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Alpha 2 ft ir spectrometer

Manufactured by Bruker
Sourced in United States, Germany, Spain

The ALPHA II FT-IR spectrometer is a compact and robust Fourier Transform Infrared (FT-IR) spectrometer designed for routine analysis. It offers high-performance infrared spectroscopy with a simple and intuitive user interface.

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45 protocols using alpha 2 ft ir spectrometer

1

Mid-infrared Spectroscopy of Samples

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Mid-infrared measurements were taken with an Alpha II FTIR spectrometer with ATR attachment (both Bruker, Germany). The ATR element was a single reflection diamond crystal. Spectra were taken at 4 cm−1 resolution in the wavenumber range 4000–600 cm−1 using 32 averaged repeats per measurement. A pipette was used to deliver 30 μL of each sample onto the crystal surface. Each sample was characterised in triplicate and the mean was used for subsequent calculations. The spectra were baseline-corrected and had the CO2 absorption peaks removed.
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2

FTIR Spectroscopy of Powdered Samples

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Fourier transform infrared spectra were initially recorded with a Bruker Alpha II FTIR spectrometer equipped with an attenuated total reflectance (ATR) accessory of Zinc-selenium crystal. The prepared powdered samples were directly placed on the crystal and were recorded within the wave number range from 4000 cm−1 to 500 cm−1.
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3

FTIR Spectroscopy of 734THIF-7HP-HPBCD

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FTIR spectra of 734THIF, different ratios of 7HP and HPBCD were obtained from the ALPHA II FTIR spectrometer (Bruker, Billerica, MA, USA), and the scan ranged from 4000 to 400 cm−1 with the rate at 2 cm−1. About 2–3 mg of each sample were ground evenly with potassium bromide by a mortar and compressed into a thin tablet for analysis.
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4

High-Pressure Organic Synthesis Protocols

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All solvents were of analytical
grade and distilled prior to use.
Unless otherwise stated, all reagents were used as received from commercial
suppliers. Reactions at 900 MPa were conducted in a liquid piston
vessel LV30/16 in a laboratory hydraulic press U101, Polish Academy
of Sciences. NMR spectra were recorded in a Bruker Fourier 300 spectrometer
(300 MHz for 1H and 75 MHz for 13C). Chemical
shifts are reported in ppm (δ), and the center of the residual
solvent signal was used as the internal standard which was related
to TMS with δ 7.26 ppm (1H in CDCl3) and
δ 77.16 ppm (13C in CDCl3). The multiplicity
of the signals is reported as s (singlet), d (doublet), t (triplet),
q (quartet), and m (multiplet). Spin–spin coupling constants
(J) are given in hertz. High-resolution mass spectrometry
(HRMS) results were recorded in a Thermo Scientific Q Exactive hybrid
quadrupole-Orbitrap mass spectrometer (Thermo Scientific Q Exactive
Plus) connected to Dionex Ultimate 3000 UHPLC+ system equipped with
a multiple-wavelength detector, using an imChem Surf C18 TriF 100A
3 μm 100 × 2.1 mm column. Infrared spectra were recorded
on a Bruker ALPHA II FT-IR spectrometer.
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5

Comprehensive Analytical Characterization

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Optical rotation measurements were made on a Rudolph research analytical AUTOPOL IV automatic polarimeter (Rudolph Research Analytical, Hackettstown, NJ, USA), IR spectra were recorded with a Bruker ALPHA II FT-IR spectrometer (Bruker, Billerica, MA, USA), and UV spectra were measured with a Thermo Scientific Nanodrop 2000C spectrophotometer (Thermo Fisher Scientific, Waltham, MA, USA). The ECD spectrum was obtained on a JASCO J-1500 circular dichroism spectrometer (Jasco, Easton, MD, USA). High-performance liquid chromatography (HPLC) was performed using a Varian ProStar 215 solvent delivery module equipped with a Varian ProStar 320 UV-Vis detector (Agilent Technologies, Santa Clara, CA, USA), operating under Star 6.41 chromatography workstation software (Agilent Technologies, Santa Clara, CA, USA). NMR spectra were obtained with a Bruker Avance III NMR spectrometer (Bruker, Billerica, MA, USA) equipped with a 3 mm cryogenic probe and operating at 600 MHz for 1H and 150 MHz for 13C. Spectra were calibrated to residual solvent signals at δH 2.50 and δC 39.5 in DMSO-d6. All 2D-NMR experiments were acquired with nonuniform sampling (NUS) set to 50% or 25%. HRESIMS data were acquired on an Agilent Technologies 6530 Accurate-Mass Q-TOF LC/MS instrument (Agilent Technologies, Santa Clara, CA, USA).
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6

Spectroscopic Characterization of Compounds

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Optical rotations were measured on a Rudolph research analytical AUTOPOL IV polarimeter. ECD spectra were recorded on a JASCO J-1500 spectrophotometer. UV spectra were measured with a PerkinElmer, Inc. Lambda 465 UV/Vis photodiode array spectrophotometer. IR spectra were recorded with a Bruker ALPHA II FT-IR spectrometer. NMR spectra were obtained with a Bruker Avance III NMR spectrometer equipped with a 3 mm cryogenic probe and operated at 600 MHz for 1H and 150 MHz for 13C. (+)-HR-ESI-MS data were acquired on an Agilent Technology 6530 Accurate-mass Q-TOF LC/MS. HPLC was performed using a Varian ProStar 215 solvent delivery module equipped with a Varian ProStar 340 UV-Vis detector, operating under Star 6.41 chromatography workstation software. A solid phase extraction (SPE) was carried out with a Waters Oasis HLB (6 cc) cartridge.
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7

Characterization of Paramagnetic Complexes

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NMR spectra were recorded
on Bruker 300 or 400 MHz spectrometers. 1H and 13C chemical shifts are reported in ppm relative to tetramethylsilane
using residual solvent as an internal standard. 19F chemical
shifts are reported in ppm relative to 5% v/v internal PhF.28 (link) Solution-phase effective magnetic moments were
determined by the method described by Evans29 (link) and are corrected for diamagnetic contributions (as are SQUID magnetometry
data).30 (link) Mass spectrometry data were collected
on a Bruker MicroTOF II with an ESI source. FTIR spectra were recorded
on solid samples using a Bruker Alpha II FTIR spectrometer operating
at 4 cm–1 resolution. Elemental analyses were performed
by Midwest Microlab. EPR spectra were recorded on a Bruker EMX spectrometer.
Simulations were performed using EasySpin31 (link) (5.2.33) in MATLAB (R2021b). DC magnetic susceptibility data for
a microcrystalline sample of 4 were collected on an MPMS
SQUID magnetometer in the range of 5–300 K with a 10,000 Oe
applied field. The sample was prepared by compressing 12.2 mg of 4 between wads of quartz wool in a length of quartz tubing,
which was then flame-sealed under vacuum. Simulations were performed
using PHI32 (link) (3.1.5).
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8

NMR and Mass Spectrometry Analysis Protocols

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NMR spectra were recorded
on a Bruker 300 MHz spectrometer. 1H and 13C
chemical shifts are reported in parts per million (ppm) relative to
tetramethylsilane using residual solvent as an internal standard. 19F chemical shifts are reported in ppm relative to 5% v/v
internal PhF.33 (link) Solution-phase effective
magnetic moments were determined by the method described by Evans34 (link) and are corrected for diamagnetic contributions.35 (link) Mass spectrometry data were collected on a Bruker
micrOTOF II instrument with an ESI source. FTIR spectra were recorded
on solid samples using a Bruker Alpha II FTIR spectrometer operating
at 4 cm–1 resolution.
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9

Multi-Technique Characterization of Materials

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Powder X-ray powder diffraction (PXRD) patterns were obtained by employing a PANalytical Empyrean X-ray platform with a capillary platform and copper radiation (Cu Kα = 1.541 78 Å). Measurements were carried out in triplicate in the 2-theta range 2–70° by employing a step size of 0.02° per step with an integration time of 1 s. The attenuated total reflectance-Fourier transform infrared spectroscopy (ATR-FTIR) spectra were recorded using a Bruker alpha II FTIR spectrometer in the 4000–400 cm−1 range. The UV-vis absorption spectra of the solid samples were recorded in the reflectance mode by using a Jasco V-670 spectrometer. X-ray photoelectron spectroscopy (XPS) spectra were recorded using a Thermo Scientific™ K-Alpha X-ray Photoelectron Spectrometer. Al Kα X-ray radiation was employed as the X-ray source. For all the elements, more than 100 spectra were recorded by employing a step of 0.1 eV with a focused spot higher than 400 μm. XPS data were analysed with the Thermo Avantage v5.9912 software.
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10

Characterization of CQD Thin Film

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The FTIR spectra of CQD thin film before and after exposure to DA solution was recorded in the range of 400–4000 cm−1 using a Bruker ALPHA II FTIR Spectrometer in ATR mode. The Bruker AFM multimode 8 in Scan Asyst mode was used in the range of 2 × 2 μm for topographic imaging of all thin films and to analyze the roughness changes of CQD film after DA adsorption on its surfaces.
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