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Invenio spectrometer

Manufactured by Bruker
Sourced in Germany, United States

The INVENIO spectrometer is a high-performance laboratory instrument designed for advanced spectroscopic analysis. It features a modular design and provides precise measurements across a wide range of spectral regions, enabling researchers to conduct in-depth investigations.

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8 protocols using invenio spectrometer

1

FTIR Spectroscopy Protocol for Precise Sample Analysis

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The FTIR spectra of the samples were measured using the Bruker INVENIO® Spectrometer (Bruker Optics, Leipzig, Germany), which was equipped with a high-throughput extension HTS-XT for precise analysis. The OPUS v8.5 software was employed to control the data acquisition process. Spectra were acquired in transmission mode, covering a range of 4000–600 cm−1 (4 cm−1 resolution). To establish a baseline, a background spectrum of the empty 96-well Silicon plate was collected before each sample measurement. The background scans were repeated 40 times. Subsequently, the 5 replicate spectra of samples were averaged and baseline corrected using the UnscramblerTM v11 software from Camo Analytics AS (Oslo, Norway).
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2

FTIR Analysis of Chitosan-Based Thin Films

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FTIR measurements were carried out on a Bruker INVENIO® Spectrometer (Bruker Optics, Germany) equipped with a high-throughput extension HTS-XT. Samples were measured as thin films on 96-well Si plates with 5 replicate measurements for each sample. Data acquisition was controlled by OPUS v8.5 software. Spectra were collected in transmission mode in the range 4000–600 cm−1 with a resolution of 4 cm−1. Before each sample measurement, a background spectrum of the empty Si plate was collected; the number of scans for both background and sample was 40. In order to achieve optimal signal response, a sample volume of 6 μL per well for CH-2% AA and 2 μL for CH-1%AA-1%CA was used. For CH-2%CA, CH-4%CA, and CH-6%CA the volume was 2 μL after diluting with H2O 1:1 to avoid detector saturation. Baseline correction and averaging of the five replicate spectra were performed with UnscramblerTM v11 (Camo Analytics AS, Oslo, Norway) software.
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3

Probing HRP Secondary Structure

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In order to reveal possible changes in the HRP secondary structure after the incubation of its solution in the center of the half-sphere, the attenuated total reflection Fourier transform infrared spectroscopy (ATR-FTIR) method was employed. HRP solutions, incubated either in the center of the half-sphere or at a 2 m distance from the half-sphere (control solution), were analyzed with an INVENIO spectrometer (Bruker Scientific LLC, Billerica, MA, USA). The ATR-FTIR measurements were performed in the following way: 12 µL of the analyzed 10−4 M HRP solution in 2 mM PBSD buffer were placed into the measuring cell of the spectrometer. Therefore, a high (10−4 M) protein concentration was used due to the sensitivity limitations of the spectrometer employed. Each experiment was carried out with three samples, and for each sample, the measurements were performed twice. The number of technical replicate scans in each experiment was 120. Data, obtained in the ATR-FTIR measurements, were presented in standard form provided by the spectrometer operation software. In order to account for the contribution of the PBSD buffer to the resulting spectra, blank measurements with pure protein-free buffer were performed prior to the experiments with the HRP solutions within the same spectral range. The so-obtained ATR-FTIR spectrum of the buffer was subtracted from that of the protein solutions.
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4

Comprehensive Material Characterization of Modified Fibres

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FTIR spectra were recorded with a Bruker Invenio spectrometer (Invenio, Germany) with a Platinum ATR module (equipped with a diamond crystal), with wavenumber ranging from 400 to 4000 cm−1 and resolution of 4 cm−1; and each sample was scanned 16 times. XPS spectra were analysed by an Escalab 250XiXPS with a monochromatic Al–Kα X-ray source. SEM (JSM-7500F) was used to observe the surface morphology of the fibres before and after modification. The samples were sprayed with aurum. The pressurized voltage was 15 kV and the resolution was 1.4 nm. TGA (Setaram Labsys Evo, France) was performed for thermal property characterization, where the samples were heated from 0 to 800°C under an N2 flow at a scanning rate of 10°C min−1 XRD (BRUKER AXSLTD, Germany) was used to detect the crystal structure. The fibre sample was fully ground into a powder. The determination conditions were as follows: Cu target, working voltage of 50 kV, current of 100 mA, scanning angle 2θ (Bragg angle) that varied from 5° to 60°, and scanning speed of 0.06° s−1.
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5

In situ ATR-FTIR of Electrochemical CO2 Reduction

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The in situ ATR-FTIR investigations were carried out with the Bruker INVENIO spectrometer with a HgCdTe (MCT) detector cooled with liquid nitrogen. A customized electrochemical H-cell was used to collect the in situ ATR-FTIR spectra, in which Pt-wire and Ag/AgCl severed as counter and reference electrodes, respectively. A fixed-angle Si prism (60°) coated with catalysts was used as the working electrode (Supplementary Fig. 41). 0.1 M KHCO3 aqueous solution constantly purged with CO2 was employed as the electrolyte. All spectra were collected with 128 scans and a resolution of 4 cm−1.
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6

Pressure-dependent CO adsorption on electrode

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In a typical SEIRAS experiment, the spectroelectrochemical cell was placed in the sample compartment with custom-built light pathway of a Bruker Invenio spectrometer equipped with a liquid nitrogen-cooled MCT detector. The pressure dependence of COL was investigated at different pressurization conditions. 1) The electrode potential was initially set to −0.9 V at 1 atm CO. CO was then pressurized to a fixed pCO while maintaining the electrode potential of −0.9 V. The system was kept for 15 min under each pressure before spectra were collected. 2) CO was pressurized to a fixed pCO at 0 V and equilibrate for 15 min. Afterward, the electrode potential was shifted to −0.9 V and spectra were then collected.
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7

FTIR Characterization of Molecular Analogues

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FTIR spectra
of MO 1 and its thioester 2 and amide 3 analogues in D2O were measured at 0.5 cm–1 resolution using a Bruker Invenio spectrometer. The
sample enclosure was purged with dry air to remove absorption peaks
from water vapor. Each spectrum is an average of 32 scans from 1000
to 4000 cm–1. The sample was equilibrated for 10
min at each temperature set point using a custom-built sample cell
connected to a recirculating water chiller, which provides a temperature
accuracy of 0.1 °C. Spectra were measured at the following temperatures:
10, 15, 20, 25, 30, 35, 40, 45, and 50 °C. Experiments were repeated
at least three times to ensure reproducibility.
Time series
FTIR spectra were measured using freshly dissolved amide 3, which was heated at 50 °C for 20 min. The sample cell was
then incubated at 25 °C, and FTIR spectra were collected every
5 min. Because the heat that the sample stores is negligible compared
to the recirculating system and the thermal conduction between the
two is efficient, the temperature of the sample reached 25 °C
in <3 min. Each spectrum was captured at 25 °C in the experiment.
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8

ATR-FTIR Analysis of HRP Structure

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In order to find out whether or not the HRP secondary structure changes after the incubation of its solution either near the apex of a pyramid or in the center of its base, ATR-FTIR method was employed. The ATR-FTIR measurements were carried out in the following way. 12 µL of 10−4 M solution of HRP in PBSD was placed in the measuring cell of an INVENIO spectrometer (Bruker Scientific LLC, Billerica, MA, USA). Such a high concentration of the protein solution was used due to the sensitivity of the spectrometer. The data were presented in a standard form provided by the spectrometer operation software. In order to account for the contribution from the PBSD buffer to the resulting spectra, a blank measurement with pure protein-free buffer was performed before the experiments with HRP solutions within the same spectral range. The spectrum obtained in the blank measurement was subtracted from those obtained in experiments with HRP solutions.
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