Yao Yao's research while affiliated with City University of Hong Kong and other places

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Publications (17)


Precursor-Confined Chemical Vapor Deposition of 2D Single-Crystalline SexTe1-x Nanosheets for p-Type Transistors and Inverters
  • Article

June 2024

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16 Reads

ACS Nano

Haoxin Huang

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Jiajia Zha

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Songcen Xu

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[...]

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Chaoliang Tan
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Structural characterization of the 4H-Au@1T′-WSe2 NWs
a, STEM image of the tip area of a 4H-Au@1T′-WSe2 NW. b,c, High-magnification HAADF-STEM images taken from the light blue dashed area (b) and light blue area (c) of the 4H-Au@1T′-WSe2 NW in a. d,e, The corresponding FFT patterns recorded in the pink dashed area (d) in b and the pink area (e) in c, respectively. f-j, STEM image (f) and the corresponding EDS elemental mappings of Au+W+Se (g), Au (h), W (i) and Se (j) of a segment of 4H-Au@1T′-WSe2 NW. k, Atomic-resolution HAADF-STEM image showing the interface between 1T′-WSe2 ML and 4H-Au NW. l, The corresponding integrated pixel intensity profiles of 1T′-WSe2 ML in red rectangle and 4H-Au NW in blue rectangle in Unit 2 in k.
Structural characterization of the 4H-Au@1T′-MoS2 NWs
a, STEM image of a representative 4H-Au@1T′-MoS2 NW. b, HAADF-STEM image of the 4H-Au@1T′-MoS2 NW recorded in the light blue area in a. c, The corresponding FFT pattern recorded in the pink area in b. d, Atomic-resolution HAADF-STEM image of a segment of a representative 4H-Au@1T′-MoS2 NW. e, Intensity profile along the red line in d, confirming the structure of 1T′-MoS2 ML. f, Atomic-resolution HAADF-STEM image showing the interface between 1T′-MoS2 ML and 4H-Au NW.
Structural characterization of the 4H-Au@1T′-MoSe2 NWs
a, STEM image of a representative 4H-Au@1T′-MoSe2 NW. b, HAADF-STEM image of the 4H-Au@1T′-MoSe2 NW recorded in the light blue area in a. c, The corresponding FFT pattern recorded in the pink area in b. d, Atomic-resolution HAADF-STEM image of a segment of a representative 4H-Au@1T′-MoSe2 NW. e, Intensity profile along the red line in d, confirming the structure of 1T′-MoSe2 ML. f, Atomic-resolution HAADF-STEM image showing the interface between 1T′-MoSe2 ML and 4H-Au NW.
In situ ABF-STEM images taken from a 4H-Au@1T′-WSe2 NW at different temperatures
a-i, In situ ABF-STEM images recorded at 100 (a), 200 (b), 300 (c), 400 (d), 500 (e), 600 (f), 700 (g), 800 (h) and 900 °C (i), respectively. As shown in Extended Data Fig. 4a–h, even the temperature increases to 800 °C, the WSe2 ML on 4H-Au still maintains the pure 1T′ phase. However, at 900 °C, the phase of WSe2 ML has changed from 1T′ to 1H (Extended Data Fig. 4i). The aforementioned results confirm that the phase transition temperature of 1T′-WSe2 ML on 4H-Au NW is much higher than that previously reported on 1T′-WSe2 crystals (~160.1 °C)¹⁷, indicating an important role of 4H-Au NWs on the stabilization of the grown 1T′-WSe2 MLs.
XANES and EXAFS characterizations of 4H-Au@1T′-WS2 NWs
a-c, Normalized S K-edge XANES spectra (a), Fourier transformed (FT) of S K-edge EXAFS spectra in R space (b) and the corresponding fitting results (c) of the as-prepared 4H-Au@1T′-WS2 NWs, 1T′-WS2 crystals and commercial 2H-WS2. The S K-edge XANES and EXAFS spectra (Extended Data Fig. 5) corroborate the strong Au-S interaction, that is, Au-S bonds, between 4H-Au NW and 1T′-WS2 ML.

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1T′-transition metal dichalcogenide monolayers stabilized on 4H-Au nanowires for ultrasensitive SERS detection
  • Article
  • Publisher preview available

April 2024

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175 Reads

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1 Citation

Nature Materials

Unconventional 1T′-phase transition metal dichalcogenides (TMDs) have aroused tremendous research interest due to their unique phase-dependent physicochemical properties and applications. However, due to the metastable nature of 1T′-TMDs, the controlled synthesis of 1T′-TMD monolayers (MLs) with high phase purity and stability still remains a challenge. Here we report that 4H-Au nanowires (NWs), when used as templates, can induce the quasi-epitaxial growth of high-phase-purity and stable 1T′-TMD MLs, including WS2, WSe2, MoS2 and MoSe2, via a facile and rapid wet-chemical method. The as-synthesized 4H-Au@1T′-TMD core–shell NWs can be used for ultrasensitive surface-enhanced Raman scattering (SERS) detection. For instance, the 4H-Au@1T′-WS2 NWs have achieved attomole-level SERS detections of Rhodamine 6G and a variety of severe acute respiratory syndrome coronavirus 2 (SARS-CoV-2) spike proteins. This work provides insights into the preparation of high-phase-purity and stable 1T′-TMD MLs on metal substrates or templates, showing great potential in various promising applications.

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Schematic illustration of the synthesis of vertical 1H/1T′ MoS2 heterophase structures.
Structure characterizations of 1H/1T′ MoS2 heterophase structures. a) TEM image of a 1H/1T′ MoS2 heterophase structure. b) Schematic of the 1H/1T′ MoS2 heterophase structure. c) HAADF‐STEM image of the cross‐section of the interface between 1H‐MoS2 (bottom) and 1T′‐MoS2 (top) in the 1H/1T′ MoS2 heterophase structure. d,e) HRTEM images of 1H‐MoS2 (d) and 1T′‐MoS2 (e) obtained from the 1H/1T′ MoS2 heterophase structure. f,g) Atomically resolved filtered STEM images of 1H‐MoS2 (f) and 1T′‐MoS2 (g) obtained from the 1H/1T′ MoS2 heterophase structure. Insets: The corresponding SAED patterns of 1H‐MoS2 (f) and 1T′‐MoS2 (g). h) Dark‐field HRTEM image of a 1H/1T′ MoS2 heterophase structure. i‐k) The corresponding elemental mapping images of the 1H/1T′ MoS2 heterophase structure in (h): Mo L signals (i), S K signals (j), and overlap of Mo L and S K signals (k).
Characterizations of 1H/1T′ MoS2 heterophase structures. a) Raman spectra of 1H‐MoS2 (pink curve) and 1T′‐MoS2 (blue curve). Inset: Raman mapping images of the 1H‐MoS2 (left) and 1T′‐MoS2 (right). b) PL spectra of 1H‐MoS2 (pink curve) and 1T′‐MoS2 (blue curve). c,d) Experimental (open circles) and fitted (solid lines) high‐resolution XPS spectra of Mo 3d (c) and S 2p (d) orbits of 1H‐MoS2 and 1H/1T′ MoS2. The pink and blue lines belong to the 1H and 1T′ phases, respectively.
Devices based on the 1H/1T′ MoS2 heterophase structure. a) Optical image of the fabricated device. b) Transfer curve of the device. Inset: schematic illustration of the fabricated transistor. c) The corresponding Ids–Vds output characteristics under different back‐gate voltages. d) Photoswitching characteristics of the device measured at a constant Vg of −20 V under 532 nm laser irradiation. e) Photoswitching characteristics measured under a constant Vds of −0.1 V and light illumination at different wavelengths (405, 532, and 635 nm).
Phase‐Controlled Growth of 1T′‐MoS2 Nanoribbons on 1H‐MoS2 Nanosheets

December 2023

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88 Reads

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7 Citations

Advanced Materials

Advanced Materials

2D heterostructures are emerging as alternatives to conventional semiconductors, such as silicon, germanium, and gallium nitride, for next‐generation electronics and optoelectronics. However, the direct growth of 2D heterostructures, especially for those with metastable phases still remains challenging. To obtain 2D transition metal dichalcogenides (TMDs) with designed phases, it is highly desired to develop phase‐controlled synthetic strategies. Here, a facile chemical vapor deposition method is reported to prepare vertical 1H/1T′ MoS2 heterophase structures. By simply changing the growth atmosphere, semimetallic 1T′‐MoS2 can be in situ grown on the top of semiconducting 1H‐MoS2, forming vertical semiconductor/semimetal 1H/1T′ heterophase structures with a sharp interface. The integrated device based on the 1H/1T′ MoS2 heterophase structure displays a typical rectifying behavior with a current rectifying ratio of ≈10³. Moreover, the 1H/1T′ MoS2‐based photodetector achieves a responsivity of 1.07 A W⁻¹ at 532 nm with an ultralow dark current of less than 10⁻¹¹ A. The aforementioned results indicate that 1H/1T′ MoS2 heterophase structures can be a promising candidate for future rectifiers and photodetectors. Importantly, the approach may pave the way toward tailoring the phases of TMDs, which can help us utilize phase engineering strategies to promote the performance of electronic devices.





Ultrahigh supercurrent density in a two-dimensional topological material

July 2023

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168 Reads

Physical Review Materials

Ongoing advances in superconductors continue to revolutionize technology thanks to the increasingly versatile and robust availability of lossless supercurrents. In particular, high supercurrent density can lead to more efficient and compact power transmission lines, high-field magnets, as well as high-performance nanoscale radiation detectors and superconducting spintronics. Here, we report the discovery of an unprecedentedly high superconducting critical current density (17MA/cm2 at 0 T and 7MA/cm2 at 8 T) in 1T′−WS2, exceeding those of all reported two-dimensional superconductors to date. 1T′−WS2 features a strongly anisotropic (both in- and out-of-plane) superconducting state that violates the Pauli paramagnetic limit signaling the presence of unconventional superconductivity. Spectroscopic imaging of the vortices further substantiates the anisotropic nature of the superconducting state. More intriguingly, the normal state of 1T′−WS2 carries topological properties. The band structure obtained via angle-resolved photoemission spectroscopy and first-principles calculations points to a Z2 topological invariant. The concomitance of topology and superconductivity in 1T′−WS2 establishes it as a topological superconductor candidate, which is promising for the development of quantum computing technology.


Reversible Semimetal-Semiconductor Transition of Unconventional-Phase WS2 Nanosheets

June 2023

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168 Reads

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7 Citations

Journal of the American Chemical Society

Phase transition with band gap modulation of materials has gained intensive research attention due to its various applications, including memories, neuromorphic computing, and transistors. As a powerful strategy to tune the crystal phase of transition-metal dichalcogenides (TMDs), the phase transition of TMDs provides opportunities to prepare new phases of TMDs for exploring their phase-dependent property, function, and application. However, the previously reported phase transition of TMDs is mainly irreversible. Here, we report a reversible phase transition in the semimetallic 1T'-WS2 driven by proton intercalation and deintercalation, resulting in a newly discovered semiconducting WS2 with a novel unconventional phase, denoted as the 1T'd phase. Impressively, an on/off ratio of >106 has been achieved during the phase transition of WS2 from the semimetallic 1T' phase to the semiconducting 1T'd phase. Our work not only provides a unique insight into the phase transition of TMDs via proton intercalation but also opens up possibilities to tune their physicochemical properties for various applications.


Te‐based MFMIS device. a) Schematic illustration of the MFMIS device, where Te nanoflake serves as the channel material, and the insulating h‐BN layer places between Te nanoflake and Gr layer, which is on the top of the ferroelectric dielectric layer CIPS. At the bottom of the vdW heterostructure, Au is used as the bottom gate. b) Optical microscope image of a typical MFMIS device. Different materials are indicated by dashed curves with different colors. Scale bar, 10 µm. c) Height profiles of the materials in the heterostructure in (b) measured by AFM. d) Raman spectra of Te, h‐BN, Gr, CIPS, and CIPS/Gr/h‐BN/Te heterostructure. e) HRTEM image of the cross section in the fabricated MFMIS device. f) STEM image of the area indicated by the pink dashed box in (e).
Electrical pulse triggered memory behavior of the MFMIS device. a) Transfer curve of the MFMIS device under the bias of 100 mV. b) Output curves of the MFMIS device. The back‐gate voltage Vbg increases from −5 V to 5 V with a step of 1 V. c–e) Evolution of the channel conductance variation of the MFMIS device triggered by electrical pulses with c) different pulse width (amplitude: −4 V), d) different amplitude (pulse width: 1 ms, pulse interval: 1 s), and e) different pulse number (amplitude: −5 V, pulse width: 1 ms, pulse interval: 1 s). The readout bias was kept as 100 mV and the internal gate was floating. f) Evolution of the channel conductance variation of the memory device (the top panel) triggered by programmed electrical pulse sequence (the bottom panel) with different pulse widths (1 ms (dark cyan) and 5 ms (pink)).
Schematic demonstration of the electronic memory behaviors of the MFMIS device. a–c) Low resistance of Te channel induced by a negative electrical pulse (Vg < 0 V). a) The negative electrical pulse input on the bottom gate leads to the downward polarization in the CIPS layer. b) When the electrical pulse is removed, the downward polarization in the CIPS layer could be maintained to keep the low resistance of Te channel. c) The band diagram and the charge distribution in different layers after the excitation of the negative electrical pulse. d–f) High resistance of Te channel induced by a positive electrical pulse (Vg > 0 V). d) The positive electrical pulse induces the upward polarization in CIPS layer. e) The high resistance of Te channel is kept by the upward polarization in CIPS layer after removing the positive electrical pulse. f) The band diagram and the charge distribution in different layers after the excitation of the positive electrical pulse. g–i) Resistance evolution of Te channel induced by IR laser. g) Under the excitation of the laser pulse, the photogenerated holes are accumulated in Te channel, inducing the metastable downward polarization in CIPS layer. h) The induced metastable downward polarization can maintain the low‐resistance state of Te channel after removing the IR laser. i) The resistance of Te channel gradually returns to its initial value due to the relaxation of the metastable polarization.
1550‐nm laser pulse triggered memory behavior of the MFMIS device. a) 1550‐nm laser pulse triggered channel conductance variation with different laser power (pulse width: 10 ms). b) 1550‐nm laser pulse triggered channel conductance variation with different pulse number (pulse width: 10 ms, pulse interval: 90 ms, laser power: 623.1 nW). c) Channel conductance variation triggered by paired optical pulses with different interval (pulse width: 10 ms, laser power: 623.1 nW). d) PPF ratio defined as (A2−A1)/A1×100%\[({A_2} - {A_1})/{A_1} \times 100\ as a function of the pulse interval, where the blue line is the fitting curve using the double exponential decay function. Inset: PPF effect induced by paired optical pulse. e) Multiple conductance state variation triggered by 1550‐nm pulse train. The laser power, pulse width, and pulse interval were 623.1 nW, 1 ms, and 9 ms, respectively. f) Zoom‐in conductance variation evolution triggered by the first 10 laser pulses indicated by transparent royal in (e). The readout bias was kept as Vds = 100mVand both internal gate and bottom gate were floating.
In‐sensor RC system at the optical communication band based on the MFMIS device. a) Schematic illustration of the RC system for classifying the MNIST dataset (MFMIS: MFMIS device; MOSFET: metal‐oxide‐semiconductor field‐effect transistor). b) Confusion matrix on classifying the MNIST test set. c) In‐situ learning performance of the RC network over epochs, using 60 000 handwritten digits for training and 10 000 digits for testing. The pink and cyan dots correspond to the classification accuracy of software and MFMIS device‐based RC system, respectively. d) Initial (top panel)/final (bottom panel) device crossbar array conductance before/after training. e) Initial (top panel)/final (bottom panel) corresponding device crossbar array conductance distributions of d) before/after training. f) Dimensionality reduction of optoelectronic reservoir outputs using linear discriminative analysis (LDA). g) Number of training operations for RC, artificial neural network (ANN) without hidden layer and with one hidden layer, respectively, showing RC significantly reduces the training complexity.
Electronic/Optoelectronic Memory Device Enabled by Tellurium-based 2D van der Waals Heterostructure for in-Sensor Reservoir Computing at the Optical Communication Band

March 2023

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320 Reads

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39 Citations

Advanced Materials

Advanced Materials

Although two-dimensional (2D) materials have been widely explored for data storage and neuromorphic computing, the construction of 2D material-based memory devices with optoelectronic responsivity in the short-wave infrared (SWIR) region for in-sensor reservoir computing (RC) at the optical communication band still remains a big challenge. In this work, we report an electronic/optoelectronic memory device enabled by tellurium-based 2D van der Waals (vdW) heterostructure, where the ferroelectric CuInP2S6 and tellurium channel endow this device with both the long-term potentiation/depression by voltage pulses and short-term potentiation by 1550-nm laser pulses (a typical wavelength in the conventional fiber optical communication band). Leveraging the rich dynamics, we demonstrate a fully memristive in-sensor RC system that can simultaneously sense, decode and learn messages transmitted by optical fibers. The reported 2D vdW heterostructure-based memory featuring both the long-term and short-term memory behaviors using electrical and optical pulses in SWIR region has not only complemented the wide spectrum of applications of 2D materials family in electronics/optoelectronics but also paves the way for future smart signal processing systems at the edge. This article is protected by copyright. All rights reserved


Citations (10)


... Wet-chemical synthesis is also a popular bottom-up approach to synthesizing nanomaterials. Li et al. realized the synthesis of high-purity and stable 1T ′ -MoS 2 , MoSe 2 , WS 2 , and WSe 2 monolayers via the wet-chemical method using 4H-Au nanowires as templates (Figure 5e) [67]. The strong interaction between the template and TMDC monolayers, and charge doping from the solution and the template stabilize the 1T ′ phase. ...

Reference:

A Mini Review: Phase Regulation for Molybdenum Dichalcogenide Nanomaterials
1T′-transition metal dichalcogenide monolayers stabilized on 4H-Au nanowires for ultrasensitive SERS detection

Nature Materials

... According to the above discussion, phase transformation can occur mainly in two ways, electronic doping and mechanical shift. Many techniques can realize these two mechanisms, and basically, we divide them into two categories, direct synthesis [56] and post processing [57,58]. ...

Phase Engineering of Nanomaterials: Transition Metal Dichalcogenides
  • Citing Article
  • March 2024

Chemical Reviews

... However, traditional antioxidants, owing to their low bioavailability and inability to breach the blood-brain barrier, are primarily responsible for failures in clinical translation and do not satisfy the clinical treatment requirements for ischemic stroke [72]. Compared to traditional antioxidants, nanomedicine can effectively improve the disadvantages of small molecule and biologic antioxidant agents. ...

Recent Progress on Phase Engineering of Nanomaterials
  • Citing Article
  • November 2023

Chemical Reviews

... On the other hand, when doping MoS2 with donor atoms, the additional electron occupation decreases the stability of 1H-MoS2 but increases the stability of 1T-MoS2. Therefore, based on the electronic doping mechanism, electrons doping to 1H-MoS2 directly cause a phase transition to the 1T phase [45]. The phase transformation mechanism between the 1H and 1T' phases is similar. ...

Phase‐Controlled Growth of 1T′‐MoS2 Nanoribbons on 1H‐MoS2 Nanosheets
Advanced Materials

Advanced Materials

... Specifically, substantial drain-source currents were only detected when the bias voltage between the TMD and gold exceeded the Schottky barrier. 15,18,24,25,47 Here, we hypothesize that the efficiency of pump-induced gold-to-WS 2 charge injection varies with the pump photon energy. By sweeping the pump photon energy from above to below the SBH, we expect the charge injection efficiency to decrease substantially, thereby permitting the determination of the SBH. ...

Reversible Semimetal-Semiconductor Transition of Unconventional-Phase WS2 Nanosheets
  • Citing Article
  • June 2023

Journal of the American Chemical Society

... The development of two-dimensional material-based memory devices with optoelectronic responsivity in the short-wave infrared (SWIR) region, particularly for in-sensor RC at the optical communication band, presents a significant challenge. Zha et al. 163 have addressed this challenge by introducing an electronic/optoelectronic memory device based on a tellurium-containing two-dimensional van der Waals heterostructure. Operating in the SWIR region, this device can sense and process photon signals within the optical communication band. ...

Electronic/Optoelectronic Memory Device Enabled by Tellurium-based 2D van der Waals Heterostructure for in-Sensor Reservoir Computing at the Optical Communication Band
Advanced Materials

Advanced Materials

... The template-assisted method provides a unique avenue for researchers to create intricate material architectures with precise control. For instance, this technique entails the transformation of layered 2D materials into nonlayered 2D structures or Janus structures, wherein two distinct surfaces or layers exhibit differing properties or functionalities [105][106][107]. Another variant of the templating method involves employing a material possessing a specific structure as a template. ...

Preparation of 2D Molybdenum Phosphide via Surface‐Confined Atomic Substitution
Advanced Materials

Advanced Materials

... d-i, In situ ABF-STEM images taken from a 4H-Au@1T′-WS 2 NW at 200 °C (d), 300 °C (e), 400 °C (f), 500 °C (g), 600 °C (h) and 700 °C (i), respectively.Content courtesy of Springer Nature, terms of use apply. . 7a) due to the different phases34 . The Fourier transform (FT) of EXAFS spectra in R space(Fig. ...

Salt‐Assisted 2H‐to‐1T′ Phase Transformation of Transition Metal Dichalcogenides
Advanced Materials

Advanced Materials

... Elemental doping, surface coating, and structural engineering have been proved as effective strategies to improve electrochemical performance of Na x MnO 2 cathode materials [9,[11][12][13]. ...

Layered-tunnel structured cathode for high performance sodium-ion batteries
  • Citing Article
  • February 2020

Functional Materials Letters

... There are many strategies to prepare NCM cathode materials nowadays. Usually, the precursors are first prepared by wet-chemical methods (mainly including coprecipitation, 18,19 sol−gel, 20,21 hydrothermal, 22,23 and spray pyrolysis 24,25 ) and then sintered with a lithium source (LiOH or Li 2 CO 3 ) at high temperature by a solid-state reaction. Coprecipitation, which is convenient for large-scale production, is currently the most widely used method to synthesize Ni-rich hydroxide precursors in either laboratory investigation or industrial production. ...

3D LiCoO2 Nanosheets Assembled Nanorod Arrays via Confined Dissolution-Recrystallization for Advanced Aqueous Lithium-Ion Batteries
  • Citing Article
  • November 2018

Nano Energy