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26 protocols using antaris 2

1

Near-Infrared Spectroscopy of Egg Structure

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Under the reflectance mode, an Antaris II near-infrared spectrophotometer (Thermo Electron Co., Waltham, MA, USA) with a fiber optic sampling probe was used to record the NIR spectrum. Comparing the whole structure of eggs, it was found that it is easier to obtain the changes of the tissue composition of eggs near the equator of the eggshell than in other parts. Therefore, the light probe is generally placed near the axis of the eggshell equator to illuminate the sample and obtain diffusely scattered light. The experiments were performed in triplicates to reduce the impact of uneven tissue on the results, and the average of these spectral data was used for analysis. Comparing the spectra collected under the conditions of a long wave (1000–2500 nm) and short wave (350–1025 nm), it was found that the reflection result of a long wave is better than that of a short wave, so the selected spectral range was 1000–2500 nm. The data was measured at 3.856 cm−1 intervals, which resulted in a total of 1557 variables. Each spectrum was acquired at three different locations under the same light source. The temperature and humidity of the laboratory were controlled at 25 °C and 70%.
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2

Near-Infrared Spectroscopy of Dry Powders

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The NIR spectra were collected using an Antaris II near-infrared spectrophotometer (Thermo Electron Co., USA) with an integrating sphere. Each spectrum was the average of 32 scanning spectra. The spectral range was from 10,000 to 4000 cm−1. The standard sample accessory holder was performed to collect sample spectra, and it was the sample cup specifically designed by Yixing jingke optical instrument Co., Ltd (Jiangsu, China) Dry sample powders (about 5 g) were put in the sample cup in the standard procedure. Each sample was collected three times and the average of the three spectra collected from the same sample was used for further analysis. The room temperature was kept at 25°C, and the humidity was kept at an ambient level in the laboratory. The spectral data of diffuse reflection (R) were transformed into absorbance spectra.
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3

Multi-Spectral Characterization of Samples

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FT-IR spectra were obtained on a NICOLET iS5 spectrometer (Thermo Scientific, Waltham, Massachusetts, USA) equipped with a DTGS detector and KBr beam splitter. Spectra were obtained in the range of 4000 cm -1 to 550 cm -1 with a resolution of 2 cm -1 using a monolithic diamond attenuated total reflectance (ATR iD7) accessory. All the spectra were recorded at room temperature with 32 scans.
Raman measurements were carried out using IDRAMAN Reader (Ocean Optics, Oxford, UK) with 785 nm emission of a laser (23.4 mW at sample) for excitation. The laser was focused on the sample contained in 2 mL vial. For signal detection, a 2048element NIR-enhanced CCD array with thermoelectric cooling to 10 °C was employed.
An averaged spectrum for each sample was recorded in the range of 200 to 3200 cm -1 , using an integration time of 10 s each 3 scans. NIR spectra were obtained using Antaris II (Thermo Electron Corporation, Waltham, Massachusetts, USA) FT-NIR analyzer, equipped with a diffuse reflection fibre optic and InGaAs detector. All the spectra, in the range of 4000 to 10000 cm -1 , were recorded at room temperature with 32 scans. In all cases, each sample was analysed in triplicate.
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4

Comprehensive Characterization of MOF199 Crystals

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Scanning electron microscopy (SEM) images were obtained on a XL30ESEM-FEG (PHILIPS, Netherlands) at 7 kV; the specimens were platinum-coated before imaging. Elemental analysis was performed by energy-dispersive X-ray spectroscopy (EDS, JSM-6480LV, JEOL, Japan). The crystalline structure was analyzed by X-ray diffraction (XRD, X PERTPRO-30X, PHILIPS, Netherlands) at a generator voltage of 40 kV and a generator current of 40 mA with a scanning step size of 0.005° and 0.2 second per step from 5° to 40° under Cu Kα radiation. FT-IR spectra of the MOF199 crystals and MOF199-coated samples were collected with an infrared spectrometer (ANTARIS II, Thermo Fisher, USA) within the range of 4000 to 600 cm−1 at a spectral resolution of 4 cm−1 and a scanning number of 64. The surface roughnesses of the bamboo and wood samples were measured by an atomic force microscope (AFM, Veeco, USA) in tapping mode with a scan area of 10 μm × 10 μm. The sizes of the crystals on the MOF199-coated samples were statistically calculated using Nano Measurer 1.2 software.
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5

Near-infrared Spectroscopy for Tea Analysis

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In this study, a Fourier Transform near-infrared spectrometer (Antaris II, Thermo Fisher Scientific, US) was used for spectral information collection. Before collecting spectral data, the spectrometer was preheated for half an hour to ensure a stable scanning state. Then, using the integrating sphere diffuse reflectance sampling module, approximately 3 g of tea powder was loaded into a sample cup rotator with an inner diameter of 4.78 cm. The sample cup was shaken to cover the bottom detection surface with tea powder before the sample was ready for testing. The instrument parameters were set to 64 scans, with a gain of 2 in the room temperature of approximately 25 °C. The background spectrum was removed and air was used as a reference. For each tea powder sample, near-infrared spectra were scanned at three different positions 120° apart at the bottom of the powder. The average of these three sets of spectral data was taken for analysis. After collecting the sample spectra, the tea powder was used for chemical content detection. Meanwhile, the sample cup was cleaned and prepared for the next collection.
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6

Near-infrared Spectral Analysis of SPI Samples

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SPI samples were scanned using a Fourier-transform near-infrared spectra analyzer (Antaris II, Thermo Fisher, Waltham, MA, USA). Samples were gently pressed into the dish (30 mm), then tapped three times with a spatula to ensure even packing. NIR spectra were captured at wavelengths of 10,000–4000 cm−1 (64 scans) measured as absorbance at a resolution of 8 cm−1 [14 (link)].
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7

FT-NIR Spectroscopy for Sample Analysis

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An FT-NIR
spectrometer (Thermo Scientific Inc., Antaris II) was used to obtain
FT-NIR spectra of fresh samples. The wavelength range of the spectrometer
was 10 000–4000 cm–1, the resolution
was 8 cm–1, and the signal was scanned 64 times.
Each scan took about 1 min. The background was deducted before testing
the sample. Three random positions of the sample cap were selected
to measure the FT-NIR spectrum every 6 h, and the average value was
taken. The spectrometer was warmed up for 2 h before measurements.
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8

FT-NIR Spectroscopy of Coconut Samples

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W. cocos samples’ spectra were collected by FT-NIR spectrometer (Thermo Scientific Inc., Antaris II). This instrument needed to be warmed up for 2 hours before collecting samples’ spectra to ensure its stability and accuracy. A sufficient amount of sample powder was placed in the sample cup. Under the condition of the spectral resolution of 8 cm-1 with a scanning range of 10000-4000 cm-1, the scanning times of each sample were 64, and the samples were collected twice in parallel. In this study, the average spectrum of the sample was used as the data source for subsequent NIR spectrum modeling. It is worth mentioning that the background signal needs to be collected every hour for correction to eliminate the interference of air. In addition, when collecting spectral information, it is necessary to make the air humidity and temperature stay at 45°C and at 25%, respectively.
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9

NIR Spectroscopy of Powder Samples

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An Antaris II spectrometer (Thermo Fisher Scientific, USA) with integrating sphere diffused reflection mode was used for obtaining NIR spectra of sample powders. Spectrum scan range was 10 000–4000 cm−1. Resolution was 8 cm−1 and each sample power has 64 accumulated scans. The obtained spectra were recorded as the logarithm of reciprocal reflectance, log(1/reflectance). In order to reduce the operation error, 20.0 g powder was filled up a uniform glass vessel to scan one by one. In addition, humidity and room temperature were kept at 30% and 25°C, respectively, in the course spectra collection to exclude interference of laboratory air. Finally, the average spectrum from triplicate measurement was calculated as the final spectrum for mathematical analysis.
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10

FT-NIR Analysis of Adulterated Garlic

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The Fourier-transform near-infrared spectra (FT-NIR) were measured using the Antaris II FT-NIR analyzer (Thermo Scientific, Waltham, MA, USA). The instrument was equipped with an integrating sphere enabling diffuse reflection analysis of different materials, including powdered samples. The FT-NIR absorbance spectra were collected between 10,000 cm−1 and 4000 cm−1 with 2 cm−1 resolution, i.e., between 1000 nm and 2500 nm, directly through glass vials. Before collecting the spectra of adulterated ground garlic mixtures, moisture was removed from the samples through drying them to constant weight in a laboratory dryer at 80 °C. Then, they were carefully mixed to obtain an even distribution of an adulterant in a sample. Finally, each mixture was described using the average FT-NIR spectrum of 32 independent scans. Spectroscopic measurements were carried out at stable room temperature (22 °C) and humidity (50%). Spectra were recorded thirty minutes after switching on the instrument in order to stabilize the radiation source. The background spectrum was recorded at the beginning of the measurements. The background correction procedure was repeated automatically every hour using an internal standard (diffusely reflective gold plate).
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