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Invia reflex

Manufactured by Leica
Sourced in United Kingdom

The InVia Reflex is a high-performance Raman spectrometer designed for advanced materials analysis. It features a compact and modular design, enabling flexibility in configuration to suit various research and industrial applications.

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6 protocols using invia reflex

1

Confocal Raman Microspectroscopy of DPI Formulations

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Confocal Raman microspectroscopy (CRM) provides noninvasive and nondestructive microspectroscopic component analysis of DPI formulations. Using similar conditions previously reported20 (link),45 (link),49 (link)–51 (link), Raman spectra were obtained at 514 nm laser excitation using Renishaw InVia Reflex using a 20 × magnification objective on a Leica DM2700 optical microscope. Raman spectral map was obtained with the stage moved in increments of 20 × 20 µm in each axis. Each map point was acquired 1 accumulation using 2 s of detector exposure time per accumulation.
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2

Raman Spectroscopic Analysis of Samples

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Raman spectroscopy studies were performed using a Renishaw InVia Reflex dispersive spectrometer with Leica microscope (Renishaw, Wotton under Edge, UK). An excitation source of λ = 785 nm, 300 mW was applied with spectral resolution 1 cm−1. Laser power was dependent on the sample and varied from 1% to 10% of the power. The spectra were accumulated within 10–300 s integration time. Test conditions T = 22 ± 2 °C, RH = 40 ± 2%. The analysis by Raman technique was carried out in a closed microscope chamber of the spectroscope with samples being placed on the microscope plate. Samples were positioned in the laser light focus using a microscope (magnification 50×) with CCD camera. The recording of spectra was carried out by Renishaw WiRE™ software (v.3.2, Wotton under Edge, UK). All Spectra processing was done with the use of Origin software (OriginLab, v.8.0, Northampton, MA, USA).
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3

Raman Spectroscopy of Powder Samples

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Raman spectra were obtained using a Renishaw InVia Reflex spectrometer coupled with a Leica optical microscope. The instrument was equipped with a double-edge filter to eliminate the Rayleigh scattering and with a CCD camera working at a temperature of 220 K with a 1024 × 246 pixel array. The spectral resolution achieved with the use of gratings of 2400 grooves/mm was 3 cm−1. The wavenumber accuracy in a vacuum was better than 0.8 cm−1. All spectra were recorded in the 300–1100 cm−1 range with an argon ion laser source emitting a 514.53 nm excitation wavelength. Inelastic spectra were collected in the backscattering mode via the confocal optical microscope. A ×50 magnification objective allowed a precise area analysis with a focused laser power of 1 mW/µm2. The probed area was around 4 µm2. The powder sample was deposited onto a glass pure silica slide. The powder surface was flattened with a flat spatula to have a well-defined focal distance. Measurements were performed on several points of the sample to ensure homogeneity and the focused power of the laser beam was checked for each wavelength to avoid any transformation or heating of the sample.
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4

Ex Situ Raman Analysis of Galvanostatic Cycling

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Ex situ measurements
were performed
at different stages of galvanostatic cycling. To avoid oxygen and
moisture contamination, an airtight Raman cell (ECC-Opto-STD, El-Cell,
GmBH) was assembled inside an argon-filled glovebox. Raman spectra
were collected with a 633 nm wavelength laser using a Raman system
(Renishaw inVia Reflex) with a microscope focused through a 50×
objective lens (Leica). The estimated power on the sample was 0.43
mW with 200 s exposure time and two accumulations. The baseline of
the spectra was corrected for clarity.
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5

Micro-Raman Analysis of Dental Samples

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Micro-Raman experiments were made with a Renishaw inVia Reflex spectrometer, with a Leica (Wetzlar, Germany) stereoscopy microscope attached, with a ×50 objective. The spectrometer was equipped with a liquid nitrogen-cooled CCD detector. For the excitation, a laser diode emitting radiation in the IR region, with a wavelength of 785 nm, was applied. The applied power of the laser was 300 mW. The teeth samples were analyzed using a Renishaw SynchroScan mode from 400 to 3200 cm−1 with a spectral resolution of about 2 cm−1. The beam was focused on the ~1 µm wide spots on the sample, and the steps were taken as 1.61 µm. The observed lines were: ν1 symmetric stretching line for PO43− ion ~960 cm−1; ν4 mode for PO43− ion 587 cm−1; 1070 cm−1 for CO32− line, substitution B; 3372 cm−1 for NH stretching line. The initial treatment of data was made using the Wire2 computer program and completed with Origin 8.1 software. The areas of overlapping peaks were calculated with Lorentzian deconvolution functions.
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6

Raman Spectroscopy of Dyed Samples

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Raman-dispersive
spectrometer: a Renishaw InVia Reflex with a Leica microscope (Renishaw,
GB) was used in the study. An excitation source of λ = 785 nm,
300 mW, was applied with a spectral resolution of 1 cm–1. The spectra of dyed and undyed samples were accumulated within
a 10 s integration time. The laser power was dependent on the sample
and varied from 1 to 10% of the power.
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