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31 protocols using labram hr spectrometer

1

In Operando Raman and XRD Spectroscopy

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Raman spectra acquisition during cell operation has been described in detail elsewhere and is schematically shown in Supplementary Figure 5 (ref. 39 (link)). For the measurements, a special electrode was used which was prepared by mixing the active materials with super P and 5 wt% PTFE in water to obtain a homogenous slurry. The final content of the active materials was 80 wt%. The slurry was rolled into a thin film, which was then pressed onto a stainless-steel mesh. A delicate battery cell with a quartz window on the top was used (Supplementary Figure 5). The Raman spectra were recorded on a MicroRaman system (LabRAM HR spectrometer, Horiba) with an Olympus BX microscope and an argon ion laser (532.05 nm). Each spectrum was acquired for 20 s. The galvanostatic discharge of the cell was controlled by an electrochemical workstation (PARSTAT 4000). A similar battery cell to that used for the in operando Raman spectroscopy was designed, replacing the quartz window with a Kapton film window to perform the in situ XRD measurements (Supplementary Figure 8).
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2

Structural Characterization of TiO2 Nanocrystals

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Transmission electron microscope (TEM) images and selected area electron diffraction (SAED) patterns of the TiO2 nanocrystals were obtained using a JEOL 2010F transmission electron microscope operated at 200 kV. Raman spectra were collected using a Raman spectrometer (LabRAM HR spectrometer, Horiba) with a 532.05-nm Ar-ion laser. XRD patterns were recorded over the range 20–80° on a Rigaku diffractometer equipped with a Cu Kα radiation source operated at 40 kV and 120 mA.
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3

Raman Spectroscopy of Single Crystals

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Unpolarised Raman spectra were measured with a Horiba LabRAM HR spectrometer using a Peltier cooled multichannel CCD detector. An objective lens with a 50× magnification was linked to the spectrometer, allowing the analysis of samples as small as 2 μm in diameter. The samples were in the form of single crystals. The incident radiation was produced by a He-Ne laser line at a power of 17 mW (λ = 632.8 nm). The focal length of the spectrometer was 800 mm, and an 1800 gr mm -1 grating was used. The spectral resolution was approximately 1 cm -1 with a slit of 100 μm. The spectrum was recorded in
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4

Biomorphic Calcium Carbonate Precipitation

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After crystallization, the resulting biomorphic precipitates are extracted out of the growth cassette and then analyzed by X-ray diffraction (Bruker D8 Venture, Cu Kα). In all cases and for all temperatures the precipitates are composed of monohydrocalcite (Supplementary Fig. 3). The crystallization at 45 and 60 °C are also analyzed by time-lapse measurements at different growth stages (12, 24, and 48 h) by in situ Raman microspectroscopy with a wavelength of 532 nm (LabRAM-HR spectrometer, Jobin-Yvon, Horiba, Japan). All the spectra collected from the biomorphic aggregates under these temperatures exhibit clear bands at 696, 719, and 1067 cm−1 (Supplementary Fig. 4), which correspond to the characteristic peaks of the carbonate group in monohydrocalcite. In addition, the sea urchin-like heterotextured architectures formed by stepwise adjustment of temperature of growth (25–70 °C) are also identified as monohydrocalcite by X-ray diffraction (Supplementary Fig. 3).
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5

Comprehensive Material Characterization

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The P-XRD analysis employed Cu Ka radiation and was conducted using the X Pert PRO X-ray Diffraction instrument. The SEM and EDX studies were investigated using a JEOL JSM-6510LA electron microscope, while a JEOL Model JEM1400 instrument was used for the TEM study. The materials were synthesized using a HD150 PAD model Muffle Furnace, and the Autolab PGSTAT204 FRA32M was utilized to carry out CV and DPV studies. The Raman spectra were obtained from various locations of the sample using a Jobin Yvon LabRam HR spectrometer equipped with Ar laser 632 nm. XPS measurements were conducted via Omicron spectrometer with Al Ka as the X-ray source (1486.6 eV) to examine the atomic ratio of the elements and determine the corresponding elemental composition of the samples.
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6

Multimodal Characterization of Graphene

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The optical images were taken using a Nikon microscope. SEM images were obtained using a LEO-1530 microscope (LEO Electron Microscopy. GERMANY). Raman spectra were collected with a HORIBA Lab RAM HR spectrometer (514 nm laser excitation) (HORIBA Jobin Yvon. FRANCE). Raman mapping images were recorded by a Raman 11 spectroscopy (Nanophonon. JAPAN). AFM images were acquired by a SPM-960 instrument (SHIMADZU. JAPAN). The transmission spectra of graphene were obtained with a UV-visible spectrophotometer.
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7

Comprehensive Characterization of NGO Crystals

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PL properties of NGO single crystals and thin films were studied by exciting with the 325 nm line of a He-Cd laser with a spot size of ~800 nm and a power of 10 mW, (laser intensity ~1.5 MW/cm2) and recorded using a JY-Horiba LabRAM HR spectrometer. Further elemental composition, valence and structural analyses were done using Rutherford backscattering spectroscopy ((using 3.5 Mev singletron accelerator)), secondary ion mass spectroscopy (using ToF-SIMS-IV from ION-TOF GmbH), x-ray photoelectron spectroscopy (using Axis Ultra Delay Line Detector from Kratos Analytical) and x-ray diffraction (using Empyrean powder XRD system from PANalytical).
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8

Raman Spectroscopy of Material Samples

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Raman spectroscopy was performed using a HORIBA Jobin Yvon LabRAM HR spectrometer. Spectra were acquired using a 532 nm laser at 25 mW power, a 50×
objective, and a 300 μm confocal pinhole. To simultaneously scan a range of Raman shifts, a 600 lines/mm rotatable diffraction grating along a path length of 800 mm was employed. Spectra were detected using a SYNAPSE CCD detector (1024 pixels)
thermoelectrically cooled to -60 °C. Prior to spectral collection, the instrument was calibrated using the Rayleigh line at 0 cm -1 and a standard Si (100) reference band at 520.7 cm -1 . Spectra were recorded for 20 s and 20 accumulations.
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9

Unpolarized Raman Spectroscopy of Crystals

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Utilizing a Peltier cooled multi-channel CCD detector, the unpolarized Raman spectra were recorded with a Horiba LabRAM HR spectrometer. All the samples were in the form of single crystals. An objective with a 50× magnification was linked to the spectrometer, allowing the analysis of samples as small as 2 µm in diameter. The incident radiation was produced by a He-Ne laser at a power of 17 mW (λ = 632.81 nm). The focal length of the spectrometer was 800 mm and a 1800 gr mm -1 grating was used. The spectral resolution was around 1 cm -1 with a slit of 100 µm. The Raman spectroscopic investigation for all the samples was executed at room temperature in the range of 100-1050 cm -1 .
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10

Characterization of As-Prepared Samples

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The structural features of the as-prepared samples were investigated by scanning electron microscopy (SEM) using a FEI Quanta 3D FEG instrument. Energy-dispersive x-ray spectroscopy (EDAX) analysis was performed on an Apollo XL instrument fitted with a Quanta 3D-5 Microscope (Port: EDAX). Transmission electron microscopy (TEM) was performed using a JEOL, JEM 3010 instrument (300 kV) fitted with a GATAN CCD camera. The powder x-ray diffraction (PXRD) patterns were recorded on a Bruker AXS, D8 Discover x-ray diffractometer using Cu Kα irradiation (λ = 1.54187 Å) in a 2θ range from 15 to 90°. A TGA 850C, Mettler Toledo thermogravimetric analyzer was used to evaluate the weight loss on heating. 10 mg of the sample was heat-treated in a ceramic crucible from 30 to 900 °C at a constant heating rate of 5 °C min−1 under a N2 atmosphere (flow rate of 40 mL min−1). To study the surface properties, x-ray photoelectron spectroscopy (XPS, VG Scientific ESCA LAB V) was used. Raman spectroscopy was performed at different locations of the sample using a Jobin Yvon LabRam HR spectrometer with a 514.5 nm Ar laser. N2 and O2 adsorption studies were performed at a 77 K temperature using a QUANTACHROME QUADRASORB SI analyzer and an AUTOSORB IQ2 instrument. Prior to the adsorption studies, all the samples were kept at 200 °C under high vacuum for 12 h.
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