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Raman spectroscope

Manufactured by Renishaw
Sourced in United Kingdom

The Raman spectroscope is a scientific instrument used for the analysis of molecular structures. It operates by detecting the inelastic scattering of monochromatic light, typically from a laser source, interacting with the sample. The resulting spectrum provides information about the vibrational, rotational, and other low-frequency modes of molecules, allowing for the identification and characterization of materials at the molecular level.

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3 protocols using raman spectroscope

1

Material Characterization Techniques

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Morphological analysis was performed using SEM (S-4800, Hitachi, Tokyo, Japan). The Raman and PL measurement were performed using a confocal Raman spectroscope (inVia, Renishaw, WUE, UK) with a 488-nm laser. The bonding characteristic was measured using XPS (Sigma Probe, Thermo VG Scientific, MA, USA).
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2

Comprehensive Characterization of Multi-Walled Carbon Nanotubes

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The pore volume, surface area, and pore diameter of the MWCNTs were evaluated using an ASAP 2020 adsorption analyzer (Micromeritics, Norcross, GA, USA) at −196 °C. An X-ray diffractometer (X’pert Pro System, PANalytical, Malvern, UK) with Cu Kα radiation was employed to observe the crystalline phase of the MWCNTs. A field-emission scanning electron microscope (JEOL JSM-6700F, Akishima, Tokyo, Japan) and a transmission electron microscope (JEOL JEM-1200CX II, Akishima, Tokyo, Japan) were used to examine their morphological features. A Fourier transmission infrared spectroscope (FTIR-8300, Shimadzu, Nakagyo-ku, Kyoto, Japan) was employed to examine the functional groups of the MWCNTs. Graphitization was assessed using a confocal Raman spectroscope (Renishaw, Gloucestershire, UK) with 632 nm He–Ne laser excitation. The stability of the MWCNTs before and after modification was examined using a thermogravimetric analyzer (Mettler Toledo, OH, USA, model TGA/SDTA851e). The surface elements on the MWCNTs were analyzed using an X-ray photoelectron spectroscope (Esca Lab 250Xi, Thermo Scientific, Waltham, MA, USA). The C1s peak at 284.60 eV was employed to calibrate the binding energy. The amounts of metallic impurities in the MWCNTs were determined using an inductively coupled plasma–mass spectrometer (ICP-MS) (Konton Plasmakon, Eching, Germany, model S-35).
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3

Raman Spectroscopy of Carious Dentine

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A high-resolution Raman spectroscope (inVia, Renishaw Plc, Wotton-under-Edge, Gloucestershire, UK) running in Streamline scanning mode was used to scan the flat tooth surfaces, and a 5/0.12 NA air objective was used. A total of 246 point scans were captured from 10 carious dentine sections. In each section, an average of 18 point scans were captured along 3 line scans starting from the outermost part of the lesion in the direction from the enamel-dentine junction towards the pulp. A further 6 line point scans were captured in clinically sound dentine in the same section. The vibrational intensity of ester functional groups was calculated for each point scan (measured at 1740 cm -1 ). Spectrum acquisition was conducted using a 785 nm laser (10 mW for mapping mode and 0.5 mW for point scanning) using a 600 line/mm grate across the spectral bandwidth of 4000-400 cm -1 for each sample. Baseline correction was performed by Raman processing software (WiRe, Renishaw, UK).
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