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Neoarm

Manufactured by JEOL
Sourced in Japan

The NEOARM is a high-performance scanning electron microscope (SEM) produced by JEOL. It is designed to provide detailed and high-resolution imaging of a wide range of samples. The NEOARM features advanced electron optics and a modular design, allowing for customization to meet the needs of various research and industrial applications.

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17 protocols using neoarm

1

Transmission Electron Microscopy of Samples

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Transmission electron microscopy was performed with two microscopes (JEOL JEM-F200 and an aberration-corrected JEOL NEOARM), both operating at 200 kV and in scanning transmission electron microscopy (STEM) mode. For ex situ studies, the sample was diluted in isopropanol and deposited on a lacey carbon film on copper grids. For in situ studies, an environmental holder for gas flow experiments manufactured by Hummingbird Scientific was used. The sample was enclosed in a microchip, made of two SiN windows and a micro electro-mechanical system for temperature control. The mass flow of gases was controlled using a gas system and a software provided by the same company.
Energy-dispersive X-ray spectroscopy (EDS) was performed with JEOL NEOARM and the maps were obtained with DigitalMicrograph by Gatan Inc (pixel time = 0.04 s and pixel size = 1.4 Å).
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2

Characterization of IrOx Catalysts

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A field emission JSM-IT700HR scanning electron microscope (SEM) with energy-dispersive X-ray spectroscopy (EDS) and Hitachi HF3300 transmission electron microscopy (TEM) was used to characterize the morphology and composition of the catalysts. A Rigaku SmartLab X-ray diffraction (XRD) system was used to analyze the catalyst's crystalline structure. With a Quantum 2000 Scanning ESCA Microprobe and a monochromatic Al Kα X-ray source, the X-ray photoelectron spectroscopy (XPS) was conducted. Survey scans were collected between 0 and 1350 eV. All the peak shift corrections were done with C 1s at 284.8 eV. With an operation accelerating voltage of 80 kV, the material phase of IrOx catalysts was studied by scanning transmission electron microscopy (STEM) on a probe-corrected JEOL NEOARM.
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3

Detailed Characterization of Zeolite Catalysts

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Aberration-corrected HAADF-STEM imaging
was performed on a probe-corrected JEOL NEOARM operated at 80 kV.
Dry powder specimens suspended on a Cu grid with a lacey carbon support
were used for HAADF-STEM characterization. Scanning electron microscopy
(SEM) was conducted on a Quanta 3D DualBeam FEG FIB-SEM with EDS analyzer
to observe the zeolite morphology. Nitrogen sorption isotherms were
measured at 77 K on a Micromeritics ASAP 2020 Plus (USA). The Brunauer–Emmett–Teller
(BET) method was utilized to calculate the specific surface areas.
Diffuse reflectance infrared Fourier transform spectroscopy (DRIFTS)
measurements were performed on a Thermo Nicolet 6700 instrument with
a Hg-Cd-Te (MCT) detector and a Praying Mantis high-temperature reaction
chamber with KBr windows. The catalysts were pretreated with 100 mL/min
of 10% O2/He at 400 °C for 30 min and then reduced
by 10% H2/He at 200 °C for 30 min. The CO adsorption
was performed at room temperature. Briefly, 5% CO/He was introduced
into the DRIFTS cell at a flow rate of 100 mL/min. After the CO saturation,
a helium purge at a flow rate of 100 mL/min was performed to remove
gas-phase CO from the DRIFTS cell. All of the spectra were recorded
using 32 scans and a resolution of 4 cm–1.
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4

Pt-NS Catalyst Structural Analysis

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A field emission JSM-IT700HR scanning electron microscope (SEM) with energy-dispersive X-ray spectroscopy (EDS) was used to characterize the morphology and composition of the samples. A Rigaku SmartLab X-ray diffraction (XRD) system was used to investigate the crystalline structure of the sample. The crystalline structure of Pt-NS catalysts was investigated by scanning transmission electron microscopy (STEM) on a probe-corrected JEOL NEOARM operated at an accelerating voltage of 80 kV.
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5

Electron microscopy analysis of nanostructures

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Sample solutions were drop cast on a continuous carbon-coated copper grids with 400 mesh (Ted Pella). The grids were then dried with filter paper and sealed away from moisture before experiments. JEOL NEOARM was operated at 80 kV in low beam conditions. A spot size of 5 and low screen brightness was combined to perform TEM studies with minimum radiation damage from the electron beam. Image J was used to extract plot profiles from the TEM images and make measurements on domain sizes. Ten measurements were performed for each sample.
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6

Ir1-xVxO2 Nanowire Characterization

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The morphologies of the Ir1 −xVxO2 nanowires were characterized with a scanning electron microscope (SEM, Quanta FEI and Zeiss Auriga 60), and the structure and growth orientations were characterized via TEM (JEOL 3200 TEM), and the chemical composition of the nanowires determined with XEDS in the SEM, JEOL 3200 TEM, and NEOARM atomic resolution analytical electron microscope by JEOL. The Raman spectra were collected at room temperature with a Renishaw inVia confocal Raman microscope system with a 532 nm excitation laser with a nominal laser power of 50 µW and calibrated with a reference Si peak at 520 cm−1.
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7

Structural Characterization of Annealed Samples

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Before imaging, samples exposed to salt solution were annealed at 300 °C for 90 min in Ar/H2. Dark-field images were acquired on a probe-corrected JEOL NEOARM operating at 200 kV with a high-angle annular dark-field (HAADF) detector. EELS spectra were acquired on a GIF Quantum Summit detector with a resolution of 0.5 eV. The 80–90 square pixel EELS maps were acquired with an acquisition time of 0.2–0.5 s/pixel.
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8

In Situ TEM Oxidation Study

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We performed in situ TEM heating experiments with the HEA samples under under study to intentionally accelerate the surface oxidation of thin TEM foils. The in situ TEM heating experiments were performed using a Gatan heating holder equipped with water connection on a conventional TEM (JEOL JEM-2010 without any correctors) equipment at 500 °C for 20 min. Afterwards, the surface oxidation of the TEM lamellar was examined using HRTEM and STEM modes in an atomic-resolution TEM (JEOL NEO-ARM) to accurately distinguish the SRO-derived diffuse scattering from the oxidation-induced reflections in the EDPs.
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9

Characterization of HfO2 and ZrO2 Thin Films

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The thickness and refractive index of the deposited single oxides of HfO2 and ZrO2 and the HZO thin films were evaluated using an ellipsometer (Elli-SE, Ellipso technology, Suwon, Korea). The shape of the thin film cross-section and the elemental composition were analyzed using transmission electron microscopy (TEM) (NEO ARM, JEOL, Tokyo, Japan) and energy-dispersive spectroscopy (EDS) (JED-2300T, JEOL, Tokyo, Japan), respectively. The crystalline structure of the HZO thin films was measured by high-resolution X-ray diffraction (HR-XRD) (Smartlab, Rigaku, Tokyo, Japan) in Bragg–Brentano geometry, and the density of the thin film was calculated through X-ray reflectometry (XRR) analysis on the same instrument. Electrical properties such as the P-E curve and fatigue endurance of the thin film were evaluated using a TF analyzer (TF-2000E, aixACCT, Aachen, Germany) connected to a microprobe station (APX-6B, WIT, Suwon, Korea). Hysteresis loop measurements were performed at a frequency of 1 kHz with a triangle pulse of ±3 V. Fatigue endurance measurements were conducted by the continuous application of a square pulse of ±3 V at 10 kHz along with a 1 kHz triangle pulse that was applied five times at each time point to measure remnant polarization.
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10

HAADF-STEM Characterization of Nanostructures

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TEM was performed with a JEOL NEOARM operating at 200 kV. All images are high-angle annular dark-field scanning transmission electron microscopy (HAADF-STEM) data. The diameter of the used condenser lens aperture was 40 μm, the probe current was 150 pA, and the camera length was 4 cm. EDS was performed with two detectors provided by JEOL Ltd. and the maps were obtained with DigitalMicrograph, a software developed by Gatan Inc.
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