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Nicolet nxr 9650 ft raman spectrometer

Manufactured by Thermo Fisher Scientific
Sourced in United States

The Nicolet NXR 9650 FT-Raman spectrometer is a laboratory instrument designed for Raman spectroscopy analysis. It utilizes Fourier Transform Raman (FT-Raman) technology to detect and measure the Raman scattering of light interacting with a sample. The core function of this spectrometer is to generate a Raman spectrum that provides information about the molecular structure and composition of the analyzed material.

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10 protocols using nicolet nxr 9650 ft raman spectrometer

1

Biochemical Characterization of Whole Kernels

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Samples of whole kernels were preliminarily prepared by grinding in a mortar and next used for HPLC (Agilent Technologies, Woldbron, Germany) and electrophoresis analysis (Hoefer, Holliston, MA USA) as well as FT-Raman analysis of biochemical components (Thermo Scientific Nicolet NXR 9650 FT-Raman spectrometer, Waltham, MA, USA) measurement.
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2

FT-Raman Spectroscopic Characterization of Samples

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FT-Raman spectra were recorded using a Nicolet NXR 9650 FT-Raman spectrometer (Thermo Fisher Scientific, USA) equipped with an Nd:YAG laser (1064 nm) and a germanium detector. Measurements were performed in the range from 150 to 3.700 cm−1 with a laser power of 1 W. Unfocused laser beam was used with a diameter of approximately 100 μm and a spectral resolution of 8 cm−1. Raman spectra were processed by the Omnic/Thermo Scientific software based on 128 scans. The obtained spectra were normalized using vector normalization in OPUS 7.0 software (Bruker Optik GmbH, Ettlingen, Germany). Moreover, each spectrum was smoothed using the Savitzky–Golay algorithm. The number of smoothing points was nine.
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3

Raman Spectroscopy of Lyophilized Plant Seedlings

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Seedlings from the previous assays were lyophilized and stored at −80 °C until use. The Raman spectra of lyophilized seedlings were recorded in the endosperm of kernels cut in half using a Nicolet NXR 9650 FT-Raman Spectrometer (Thermo Scientific, Walthman, MA, USA) equipped with an Nd: YAG laser (1064 nm) and an InGaAs detector. The measurements were performed according to the method described by Troć et al.45 (link) at room temperature at a spectral resolution of 8 cm−1 using an unfocused laser beam approximately 50 μm in diameter and an aperture of 80 μm. The laser power was 0.5 W, and the measurement range was 400 to 2000 cm−1. For each object 64 scans per spectrum were performed. The Raman spectra were registered and processed using the Omnic/Thermo Scientific software program (Thermo Scientific, Walthman, MA, USA). Six spectra from different plants were collected and averaged for each plant species and treatment. The spectra were baseline corrected. A hierarchical cluster analysis (similarities between FT-Raman spectra) was used to group the studied objects into clusters to find significant and systematic differences in the measured FT-Raman spectra and was performed using Statistica ver. 13.3 (TIBCO Software Inc., Palo Alto, CA, USA) for the whole wavenumber range. The spectral distances were calculated using Ward's algorithm.
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4

Raman Spectroscopy Analysis of Liposome Samples

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Raman spectral data were collected using a Nicolet NXR 9650 FT-Raman spectrometer (Thermo Scientific, USA), which includes a MicroStage extension, a neodymium-doped yttrium orthovanadate (Nd: YVO4) laser operating at 1064 nm with a power of 100 mW for excitation, and an indium gallium arsenide (InGaAs) detector for signal detection. Each analysis involved placing a 10 μL drop of the sample liposome suspension onto a gold substrate, which was then allowed to dry via exposure to the laser. The FT-Raman spectra captured a frequency range from 3700 to 0 cm−1, achieving a resolution of 4 cm−1 by averaging over 1024 scans (Fig. S7). The study maintained a consistent concentration of the compounds at 50 μM and lipids at 0.1 mg/ml to optimize the signal-to-noise ratio. Spectral acquisition was performed immediately following the dissolution of samples. Spectral processing and analysis were conducted using OriginPro 2021 software (Origin Lab Corporation, Northampton, Massachusetts, United States), with procedures including baseline adjustment, Savitzky-Golay (SG) smoothing with a window of 35 points and a polynomial order of 2, and normalization of spectra within the [0–1] range for the specific band region under investigation.
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5

FT-Raman Spectroscopy for Material Analysis

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An FT-Raman spectra measurement was performed using a Nicolet NXR 9650 FT-Raman Spectrometer (Thermo Fisher Scientific, Waltham, MA, USA) with Nd: YAG laser source (1064 nm) and a Germanium detector. A spectral range of 150 to 3700 cm−1 and a laser power of 500 mW were used. This power was constant for each sample and each measurement. An unfocused laser beam was used of approximately 100 μm in diameter and a spectral resolution of 8 cm−1. Raman spectra were processed using the Omnic/Thermo Scientific software (Thermo Fisher Scientific) based on 64 scans for measurements, which means the number of scans performed on one spot was 64, and the obtained spectrum was an average of these scans. All spectra were smoothed using the Savitzky–Golay algorithm for 7 points. Moreover, all spectra were normalized using vector normalization. Additionally, baseline corrections using a Rubberband correction were done. All these operations were performed using OPUS software (Bruker Optik GmbH, Ettlingen, Germany). Moreover, each sample was measured three times in three different places. Next, the spectra were averaged and this average was used for statistical analysis.
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6

Whole Grain Biochemical Analysis

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Samples of whole grains were preliminarily prepared by grinding in a mortar and next used for HPLC (Agilent Technologies, Woldbron, Germany) and electrophoresis analysis (Hoefer, Holliston, MA, USA) as well as gliadins’ extraction prior to FT-Raman (Thermo Scientific Nicolet NXR 9650 FT-Raman spectrometer, Waltham, MA, USA) measurement. For FT-Raman analysis of biochemical components, whole grains were cut into half and used for spectroscopic measurements.
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7

FT-Raman Spectroscopy Analysis

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FT-Raman spectra were obtained with a Nicolet NXR 9650 FT-Raman spectrometer (Thermo Fisher Scientific, Waltham, MA, USA) equipped with Nd:YAG excitation laser (1064 nm, 250 mW), InGaAs detector and MicroStage extension. All samples spectra were collected in the range of 4000–250 cm−1 with a spectral resolution of 4 cm−1, averaging 128 scans. All spectra were analyzed using the OriginPro (ver. 2019, OriginLab Corporation, Northampton, MA, USA).
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8

Raman Spectroscopy Analysis of Unground Wheat Grain

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Unground wheat grain was used to assess chemical composition using Raman spectroscopy. The Raman spectra were taken with a Nicolet NXR 9650 FT-Raman spectrometer (Thermo Fisher Scientific, Waltham, MA, USA) equipped with an Nd laser: YAG (1064 nm) and germanium detector. Measurements were carried out in the range from 150 to 3700 cm−1 at a laser power of 1 W. An out-of-focus laser beam with a diameter of about 100 μm and a spectral resolution of 8 cm−1 was used. Each spectrum was collected using 128 scans. The Raman spectra were analyzed using OPUS 7.0.129 software.
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9

Raman and FTIR Spectroscopy of Ovarian Cancer

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Nicolet NXR 9650 FT-Raman spectrometer (Thermo Fisher Scientific, USA) was used in this study to collect spectra of frozen tissues of ovarian cancer tissues. This spectrometer has Nd:YAG laser with 1064 nm wavelength and a germanium detector. In this study unfocused laser beam was used with a diameter of approximately 100 μm. Moreover, each sample was scanned 64 times with spectral resolution of 8 cm−1 and laser power of 1 W. The measurement range was between 150 and 3700 cm−1. In the other hand, a Bruker Vertex 70v spectrometer equipped with an attenuated total reflection (ATR) diamond crystal plate was used to collect FTIR spectra of ovarian tissues. The absorbance spectra were collected in the range between 400 and 4000 cm−1 using 32 scans and spectral resolution 4 cm−1. Before FTIR measurement, a background spectrum was collected. Moreover after each measurement, diamond crystal was cleaned using 70% of ethanol. For measurements, frozen ovarian cancer tissues were cut into thin (10 µm) slides and put on the gold standard for Raman and CaF2 glasses for FTIR spectra collected.
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10

Raman Analysis of Maize and Barnyard Grass

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The Raman spectra of lyophilized seedlings of maize and barnyard grass were recorded using a Nicolet NXR 9650 FT-Raman Spectrometer (Thermo Scientific, Walthman, MA, USA) equipped with an Nd:YAG laser (1064 nm) and a InGaAs detector. The measurements were performed at room temperature in the range of 400 to 2000 cm−1 with a laser power of 0.5 W (64 scans per spectrum), at a spectral resolution of 8 cm−1 using an unfocused laser beam approximately 50 μm in diameter and aperture of 80 according to the method described by [39 (link)]. The Raman spectra were registered and processed using the Omnic/Thermo Scientific software program (Thermo Scientific, Walthman, MA, USA). Six spectra from different plants were collected and averaged for each plant species and treatment. The spectra were baseline corrected. A hierarchical cluster analysis (similarities between FT-Raman spectra) was performed using Statistica ver. 13.3 (TIBCO Software Inc., Palo Alto, CA, USA) for the whole wavenumber range. The spectral distances were calculated using Ward’s algorithm.
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