9 research outputs found

    Electron Microscopy Observation of TiO<sub>2</sub> Nanocrystal Evolution in High-Temperature Atomic Layer Deposition

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    Understanding the evolution of amorphous and crystalline phases during atomic layer deposition (ALD) is essential for creating high quality dielectrics, multifunctional films/coatings, and predictable surface functionalization. Through comprehensive atomistic electron microscopy study of ALD TiO<sub>2</sub> nanostructures at designed growth cycles, we revealed the transformation process and sequence of atom arrangement during TiO<sub>2</sub> ALD growth. Evolution of TiO<sub>2</sub> nanostructures in ALD was found following a path from amorphous layers to amorphous particles to metastable crystallites and ultimately to stable crystalline forms. Such a phase evolution is a manifestation of the Ostwaldā€“Lussac Law, which governs the advent sequence and amount ratio of different phases in high-temperature TiO<sub>2</sub> ALD nanostructures. The amorphousā€“crystalline mixture also enables a unique anisotropic crystal growth behavior at high temperature forming TiO<sub>2</sub> nanorods via the principle of vapor-phase oriented attachment

    Atom Probe Tomography Analysis of Ag Doping in 2D Layered Material (PbSe)<sub>5</sub>(Bi<sub>2</sub>Se<sub>3</sub>)<sub>3</sub>

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    Impurity doping in two-dimensional (2D) materials can provide a route to tuning electronic properties, so it is important to be able to determine the distribution of dopant atoms within and between layers. Here we report the tomographic mapping of dopants in layered 2D materials with atomic sensitivity and subnanometer spatial resolution using atom probe tomography (APT). APT analysis shows that Ag dopes both Bi<sub>2</sub>Se<sub>3</sub> and PbSe layers in (PbSe)<sub>5</sub>(Bi<sub>2</sub>Se<sub>3</sub>)<sub>3</sub>, and correlations in the position of Ag atoms suggest a pairing across neighboring Bi<sub>2</sub>Se<sub>3</sub> and PbSe layers. Density functional theory (DFT) calculations confirm the favorability of substitutional doping for both Pb and Bi and provide insights into the observed spatial correlations in dopant locations

    Rapid Wafer-Scale Growth of Polycrystalline 2H-MoS<sub>2</sub> by Pulsed Metalā€“Organic Chemical Vapor Deposition

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    High-volume manufacturing of devices based on transition metal dichalcogenide (TMD) ultrathin films will require deposition techniques that are capable of reproducible wafer-scale growth with monolayer control. To date, TMD growth efforts have largely relied upon sublimation and transport of solid precursors with minimal control over vapor-phase flux and gas-phase chemistry, which are critical for scaling up laboratory processes to manufacturing settings. To address these issues, we report a new pulsed metalā€“organic chemical vapor deposition (MOCVD) route for MoS<sub>2</sub> film growth in a research-grade single-wafer reactor. Using bisĀ­(<i>tert</i>-butylimido)Ā­bisĀ­(dimethylamido)molybdenum and diethyl disulfide, we deposit MoS<sub>2</sub> films from āˆ¼1 nm to āˆ¼25 nm in thickness on SiO<sub>2</sub>/Si substrates. We show that layered 2H-MoS<sub>2</sub> can be produced at comparatively low reaction temperatures of 591 Ā°C at short deposition times, approximately 90 s for few-layer films. In addition to the growth studies performed on SiO<sub>2</sub>/Si, films with wafer-level uniformity are demonstrated on 50 mm quartz wafers. Process chemistry and impurity incorporation from precursors are also discussed. This low-temperature and fast process highlights the opportunities presented by metalā€“organic reagents in the controlled synthesis of TMDs

    Probing the Optical Properties and Strain-Tuning of Ultrathin Mo<sub>1ā€“<i>x</i></sub>W<sub><i>x</i></sub>Te<sub>2</sub>

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    Ultrathin transition metal dichalcogenides (TMDCs) have recently been extensively investigated to understand their electronic and optical properties. Here we study ultrathin Mo<sub>0.91</sub>W<sub>0.09</sub>Te<sub>2</sub>, a semiconducting alloy of MoTe<sub>2</sub>, using Raman, photoluminescence (PL), and optical absorption spectroscopy. Mo<sub>0.91</sub>W<sub>0.09</sub>Te<sub>2</sub> transitions from an indirect to a direct optical band gap in the limit of monolayer thickness, exhibiting an optical gap of 1.10 eV, very close to its MoTe<sub>2</sub> counterpart. We apply tensile strain, for the first time, to monolayer MoTe<sub>2</sub> and Mo<sub>0.91</sub>W<sub>0.09</sub>Te<sub>2</sub> to tune the band structure of these materials; we observe that their optical band gaps decrease by 70 meV at 2.3% uniaxial strain. The spectral widths of the PL peaks decrease with increasing strain, which we attribute to weaker excitonā€“phonon intervalley scattering. Strained MoTe<sub>2</sub> and Mo<sub>0.91</sub>W<sub>0.09</sub>Te<sub>2</sub> extend the range of band gaps of TMDC monolayers further into the near-infrared, an important attribute for potential applications in optoelectronics

    Nanoscale Heterogeneities in Monolayer MoSe<sub>2</sub> Revealed by Correlated Scanning Probe Microscopy and Tip-Enhanced Raman Spectroscopy

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    Understanding growth, grain boundaries (GBs), and defects of emerging two-dimensional (2D) materials is key to enabling their future applications. For quick, nondestructive metrology, many studies rely on confocal Raman spectroscopy, the spatial resolution of which is constrained by the diffraction limit (āˆ¼0.5 Ī¼m). Here we use tip-enhanced Raman spectroscopy (TERS) for the first time on synthetic MoSe<sub>2</sub> monolayers, combining it with other scanning probe microscopy (SPM) techniques, all with sub-20 nm spatial resolution. We uncover strong nanoscale heterogeneities in the Raman spectra of MoSe<sub>2</sub> transferred to gold substrates [one near 240 cm<sup>ā€“1</sup> (A<sub>1</sub>ā€²), and others near 287 cm<sup>ā€“1</sup> (Eā€²), 340 cm<sup>ā€“1</sup>, and 995 cm<sup>ā€“1</sup>], which are not observable with common confocal techniques and appear to imply the presence of nanoscale domains of MoO<sub>3</sub>. We also observe strong tip-enhanced photoluminescence (TEPL), with a signal nearly an order of magnitude greater than the far-field PL. Combining TERS with other SPM techniques, we find that GBs can cut into larger domains of MoSe<sub>2</sub>, and that carrier densities are higher at GBs than away from them

    Characterization of Few-Layer 1Tā€² MoTe<sub>2</sub> by Polarization-Resolved Second Harmonic Generation and Raman Scattering

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    We study the crystal symmetry of few-layer 1Tā€² MoTe<sub>2</sub> using the polarization dependence of the second harmonic generation (SHG) and Raman scattering. Bulk 1Tā€² MoTe<sub>2</sub> is known to be inversion symmetric; however, we find that the inversion symmetry is broken for finite crystals with even numbers of layers, resulting in strong SHG comparable to other transition-metal dichalcogenides. Group theory analysis of the polarization dependence of the Raman signals allows for the definitive assignment of all the Raman modes in 1Tā€² MoTe<sub>2</sub> and clears up a discrepancy in the literature. The Raman results were also compared with density functional theory simulations and are in excellent agreement with the layer-dependent variations of the Raman modes. The experimental measurements also determine the relationship between the crystal axes and the polarization dependence of the SHG and Raman scattering, which now allows the anisotropy of polarized SHG or Raman signal to independently determine the crystal orientation

    Electrolyte Stability Determines Scaling Limits for Solid-State 3D Li Ion Batteries

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    Rechargeable, all-solid-state Li ion batteries (LIBs) with high specific capacity and small footprint are highly desirable to power an emerging class of miniature, autonomous microsystems that operate without a hardwire for power or communications. A variety of three-dimensional (3D) LIB architectures that maximize areal energy density has been proposed to address this need. The success of all of these designs depends on an ultrathin, conformal electrolyte layer to electrically isolate the anode and cathode while allowing Li ions to pass through. However, we find that a substantial reduction in the electrolyte thickness, into the nanometer regime, can lead to rapid self-discharge of the battery even when the electrolyte layer is conformal and pinhole free. We demonstrate this by fabricating individual, solid-state nanowire coreā€“multishell LIBs (NWLIBs) and cycling these inside a transmission electron microscope. For nanobatteries with the thinnest electrolyte, ā‰ˆ110 nm, we observe rapid self-discharge, along with void formation at the electrode/electrolyte interface, indicating electrical and chemical breakdown. With electrolyte thickness increased to 180 nm, the self-discharge rate is reduced substantially, and the NWLIBs maintain a potential above 2 V for over 2 h. Analysis of the nanobatteriesā€™ electrical characteristics reveals space-charge limited electronic conduction, which effectively shorts the anode and cathode electrodes directly through the electrolyte. Our study illustrates that, at these nanoscale dimensions, the increased electric field can lead to large electronic current in the electrolyte, effectively shorting the battery. The scaling of this phenomenon provides useful guidelines for the future design of 3D LIBs

    Rydberg Excitons and Trions in Monolayer MoTe<sub>2</sub>

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    Monolayer transition metal dichalcogenide (TMDC) semiconductors exhibit strong excitonic optical resonances, which serve as a microscopic, noninvasive probe into their fundamental properties. Like the hydrogen atom, such excitons can exhibit an entire Rydberg series of resonances. Excitons have been extensively studied in most TMDCs (MoS2, MoSe2, WS2, and WSe2), but detailed exploration of excitonic phenomena has been lacking in the important TMDC material molybdenum ditelluride (MoTe2). Here, we report an experimental investigation of excitonic luminescence properties of monolayer MoTe2 to understand the excitonic Rydberg series, up to 3s. We report a significant modification of emission energies with temperature (4 to 300 K), thereby quantifying the excitonā€“phonon coupling. Furthermore, we observe a strongly gate-tunable excitonā€“trion interplay for all the Rydberg states governed mainly by free-carrier screening, Pauli blocking, and band gap renormalization in agreement with the results of first-principles GW plus Betheā€“Salpeter equation approach calculations. Our results help bring monolayer MoTe2 closer to its potential applications in near-infrared optoelectronics and photonic devices

    Vertical 2D/3D Semiconductor Heterostructures Based on Epitaxial Molybdenum Disulfide and Gallium Nitride

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    When designing semiconductor heterostructures, it is expected that epitaxial alignment will facilitate low-defect interfaces and efficient vertical transport. Here, we report lattice-matched epitaxial growth of molybdenum disulfide (MoS<sub>2</sub>) directly on gallium nitride (GaN), resulting in high-quality, unstrained, single-layer MoS<sub>2</sub> with strict registry to the GaN lattice. These results present a promising path toward the implementation of high-performance electronic devices based on 2D/3D vertical heterostructures, where each of the 3D and 2D semiconductors is both a template for subsequent epitaxial growth and an active component of the device. The MoS<sub>2</sub> monolayer triangles average 1 Ī¼m along each side, with monolayer blankets (merged triangles) exhibiting properties similar to that of single-crystal MoS<sub>2</sub> sheets. Photoluminescence, Raman, atomic force microscopy, and X-ray photoelectron spectroscopy analyses identified monolayer MoS<sub>2</sub> with a prominent 20-fold enhancement of photoluminescence in the center regions of larger triangles. The MoS<sub>2</sub>/GaN structures are shown to electrically conduct in the out-of-plane direction, confirming the potential of directly synthesized 2D/3D semiconductor heterostructures for vertical current flow. Finally, we estimate a MoS<sub>2</sub>/GaN contact resistivity to be less than 4 Ī©Ā·cm<sup>2</sup> and current spreading in the MoS<sub>2</sub> monolayer of approximately 1 Ī¼m in diameter
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