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Axis ultra xps spectrometer

Manufactured by Shimadzu
Sourced in United Kingdom

The AXIS Ultra XPS spectrometer is a high-performance X-ray photoelectron spectroscopy (XPS) instrument manufactured by Shimadzu. It is designed to provide detailed surface analysis of a wide range of materials, including metals, semiconductors, and polymers. The AXIS Ultra XPS spectrometer utilizes advanced technology to deliver accurate and reliable data for researchers and scientists.

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6 protocols using axis ultra xps spectrometer

1

Surface Analysis of Plasma-Treated Papers

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A scanning electron microscope (SEM) with an acceleration voltage of 3 kV was used to analyze the morphologies of the untreated and treated papers. The surface element content analysis was carried out with an X-ray photoelectron spectroscopy instrument (XPS, AXIS Ultra XPS spectrometer, KRATOS analytical, Manchester, UK). The parameters for XPS were set as a monochromatic Al K X-ray at 150 W anode power, survey spectra from 0 to 1200 eV with a pass energy of 80 eV for a survey, and 20 eV for core-level spectra. The chemical alterations in the paper samples following the plasma treatments were evaluated using two specimens of each group, and each specimen was analyzed for two sampling points. Characteristic oxygen (1s), carbon (1s), and fluorine (1s) peaks were searched, and the spectra were charge-corrected for the C–C/C–H peak (binding energy 284.7 eV). Spectra were evaluated with Casa XPS code software (Casa Software Ltd., Cheshire, UK).
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2

Comprehensive Characterization of Catalytic Materials

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Infrared (IR) spectroscopy spectra were collected on a Nicolet 330 FTIR spectrometer within the 4000–500 cm−1 region. Elemental analyses (C, H, and N) were conducted on a PerkinElmer 240 elemental analyzer. Thermogravimetric analysis (TGA) was performed on a Mettler Toledo TGA under a N2 flow by heating from room temperature to 900 °C (10 °C min−1). Powder X-ray diffraction (PXRD) measurements were carried out on an analytical X-Pert pro diffractometer with Cu-Kα radiation (γ = 1.5478 Å). Surface area and pore size distributions of the catalysts were determined using nitrogen adsorption–desorption isotherms obtained on a Micromeritics ASAP 2020 surface area analyzer at 77 K. The Pd contents were determined by inductively coupled plasma atomic emission spectroscopy (ICP-AES) on an IRIS Intrepid II XSP instrument (Thermo Electron Corp.). Scanning electron microscopy (SEM) images were obtained using a JEOL JSM-7600 field-emission SEM with an accelerating voltage of 5 kV. TEM images were collected on a FEI Tecnai F20 microscope operating at 200 kV. X-ray photoelectron spectroscopy (XPS) analysis was performed on an Axis Ultra XPS spectrometer (Kratos, U.K.) with 225 W of Al Kα radiation. The Raman spectrum was collected via a HORIBA Evolution Raman microscope using 532 nm incident wavelength.
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3

Surface Analysis of Coated Biomaterials

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The chemical alteration of the coating after the immersion in SBF was evaluated by X-ray photoelectron spectroscopy (XPS, AXIS Ultra XPS spectrometer, KRATOS analytical, Stretford, Manchester, UK). The parameters for XPS were set as in a previous study [27 ]; the monochromatic Al K X-ray was at 150 W anode power, survey spectra from 0 to 1200 eV with a pass energy of 80 eV for a survey, and 20 eV for core-level spectra. Two specimens of each group were used for the XPS test. Each specimen was tested for two points. In addition, the atomic percentage of each element was measured. The average value of calcium (Ca) and phosphorus (P) was used for the Ca/P ratio calculation.
The surface morphology was analyzed via scanning electron microscope (SEM) (JSM-IT300LV, JEOL USA Inc., Peabody, MA, USA). The coating surface roughness was evaluated by atomic force microscope (AFM) (Park XE7, Park system, Mannheim, Germany) in non-contact mode. The surface roughness measurement was repeated four times on each specimen. The average roughness value was calculated.
All experiments and tests were performed at Chiang Mai University, Thailand.
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4

Comprehensive Characterization of Nanomaterials

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The Raman spectra and mapping were measured on a Renishaw system using a 532 nm wavelength laser source. The absorption spectra and PL spectra were recorded with a spectrograph (Andor) and an EMCCD (Andor) integrated into an inverted optical microscope. The scanning electron microscopy (SEM) images were taken with a FEI Quanta 650 SEM. TEM images and diffraction patterns were obtained with a JEOL 1400 (120kV) with Gatan Inc. One view camera and a specialized TEM holder (Laser Prismatics). Near-field nano-FTIR measurements were performed with a commercial Neaspec system equipped with a broadband laser source45 (link). The XPS spectra were collected on a Kratos AXIS Ultra XPS spectrometer.
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5

X-ray Photoelectron Spectroscopy Calibration

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The XPS measurements were performed on an Axis Ultra XPS spectrometer from Kratos, Japan. The operation was under 225 W of accelerating voltage and Al Kα radiation. The C 1s line located at 284.8 eV was used to calibrate each spectra for accurate binding energies.
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6

X-ray Photoelectron Spectroscopy of Modified Wood

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The wood powder was scraped from the slice of less than 2 mm on the surfaces of all untreated and THM wood. The XPS measurements were performed on an Axis Ultra XPS spectrometer (Kratos Analytical) with monochromated Al Kα (hν = 1486.6 eV) source. All samples were analyzed in vacuum ranging from 1.33 × 10 -6 to 1.33 × 10 -5 Pa. Three types of spectrum were collected: a survey spectrum, a lowresolution spectrum from 0 to 1100 eV, and a high-resolution spectrum of the C-C or C-H group (C1s) region from 280 to 300 eV. The ratio of oxygen to carbon element (O/C) was determined from the low-resolution spectra. The peak analysis was carried out by means of peak decomposition to fit a Gaussian function. Chemical bond analysis of the carbon was accomplished by curve fitting and the high-resolution C1s peak was deconvoluted into four sub peaks.
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