelectricity and efficient red luminescence

Journal of Advanced Ceramics