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Axis ultra dld x ray photoelectron spectrometer

Manufactured by Shimadzu
Sourced in United Kingdom, Japan

The Axis Ultra DLD X-ray photoelectron spectrometer is a laboratory instrument designed for surface analysis. It utilizes X-ray photoelectron spectroscopy (XPS) to provide detailed information about the chemical composition and electronic states of the surface of a sample.

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38 protocols using axis ultra dld x ray photoelectron spectrometer

1

Surface Characterization of IrO2/Ir-TiO2 Catalysts

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A JEOL 6300 microscope (JEOL Ltd, Akishima, Japan) equipped with an Oxford ISIS 2000 X-ray EDS (EDAX) system (Oxford Instruments Ltd, Oxford, UK) was used to obtain SEM micrographs and EDS elemental composition analysis. XPS measurements of (IrO2/Ir-TiO2)/Ti samples were performed at an AXIS Ultra DLD X-ray Photoelectron Spectrometer by Kratos Analytical, Wharfside, Manchester, UK, with a monochromated Al-Ka1 X-ray beam (λKa = 1.4866 Å). A 4 keV Ar+ ion beam helped to (a) remove adventitious carbon and other surface contaminants from the samples and (b) etch the samples at a specific depth (20 s of sputtering results in a ca. 1 nm material etching).
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2

Surface Characterization of Coated Aluminum Chips

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The surface morphology of the coated aluminum chips was examined using a scanning electron microscope (SEM, JEOL-7100), and surface element analysis was conducted with the in-build energy-dispersive X-ray spectroscopy system in the SEM (SEM-EDS, JEOL-7100). The surface roughness of the chips was characterized using atomic force microscopy (AFM) imaging (Dimension Icon). The elemental composition of the coated chip’s surface was also identified using X-ray photoelectron spectroscopy (XPS) with an Axis Ultra DLD X-ray photoelectron spectrometer (Kratos). Attenuated total reflection-Fourier-transform infrared spectroscopy (ATR-FTIR) for the surface of the chip was conducted with Vertex 70 Hyperion 1000 (Bruker).
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3

Structural Characterization of Thin Films

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The crystal structures of the Au, Ag, In, and Sn thin films were analyzed with a Rigaku Smartlab X-ray diffractometer (XRD) using Cu Kα radiation (40 kV, 40 mA). The near-surface compositions of the thin films were measured with a Kratos Axis Ultra DLD X-ray photoelectron spectrometer (XPS). All spectra were acquired using monochromatized Al Kα radiation (15 kV, 15 mA). The kinetic energy scale of the measured spectra was calibrated by setting the C 1s binding energy to 284.8 eV. The surface structure of those thin films was recorded using an FEI XL30 Sirion scanning electron microscope (SEM) at the 5 kV acceleration voltage, Everhart-Thornley detector, secondary electrons mode.
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4

Characterization of Carbon Dots

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The transmission electron microscopic (TEM) images were obtained on a JEOL JEM-2100F transmission electron microscopy (Tokyo, Japan). The X-ray photoelectron spectra (XPS) were recorded on a Kratos AXIS ULTRA DLD X-ray photoelectron spectrometer (Tokyo, Japan). The Fourier transform infrared spectra (FTIR) were acquired on a Bruker Tensor II FTIR spectrometer (Bremen, Germany). The UV-vis was performed on a Lambda 950 absorption spectrophotometer (PerkinElmer, Llantrisant, UK). Nanosecond fluorescence lifetime assays and photoluminescence spectra were recorded by FLS 980 fluorescence spectrometer steady-state model and time-correlated single-photon counting (TCSPC) system (Edinburgh Instruments Ltd, England), respectively. The quantum yields (QYs) of the as-prepared carbon dots were determined using quinine sulfate in 0.1 M H2SO4 (literature QYs: 54.6%) as the standard sample by comparing the integrated fluorescence intensities (excitation at 360 nm) and absorbance values at 360 nm of the carbon dots aqueous solutions with those of quinine sulfate, which was determined by FLS 980 spectrophotometer.26,27 (link)
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5

Comprehensive Characterization of ZnO Nanostructures

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FESEM images
of the precipitates were recorded using a Hitachi S-4800 field emission
scanning electron microscope (Hitachi Limited, Japan) with an operating
voltage of 5.0 kV. The samples were sputter-coated with Au for 25
s prior to imaging. TEM, HRTEM, SAED, and electron diffraction (EDX)
measurements were carried out using a JEM-2100 transmission electron
microscope (JEOL, Japan) at 200 kV. Powder XRD patterns were obtained
on a Rigaku D/max-2400 X-ray diffractometer (Japan) with Cu Kα
radiation (40 kV, 40 mA) at a scanning rate of 0.02°/s in the
2θ range from 10 to 80°. XPS experiments were performed
on a Kratos Axis UltraDLD X-ray photoelectron spectrometer (England)
with a monochrome X-ray source using AlKα (1486.6 eV) radiation.
The measured binding energies were corrected by referencing the C
1s line to 284.5 eV. TGA was carried out on a TGA/NETZSCH STA449 F3
instrument under a nitrogen atmosphere at a heating rate of 10 °C/min
from 27 °C to 800 °C. The Brunauer–Emmett–Teller
(BET) method was employed to calculate the specific surface areas
(SBET). The room-temperature photoluminescence
spectra were acquired on a Hitachi F-7000 luminescence spectrometer
using a Xe lamp with an excitation wavelength of 325 nm. The UV–vis
spectra of the ZnO samples were measured on a UV-1750 UV–vis
spectrophotometer.
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6

X-ray Photoelectron Spectroscopy of nMOF

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X-ray photoelectron spectroscopy (XPS) was performed by drying a dilute nMOF sample onto a silicon wafer at room temperature. XPS analysis was conducted using Kratos Axis Ultra DLD X-ray Photoelectron Spectrometer in Analytical and Nanofabrication Laboratory in the Department of Chemistry at the University of North Carolina at Chapel Hill. The XPS spectrometer was equipped with a monochromatic Al X-ray source operating at 6 mA and 15 kV at less than 10-8 torr. The step size was 0.5 eV for the survey spectra (pass energy = 160 eV) and 0.05 eV for high-resolution core-line spectra (pass energy = 80 eV).
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7

Comprehensive Characterization of Carbon Quantum Dots

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Transmission electron microscopy (TEM) and high-resolution TEM images (HRTEM) were taken on a JEOL JEM-2100 microscope with an accelerating voltage of 60 kV. Fourier transform infrared (FT-IR) spectra were recorded in the form of KBr pellets with a BRUKER TENSOR 27 spectrometer. X-ray photoelectron spectroscopy (XPS) measurements were conducted on a Kratos AXIS ULTRA DLD X-ray photoelectron spectrometer with mono X-ray source Al Kα excitation (1486.6 eV). The excitation and emission spectra of l-/d-CQDs aqueous solution were collected on a Horiba Fluoromax-4 luminescence spectrometer using Xe lamp as excitation source. The circular dichroism spectra (CD) and ultraviolet-visible (UV-vis) absorption spectra of samples aqueous solution were obtained on a JASCO J-1500 spectropolarimeter.
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8

Comprehensive Characterization of TiCN Nanoparticles

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Transmission electron microscopy (TEM) images of the sample were recorded on a JEM-2100F microscope operated at 200 kV acceleration voltage using super thin carbon films. X-ray diffraction (XRD) patterns were obtained with a Rigaku 18 KW D/max-2550 using Cu Kα radiation. X-ray photoelectron spectroscopy (XPS) measurements were performed using a Kratos Axis Ultra DLD X-ray photoelectron spectrometer. The zeta potential and size of the sample were recorded by a Malvern Zetasizer Nano ZS90 Zeta potential analyzer. UV-vis-NIR absorption spectrum was obtained by Agilent Cary 5000 spectrophotometers. TiCN was purchased by XFNANO Materials Tech Co., Ltd (Jiangsu, China).
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9

Characterization of Synthesized SBO Nanoparticles

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Crystallographic data for the synthesized nanoparticles were investigated by powder X-ray diffraction (P-XRD). The P-XRD pattern of the SBO NPs was recorded using a BRUKER ECO D8 advance with Cu Kα radiations (λ = 0.15406 nm) at room temperature. The FT-IR spectrum of the synthesized nanoparticle (as pellets in KBr) was recorded using a IRTRACER-100 FT-IR spectrometer. The morphology of the synthesized NPs was investigated by high-resolution transmission electron microscopy (HR-TEM, JEOL, JEM-2100 plus, Japan) and high-resolution scanning electron microscopy (HR-SEM, Thermo Scientific, Apreos), with energy-dispersive spectroscopy (EDS) and mapping to elemental analysis. A Kratos Axis Ultra-DLD X-ray photoelectron spectrometer was utilised in order to carry out the X-ray photoelectron spectroscopic (XPS) investigations.
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10

Comprehensive Characterization of Carbon Quantum Dot Phosphors

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Transmission electron microscopy (TEM) and high-resolution transmission electron microscopy (HRTEM) images of CQDs/PC phosphor were obtained on JEOL JEM-2010. The powder sample was first dispersed in deionized water ultrasonically and then dripped onto ultra-thin carbon films. Fourier-transform infrared (FTIR) spectra were obtained on a Bruker Tensor 27 spectrometer with the sample in KBr disk. The X-ray diffraction (XRD) pattern of the CQDs/PC was measured by Rigaku-D/MAX 2500 diffractometer with Cu Kα (λ = 1.5406 Å) radiation at a scanning speed of 4°/min in the 2θ range from 10° to 80°. Photoluminescence (PL) spectra were recorded on Horiba Fluoromax-4 fluorescence spectrophotometer. The thermogravimetric (TG) curve was characterized by Setaram Labsys Evo TG analyzer under a high-purity argon atmosphere with a 10 K/min heating rate. The absolute QY of CQDs/PC phosphor was measured by an integrating sphere. X-ray photoelectron spectroscopy (XPS) measurement was conducted on Kratos AXIS ULTRA DLD X-ray photoelectron spectrometer with mono X-ray source Al Kα excitation. WLED devices were tested by the F-star photoelectric testing system.
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