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12 protocols using is50 ft ir

1

FTIR Analysis of FNB-Carrier Interactions

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The intermolecular interactions between FNB and the carrier matrix were investigated using an FTIR analysis (iS50 FTIR equipped with a SMART OMNI-Sampler, ThermoFisher Scientific, Waltham, MA, USA). The FNB, HPMC AS LG, PM, and crushed EXT were analyzed from 4000–700 cm−1, at a resolution of 4 cm−1 for % transmittance with 64 scans per run. The background was collected before every run. Weak intermolecular interactions were analyzed and assessed on the OMNICTM series software (ThermoFisher Scientific, Waltham, MA, USA) for the collected spectra.
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2

Spectroscopic Characterization of Materials

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To characterize the products, ATR-FTIR spectra were recorded on a Nicolet iS5 apparatus from Thermo Scientific, using a diamond iD7 transmission accessory (16 scans, 4 cm−1 resolution, 4000–400 cm−1). On the other hand, TGA residues were analyzed by Thermo Scientific iS 50 FTIR (32 scans, 8 cm−1 resolution and 4000–400 cm−1 for middle IR and 32 scans, 4 cm−1 resolution and 1800–100 cm−1 for far IR).
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Thermal Analysis Coupled with FTIR

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The TGA evolved compound were analyzed coupling the TGA instrument (TGA Q500 from TA Instruments, EGA furnace) with an Infrared (FTIR) spectrometer (Thermo iS 50 FTIR) by means of a TGA-interface. First, 10–15 mg of the sample was heated from 30 °C to 800 °C at a rate of 10 °C·min−1 under nitrogen atmosphere. The temperature of the Thermo Scientific transfer line between the thermobalance and the FTIR gas cell were set at 220 °C. The flow rate of nitrogen in the cell was set at 90 mL·min−1 and the spectra in the form of interferograms were continuously recorded in the spectral range of 4000–500 cm−1. Afterward, these interferograms were processed to build up the Gram–Schmidt (GS) reconstruction.
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Elemental and Spectral Analysis Protocols

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Microanalyses were performed using a CE–440 elemental analyzer (Exeter Analytical Inc.). Infrared spectra were obtained (KBr disk, 400–4000 cm−1) on Thermo Scientific iS50 FTIR. UV-visible and photoluminescence spectra were carried out with Thermo Scientific Evolution 201 UV-visible spectrophotometer and PerkinElmer LS55 fluorescence spectrophotometer, respectively.
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5

FTIR Analysis of POSS Nanoparticle Interaction

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FTIR was used to investigate the possible interaction between POSS® nanoparticles with the composite membranes. The IR spectroscopy experiments were carried out with a FTIR spectrometer (iS50 FT-IR, Nicolet, Thermo Fisher Scientific, Waltham, MA, USA) with a smart endurance reflection cell.
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6

Multimodal Spectroscopic Analysis of Materials

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Raman spectroscopy and Fourier-transform infrared (FT-IR) spectroscopy were performed on Thermo Scientific-Nicolet 6700 Raman Spectroscope and iS50 FT-IR (Bangalore, India), respectively. Surface morphology was visualized via scanning electron microscopy (SEM), and elemental composition was analyzed via energy dispersive X-ray (EDX) on ZEISS EVO SEM coupled with SmartSEM software (Germany). Cyclic and differential pulse voltametric experiments were carried out on PalmSens4 potentiostat from PalmSens (The Netherlands).
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7

Characterization of N-CDs Inhibiting Aβ Fibrillation

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PL and UV-vis absorption spectra were characterized by Horiba Duetta. The time-resolved PL spectra were obtained with a Horiba FluoroMax with a 455 nm laser. A transmission electron microscopy (TEM) image was performed by using a Japan Hitachi HT7700. The Raman spectrum was achieved by an Anton-Paar Cora 5001 with 785 nm of laser wavelength. The Fourier transform infrared (FT-IR) spectrum was characterized with a Thermo Scientific iS50 FT-IR. The X-ray photoelectron spectroscopy (XPS) spectrum was acquired using a Thermo ESCALAB 250Xi spectrometer. Dynamic light scattering (DLS) is a powerful tool used to monitor particle size evolutions. Aβ1–42 peptides were mixed with 6 mg/mL N-CDs incubated for 24 h at 37 °C and then the size distribution was measured by a ZetasizerNano ZS nanoparticle size analyzer (Malvern Instruments Ltd., Malvern, UK). Aβ1–42 solutions incubated with PBS were also utilized as controls. After measuring the effect of N-CDs on Aβ1–42 fibrosis by ThT and DLS as shown previously, the morphologies of the Aβ1–42 aggregates incubated with or without N-CDs were observed and visualized by TEM (Japan Hitachi HT7700, Japan, Tokyo).
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8

Structural and Dielectric Properties of CPs

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Powder X-ray diffraction (PXRD; Rigaku model RINT Ultima III diffractometer) profiles were obtained to explore the structure of the CPs. Surface morphology was determined by field emission scanning electron microscopy (FE-SEM; Zeiss Merlin Compac), and elemental distribution was investigated using energy dispersive spectroscopy (EDS) and the mapping software that came with the FE-SEM instrument. Fourier transform infrared (FT-IR) spectra were obtained using a Thermo iS50 FT-IR with KBr pellets in the range 400–4000 cm−1. X-ray photoelectron spectroscopy (XPS) was conducted with Al Kα radiation as X-ray source using a Kratos AXIS ULTRA X-ray photoelectron microscope. The dielectric constants of compounds 1 and 2 were measured within the range of 103–106 Hz at room temperature. The dielectric constants of compounds 1 and 2 were measured by a compass test platform at room temperature with an impedance analyzer (Agilent 4294A) in the frequency range of 103–107 Hz.
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FTIR Analysis of Immobilized Hydrogels

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The FTIR spectra of hydrogels after β-galactosidase immobilization were obtained by means of spectroscope Thermo Scientific, USA, model iS50 FTIR. The samples of hydrogels were evaluated in the region from 400 to 4000 cm -1 with resolution of 4 cm -1 and 64 scannings using the accessory of de ATR GladiATR diamond (Pike Technologies, USA).
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10

Comprehensive Characterization of Nanoparticles

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Attenuated total reflectance (ATR) FTIR spectra were acquired on a Thermo Scientific iS50 FTIR with ATR attachment. Absorption spectra were collected by obtaining 64 scans at autogain with a resolution of 2 cm−1. X-ray diffractograms were obtained using a Bruker D8 Discover XRD system. Cu-Kα X-ray generator with a wavelength of 1.54184 Å at a voltage 40 kV and 40 mA current was used. Surface and morphological analyses were conducted using a Zeiss Ultra Plus field emission scanning electron microscope (FESEM) equipped with an energy dispersive X-ray detector for elemental analysis. Powder sample was dispersed in formic acid to obtain a 0.1% (w/w) suspension, which was spin coated on silicon wafer to make the surface fairly conductive without using gold/carbon sputtering. Secondary electron (SE) detector images were obtained to analyse the morphology of the nanoparticles obtained. Raman analysis was performed on a Renishaw Invia-Raman microscope by using either 532 or 785 nm laser sources. Ca/P atomic ratio was determined by XRF using a Bruker Tiger S8 instrument.
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