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Xplora spectrometer

Manufactured by Horiba
Sourced in Japan, France

The XploRA spectrometer is a compact and versatile Raman microscope system designed for a wide range of applications. It features high-performance optics, advanced imaging capabilities, and easy-to-use software. The core function of the XploRA spectrometer is to provide efficient and accurate Raman spectroscopic analysis.

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10 protocols using xplora spectrometer

1

Raman Spectroscopic Analysis of Samples

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The Raman spectra were measured using an XploRA spectrometer (Horiba, Japan) coupled to an optical microscope (BXFM, Olympus, Japan) and equipped with a 532 nm laser that was focused on the samples through a 100 × objective (NA = 0.9). The same objective lens was used for collecting Raman scattered light after interaction with the sample, in backscattering geometry. The frequency calibration was set by reference to the 520 cm–1 vibrational bands of a silicon wafer. Under the same conditions, five Raman spectra were captured from each sample of both groups in the spectral range of 600–1,800 cm–1. To minimize laser-induced heating of the specimens, low power irradiation at the sample surface was used, around 5 mW, combined with a short exposure time (3 s laser exposure for five accumulations). The diffraction grating used had 1,200 lines/mm, which yielded a spectral resolution of 1.5 cm–1.
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2

Characterization of Solid ZIF-8 Adsorbents

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The adsorbents (solid ZIF-8) were characterized by XRD (SIMADU XRD 6000) with Cu Kα radiation (0.1542, nm, 40 kV and 400 mA) at a scanning rate of 2 °C per minute. The morphologies and energy dispersive X-ray spectroscopy measurements were obtained using a FEI Quanta 200F scanning electron microscope. Fourier transform infrared spectra were obtained using a Bruker 80v spectrometer. Fourier transform Raman spectra were obtained using a HORIBA XploRA spectrometer. The thermogravimetric measurements were carried out at a NETZSCH STA 409 PC/PG instrument.
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3

Raman Spectroscopic Analysis of Cell Nuclei

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Raman spectra were measured using an XploRA spectrometer (Horiba, Japan), coupled to an optical microscope (BXFM, Olympus, Japan) and equipped with a 532-nm laser that was focused on the nucleus of the cells through a 100 × objective (NA = 0.9). The same objective lens was used for collecting Raman-scattered light after interaction with the sample, in backscattering geometry. The frequency calibration was set by reference to the 520-cm–1 vibrational bands of a silicon wafer. Under the same conditions, 60 cell spectra captured in three different experiments for each group were measured in the spectral range of 600–1,800 cm–1. To minimize laser-induced heating of the specimens, low-power irradiation at the sample surface was used, around 5 mW, during a short exposure time (3-s laser exposure for five accumulations). The diffraction grating used had 1,200 lines/mm, which yielded a spectral resolution of 1.5 cm cm–1.
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4

Characterization of Reduced Graphene Oxide Aerogels

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The GO flake sizes
and the morphologies and structures of rGO aerogel membranes were
characterized by SEM (Zeiss Ultra 55, Germany). The rGO hydrogel and
aerogel membranes were characterized by XRD (Bruker, Cu Kα,
λ = 0.154 nm, Germany). Raman spectra were recorded using an
XploRA spectrometer (Horiba Jobin Yvon, France) with a 532 nm laser
source. The chemical compositions of membranes were analyzed by XPS
(Thermo Fisher Scientific ESCALAB 250XI, Al Kα source, USA).
TGA of rGO hydrogel and aerogel membranes was carried out with a thermal
analyzer (Mettler Toledo TGA 1, Swiss) at a heating rate of 10 K min–1 under a N2 atmosphere. Attenuated total
reflection-FTIR spectra of rGO aerogel membranes were recorded on
a Thermo Fisher Nicolet 6700. Hydrophilicity of the aerogel membranes
was evaluated using a contact angle goniometer. UV–vis spectra
for the dye solutions were recorded on a Lambda 750 spectrophotometer
(PerkinElmer, USA).
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5

Raman Spectroscopy of Aqueous Droplets

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Raman spectroscopy was carried out using ACDs in aqueous droplets on the slide. The spectra were recorded on a Horiba Jobin Yvon XploRA spectrometer equipped with a 10× objective and a laser with a wavelength of 532 nm. Data were collected between 850 cm–1 and 1700 cm–1 using a grating of 600 grooves per mm. They were normalized using the LabSpec Version 5 software package.
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6

Raman Spectra of Si Nanoparticles

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Raman spectra were collected with an Xplora spectrometer by Horiba, equipped with a confocal microscope. Samples were prepared by drop casting Si nanoparticles suspended in chloroform onto a glass microscope slide. An objective lens with a magnification of 50× was used to observe the sample and choose the measurement area. A 100× objective lens was employed to focus the laser beam on the selected spot. The spectra were run using a 532 nm excitation wavelength, using a filter to reduce the laser power to 50% of the total power. A 1800T grating was used to separate the scattered light into its components. Baseline subtraction was performed on each spectrum, using a linear baseline. Five measurements in five different zones were collected for each sample, to assess the reproducibility of the measurement and the uniformity of the sample.
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7

Raman Spectroscopy Analysis of Solutions

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Raman spectroscopy was performed using an Xplora spectrometer (Horiba Scientific, France). The Raman spectra were recorded at an excitation wavelength of 785 nm (diode laser) at room temperature. For the measurements in the solution, a macro-objective with a focal length of 40 mm (NA = 0.18) was used in the backscattering configuration. The spectral resolution achieved was approximately 2 cm−1.
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8

Raman Spectroscopy of Microscale Samples

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Raman spectra were recorded on an Xplora spectrometer by Horiba, equipped with a confocal microscope. An objective lens with a magnification of 10× was used to observe the sample inside the capillary and choose the measurement area. An Olympus LM Plan FLN 100× objective lens with 0.80 numerical aperture and 3.4 mm working distance was employed to focus the laser beam on the sample and collect the scattered light. A longpass edge filter was used to remove the fundamental line from the collected scattered light. The spectra were run using a 632.81 nm HeNe gas laser or a 785 nm laser diode excitation, using a filter to reduce the laser power to 50% of the total power. A 600 lines per mm grating was used to separate the scattered light into its components that were collected onto a Syncerity TE-cooled FI-UV-VIS detector. Baseline subtraction was performed on each spectrum, using a linear baseline. Five measurements in five different zones were collected for each sample, to assess the reproducibility of the measurement and the uniformity of the sample.
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9

UV-Vis and Raman Analysis of Hematin-Fibrinogen Interaction

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UV–Vis absorption spectra of hematin (2 × 10−5 M) in the absence or presence of fibrinogen (5 mg/mL) were obtained by a UV–Vis spectrometer (SHIMADZH UV-2550) at ambient temperature. The scans were performed with quartz cuvettes with 1 mm optical path. For Raman measurements, a volume of 10 μL hematin solution (2 × 10−5 M) in the absence or presence of fibrinogen (5 mg/mL) was deposited onto quartz substrate and allowed to dry at 30 °C and the spectra were acquired with a HORIBA JOBIN YVON XploRA spectrometer which worked in the confocal mode. The spectra were collected on the edge of the “coffee-ring” arising from the outward flow of solvent36 . A 100× objective (Olympus, MPlanN, NA 0.9) was used to focus the laser onto the sample (with spot size ∼3 μm in diameter) and also collect the back-scattered Raman light into the detector. The laser power at the sample was reduced to approximately 5.0 mW. All the spectra represent the average from three cycles of 60 seconds Raman spectra acquired consecutively under the same conditions. For every sample, Raman measurements were conducted at 5 points at least, and at every point, the Raman spectra were collected with the parameters as described above.
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10

Raman Spectroscopy of Diamond Nanoparticles

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Raman spectra were recorded with a Horiba Xplora spectrometer equipped with a 532 nm laser with a 0.79 mW power (Kyoto, Japan). 10 μL of DND in water were deposited on a silicon substrate and dried. Each spectrum is the average of 3 acquisitions realized at different positions on the substrate. The acquisition time is one minute, cumulated 10 times.
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