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Invia micro raman spectroscopy system

Manufactured by Renishaw
Sourced in United Kingdom

The INVIA micro-Raman spectroscopy system is a laboratory instrument designed for material analysis and characterization. It uses Raman spectroscopy, a non-destructive technique, to provide detailed information about the chemical composition and molecular structure of a wide range of samples. The system features a high-performance microscope and advanced optics to enable high-resolution spatial analysis of sample materials.

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6 protocols using invia micro raman spectroscopy system

1

Comprehensive Physicochemical Characterization of Novel Material

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Crystal structure information of sample was conducted by D8 Discover X-ray diffractometer (XRD) using Cu-Kα X-ray source with radiation. Field emission scanning electron microscopy (FESEM, JEOL-7100F) and Energy-Dispersive Spectroscopy (EDS) were used to analyze morphology and element distribution. Transmission electron microscopy (TEM) images were obtained by using JEM-2100F with acceleration voltage 200 kV. Fourier transform infrared Spectroscopy (FTIR) measurements were collected by using Nicolet 6700 (Thermo Fisher Scientific Co., USA) IR spectrometer with wavenumber range from 400 to 4000 cm−1. Thermogravimetric analysis (TGA) was conducted with a STA-449C from 30 to 600 °C. The Tristar II 3020 instrument was performed to measure BET specific surface area and pore volume by adsorption of nitrogen at 77 K. The X-ray photoelectron spectroscopy (XPS) analysis was tested by ESCALAB 250 Xi spectrometer. Raman spectroscopy was performed on Renishaw INVIA micro-Raman spectroscopy system.
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2

Multimodal Characterization of Nanomaterials

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The morphology of transmission electronic microscope (TEM) image was collected on a Hitachi H-800 spectroscope (Japan) operating at 10 kV. Fourier Transform infrared spectroscopy (FT-IR) profiles were recorded on a Bruker Vertex 70 (German) from 400 to 4000 cm−1 at a resolution of 2 cm−1, equipped with a temperature- controlled attenuated total reflectance (ATR) device with a ZnSe crystal (Pike Technology). X-ray photoelectron spectroscopy (XPS) was performed on a ThermoFisher Scientific ESCALAB 250XI (USA) using monochromated Al Kalph source (150 W, 500 μm). The pass energy was 50 eV for survey, and 30 eV for high resolution scans. All binding energies were reference to the C1s peak at 284.4 eV. X-ray diffraction (XRD) patterns were recorded on a Bruker D2-phaser diffractometer (German) at 40 mA and 40 kV using Cu Kα radiation (λ = 1.54, 6.88°/min from 5 to 90°). Raman spectra were recorded on a Renishaw inVia Micro-Raman Spectroscopy System (England) equipped with charge-coupled device detector at 633 nm. Specific surface areas and pore size distributions were determined by Brunauer Emmett-Teller (BET) method on Micromeritics ASAP 2460 apparatus (USA) from nitrogen sorption isotherms collected at 77 K. The samples were degassed at 250 °C for 12 h prior to measurement.
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3

Characterization of CoXNiy@C Nanosheets

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FESEM (field-emission scanning electron microscopy, JEOL, JSM-7100F) and TEM (transmission electron microscopy, JEOL, JEM-2100F) were used to analyze the morphology and microstructure of the CoxNiy@C nanosheets. Raman spectra (Renishaw INVIA micro-Raman spectroscopy system) and XRD (D8 Advance X-ray diffractometer, Cu Kα radiation, λ = 1.5418 Å) was used to characterize the structure of the CoxNiy@C nanosheets. X-ray photoelectron spectroscopy (XPS, VGMultiLab 2000) was used to test the chemical states of elements. Adsorption of nitrogen was used to measure Brunauer–Emmett–Teller (BET) surface area using Tristar II 3020 instrument. Agilent PNA N5244A vector network analyzer (VNA) was used to test the electromagnetic parameters in the range of 2–18 GHz with coaxial wire analysis model [27 (link)]. Compressing sample and paraffin with 20% filler loading ratio made a ring with inner and outer diameter of 3.04 mm and 7.00 mm to measure.
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4

Comprehensive Characterization of Materials

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The crystallographic information of the final products was measured using a Bruker D8 Advance X-ray diffractometer equipped with a Cu Kα radiation source; the samples were scanned over the 2θ range from 10° to 80° at room temperature. SEM images were collected using a JEOL-7100F SEM, and TEM images were collected using a JEM-2100F TEM. The BET surface area was calculated from nitrogen adsorption isotherms measured at 77 K using a Tristar-3020 instrument. Energy-dispersive X-ray spectra were recorded using an Oxford IE250 system. thermogravimetric–DSC analyses were conducted using a STA-449C. X-ray photoelectron spectroscopy analysis was conducted on a VG Multilab 2000. Raman spectra were obtained using a Renishaw INVIA micro-Raman spectroscopy system. The surface tension was tested by an automatic surface tensiometer (CC2L202) from 2 to 200 N m−1.
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5

Micro-Raman Spectroscopy for Material Analysis

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Micro-Raman spectrum ranged from 3200 to 300 cm−1 and it was measured by the Renishaw InVia Micro-Raman Spectroscopy system (Renishaw plc, Gloucestershire, UK) equipped with a confocal optical microscope for fast mapping. The Raman wavelength range was between 200 and 2200 nm, the spectral data was collected with resolution of 0.3 cm−1, and the stability was <±0.001 cm−1. The tested samples were irradiated with diode laser with excitation wavelength of 532 nm. The output power of laser was 5 mW, The Raman scatterings from the samples were collected by an objective lens, filtered into the microscope frame, and directed to a 50× eyepiece for visual observations. A multichannel charge-coupled device (CCD) detector was used for spectral analyses, and a digital camera with high sensitivity mode was applied for imaging.
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6

Comprehensive Structural Characterization of Materials

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Crystallographic phases of all the products were investigated by powder X-ray diffraction (XRD, Rigaku D/max2500) with Cu Kα (λ = 1.5406 Å) radiation. The morphologies of the samples were examined by field-emission scanning electron microscopy (SEM, FEI Nova NanoSEM 230) and transmission electron microscopy (TEM; JEOL-JEM-2100F transmission electron microscope). A combined Differential Scanning Calorimetry (DSC)/Thermogravimetric Analysis (TGA) instrument (Netzsch STA449C, Germany) was used to study the reactions during the annealing process and measure the carbon content in CW-LVP. Raman spectra were obtained using a Renishaw INVIA micro-Raman spectroscopy system. Nitrogen adsorption-desorption measurements were conducted at 77K (NOVA 4200e, Quantachrome Instruments).
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