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13 protocols using senterra spectrometer

1

Comprehensive Characterization of Lithium-Containing Ferrites

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Fourier-transform infrared (FTIR) detected the functional groups attached to the LCF surface (Shimadzu FTIR–8400 S, Kyoto, Japan). Raman spectra were recorded using (SENTERRA spectrometer, Bruker, Karlsruhe, Germany) with a 532 nm Ar laser. The LCF surface features and characteristic morphology were inspected by scanning electron microscopy using (SEM, JEOL Model JSM6360 LA, Tokyo, Japan) at room temperature with accelerating voltage 15 kV. The SEM device is equipped with an EDX detector to identify and map the synthesized LCF’s basic element structure. Magnetic characteristics of LCF were scrutinized by a vibrating-sample magnetometer (VSM, LakeShore-7410, Lake Shore Cryotronics, Inc., Westerville, OH, USA) with sensitivity up to 1 μ emu and a strong magnetic field up to ±20 koe to fully saturate the sample uniformly across the sample space.
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2

Raman Spectroscopy of Oxidation-Sensitive Samples

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Raman spectra were recorded by a SENTERRA spectrometer (Bruker Optics GmbH, Ettlingen, Germany) equipped with a 488 nm laser. Low laser powers (1 mW) were chosen in order to prevent oxidation of the samples. A baseline correction was accomplished with the software OPUS 7.2 for spectra measured by Raman spectroscopy using the concave rubber band method.
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3

Raman Scattering Spectroscopy Protocol

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Raman scattering spectra were collected on the Bruker Senterra spectrometer (spectral range 100–4,000 cm−1, incident laser 488 nm 20 mW, spectrum accumulation time 10 s).
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4

Multimodal Characterization of Materials

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The morphology of samples was characterized by SEM (JEOL JSM-2100, JSM-7800F, Japan), TEM (JEOL JEM-2100, Japan) and optical microscope (Keyence VHX-5000, Japan). The Raman spectra were recorded on a Bruker Senterra spectrometer (Germany). The SAXS patterns were recorded on an Antonparr Saxes M2 scattering system (Austria). The unit-cell parameters were calculated from the equation of a0 = 2d100/√3. The XPS measurement was conducted on a Thermo Fisher ESCALAB 250Xi spectrometer (USA) using Al Kα radiation (15 kV, 10.8 mA). The thermogravimetric analysis (TGA, Netzsch STA 449 F3) was performed from 40 to 900 °C with a heating rate of 10 °C min−1 under air atmosphere. The nitrogen adsorption/desorption isotherms were measured on a QuantaChrome Quadrasorb SI analyzer (USA) after vacuum degassing at 120 °C for 6 h. The specific surface areas and the pore volumes were calculated using the Brunauer–Emmett–Teller (BET) method. The pore size distributions were obtained from the adsorption branches of the isotherms using Barrett–Joyner–Halenda (BJH) model. The microporous specific surface areas and pore volumes were analyzed using t-plot method. The elemental analysis (C, N and H) of samples was carried out using an Elementar Vario EL III analyzer (Germany).
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5

Comprehensive Material Characterization Protocol

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High-resolution transmission electron microscopy images and energy dispersive X-ray spectroscopy analysis were manufactured on FEI Europe, model Tecnai F20 X-Twin operated at 200 kV and Quantax 200 with XFlash 4010 detector by Bruker AXS operated at 28 kV. X-ray powder diffraction patterns of samples were carried out by Philips X’Pert diffractometer, which was radiated by graphite monochromatized Cu Kα (λ equal 1.540598 Å). The operating voltage was maintained at 40 kV, the current was maintained at 30 mA and analyzed in the range from 20° to 90°. The X-ray photoemission spectroscopy was performed on PHI5000 PHI VersaProbeII spectrometer using focused monochromatic X-ray of the Al Kα line (1486.6 eV). The vacuum value during the measurement oscillated around 3 × 10−9 mbar. The elemental composition (C, N, H) was carried out using a Vario MACRO elemental analyzer from CHN ELEMENTAR Analysensysteme GmbH. Raman spectra were performed on Senterra spectrometer by Bruker Optik. N2 adsorption isotherms were carried out on ASAP 2020 Plus instrument (Micromeritics). The specific surface area and pore size distribution curves were determined by the Brunauer–Emmett–Teller (BET) method and density functional theory (DFT).
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6

Raman Spectroscopy of LDH Materials

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Raman spectra were measured on a Bruker Senterra spectrometer (Billerica, MA, USA) in the spectral range of 80–3700 cm−1, using a 785 nm laser (power 50 mW, single accumulation time 120 s, 8 repetitions) for ZnCr-LDHs and a 532 nm laser (power 5 mW, single accumulation time 60 s, 4 repetitions) for NiCr-LDHs. In the first case, the signal was collected in a luminescence subtraction mode and the region of 1500–3700 cm−1 was upscaled 10 times.
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7

Raman Spectroscopy of Materials

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The Raman spectra were measured using a Bruker Senterra spectrometer operated in backscattering mode at ambient conditions. The utilized wavelength of 532 nm was obtained from a frequency-doubled Nd:YAG laser. A 50× objective and a thermoelectrically cooled CCD detector (−65 °C) were used. The spectral resolution of the system is 2–3 cm−1.
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8

Raman Spectroscopy Hydrogel Analysis

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Raman spectroscopy measurements were obtained from a composition comprising 30 ​nL SAP, 60 ​nL PEGMA, 10 ​nL DMAEMA, and 30 nLl PEGDMA (5 ​mol%) with a Bruker Senterra spectrometer (Bruker Optics, Germany). For focusing of the excitation laser and collimation of backscattered light an Olympus MPLAN 20 ​× ​objective (NA 0.4) was used, resulting in a spot diameter of 5 μm on the sample surface. The excitation laser (λ ​= ​532 ​nm) was operated at 10 ​mW output power. Each spectrum was integrated over 60 ​s with three coadditions (3 ​× ​20 ​s). The total number of measurement spots per hydrogel micropad was 144, arranged in a 12 ​× ​12 matrix (Fig. S4).
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9

Raman Spectroscopy and SEM Analysis of Samples

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The Raman spectra were obtained using a Bruker SENTERRA spectrometer, solid state laser excitation operating at a wavelength of 785 nm and a CCD detector. The measurements were made with resolution of 3–5 cm−1, aperture of 25 × 1000 μm and over a spectral range of 1780 to 390 cm−1. The laser power at the exit of the laser was 50 mW and 10 accumulations were made with an acquisition time of 50 s each. These parameters were previously adjusted to obtain the best signal-to-noise ratio without altering the physical and chemical integrity of the samples. The spectra obtained were treated with OPUS 7.0 and Origin 8 software from Bruker and a baseline correction was applied.
SEM measurements were performed in a scanning electron microscope combined with an Energy dispersive X-ray spectroscopy (EDS) Hitachi model TM 3000 compact instrument, with a smoothing magnification of 15x up to 30,000x (digital zoom: 2x and 4x), which allows topographic images to be obtained with a large depth of focus. No sample preparation was required for the analyses, and each one of the samples were fixed in a specific metallic sampler from the SEM equipment.
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10

Raman Spectra of Samples

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Raman spectra were obtained on a Bruker Senterra spectrometer (spectral range 100–4,000 cm−1, laser 488 nm, 20 mW, spectrum accumulation time 10 s).
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