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369 protocols using axis ultra dld

1

Comprehensive Microstructural Analysis of Nanofibers

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The crystalline microstructures of the samples were examined by XRD (X-ray diffraction, Rigaku D/Max-2400 diffractometer, Cu Kα radiation, λ = 0.15406 nm) in the range of 10–80° with a scanning speed of 2° min−1. The applied tube voltage and current were 40 kV and 30 mA, respectively. The element types, valence states and detailed chemical bonding energy were investigated by X-ray photoelectron spectroscopy (XPS, Kratos AXIS Ultra DLD, Al Kα probe beam, the applied photoelectron energy hv = 1486.6 eV), and the nanofiber sample was pressed into a film by a tablet press and evacuated for 1 day before testing. The fitting software of the high-resolution spectra was XPS Peak.
To prepare the FE-SEM (field-emission scanning electron microscopy, S-4800, Hitachi) characterization, the sample is glued to the metal table with conductive glue. In addition, a TEM (transmission electron microscopy, FEI, Tecnai G2 F20) with EDX (energy dispersive X-ray) spectroscope was applied to acquire the detailed microstructure and composition. During the sample preparation, the sample was first put into an alcohol solution and ultrasonicated for about 10 min. Next, a dropper was used to draw a small amount of supernatant onto the micro-grid. Finally, the micro-grid with the sample was dried for a few minutes to evaporate alcohol.
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2

Characterization of Graphene Oxide by AFM

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The samples were characterized by using a MultiMode 8 AFM (Bruker) equipped with a J scanner. Silicon cantilevers coated with a 30 nm Pt layer with a nominal spring constant of 2.8 N·m−1 and oscillating frequencies of 60–90 kHz (NSC18/ Pt, MikroMasch Co.) were used. Height and adhesion mapping were conducted in PeakForce Quantitative Nano-Mechanics (PF-QNM) mode, in which the maximum force (peak force) applied to the sample by the tip was directly regulated through the peak force setpoint and kept constant throughout the whole scan. In this mode, the peak force amplitude was set at 150 nm, the Z-piezo oscillation frequency at 2.0 kHz, and the scan rate at 1 Hz. Voltage to the tip was applied using the scan parameter “tip bias”. All AFM experiments were conducted under ambient conditions at a room temperature of 18–25 °C and relative humidity of 35–60%. AFM images of the samples were processed using the software Nanoscope Analysis v1.7. For each image, a first-order flatten correction was applied to remove sample inclination. The reduction extent of the GO was characterized by X-ray photoelectron spectroscopy (XPS, AXIS Ultra DLD, Kratos).
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3

Comprehensive Characterization of Polymer Materials

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ICP-OES measurements were performed on an Agilent ICP-OES 730, while ICP-MS measurements were conducted on an Agilent ICP-MS 7850.
SEM characterization was conducted on a Zeiss sigma 300, or on Zeiss Merlin Compact.
FTIR spectroscopy was conducted on Bruker VERTEX80v or Thermo Fisher Nicolet iS 10 on a range from 400 to 3000 cm−1.
XPS characterization were conducted on a Kratos AXIS Ultra DLD using Alka-ray source (hv= 1486.6 eV). Operation vacuum, voltage, filament current, and pass energy is 1×10−9 mBar, 15 kV, 10 mA and 30 eV.
HRTEM photographs and EDX mapping and spectra were obtained on a Tecnai G20 20 TWIN UEM.
The specific surface area and pore size distribution of FEP powder were obtained using the Brunauer– Emmett–Teller (BET) approach with BSD-660S.
The TG-DSC analysis was conducted on NETZSCH STA 449 F5 using N2 atmosphere. The ramp is 10.00 °C per min.
GPC was employed to measure the molecular weight of PP. The experiment was carried on Agilent PL-GPC 220 with PLgel 10um MIXED-B LS 300×7.5 mm tandem column, using 150°C 1,2,4-Trichlorobenzene as the solvent. The flow is 1 mL min−1.
The molecular weight of FEP and PTFE was calculated based on the data provided by Dupont (SSG method), using the formula30 : LogMn¯=2.61SSG0.06
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4

Multimodal Characterization of AZO-GO Hybrids

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Fourier transform infrared spectroscopy (FT-IR) spectra were recorded on NEXUS-670 spectrometer with a disc of KBr. X-ray photoelectron spectroscopy (XPS) analyses were performed with a Kratos Axis Ultra DLD on model surface analysis system with a 450 W Mg Kα X-ray (1000–1500 eV) source at a base pressure in the 10−8 to 10−9 Torre range. Thermogravimetry-differential analyses (TGA) of the samples were conducted in air condition by using a STA PT1600 simultaneous thermal analyzer (Linseis Germany). The energy density of AZO-GO was evaluated by differential scanning calorimetry (DSC) on the same apparatus with the heating rate of 5 °C/min during the temperature range of 20 °C to 180 °C. The X-ray diffraction (XRD) patterns were taken by an X′Pert Pro X-ray diffractometer of Philips using Cu Kα radiation (λ = 0.15 nm) at a voltage of 40 kV and a current of 40 mA. UV–vis absorption spectra were recorded at room temperature in ethyl alcohol solution on a UV–vis spectrophotometer (LG-722SP). Time evolutions of the absorption spectra of the AZO-GO and AZO-RGO hybrids in ethyl alcohol solution (1 × 10−4 g/mL) upon irradiation of UV light at 365 nm were performed by Perkin Elmer950 spectrometer at room temperature. Raman spectra were recorded by J.Y.HR800, all sample powders were measured excited at 532 nm.
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5

Comprehensive Characterization of Composite Materials

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The structure and morphology were investigated by field-emission scanning electron microscopy (FE-SEM, INSPECT F50) and transmission electron microscopy (TEM, ZEISS Libra 200). Powder X-ray diffraction (XRD) measurements were conducted to determine the phase of the as-synthesized composites with Cu Kα radiation operated at 40 kV and 30 mA. X-ray photoelectron spectroscopy (XPS) analysis was performed on a Kratos AXIS Ultra DLD instrument using monochromated Al Kα X-rays as the excitation source. Raman spectra were collected using a Witec alpha 300M+ instrument with an excitation laser wavelength of 488 nm. Nitrogen adsorption–desorption isotherm measurements were conducted at 77 K using a micromeritics system (JW-BK132F). The contents of amorphous carbon, rGO and sulfur in the samples were analyzed by thermogravimetric (TGA) on a Netzsch STA 449C analyzer in air for the amorphous carbon and rGO or in N2 atmosphere for the sulfur at a temperature ramp rate of 10 °C·min−1.
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6

Characterization of Hybrid Materials

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All the solid samples
synthesized were characterized by powder XRD using a PANalytical X’pert
Pro diffractometer (Cu Kα radiation, secondary graphite monochromator,
scanning rate of 1° 2θ/min). IR spectra of the samples
were recorded using a PerkinElmer FT-IR spectrometer, Spectrum TWO,
UATR TWO. SEM analysis of the hybrid wafers was carried out using
a Zeiss Ultra 55 field emission scanning electron microscope. UV–visible
spectra of the reaction mixtures were recorded on a PerkinElmer (LS
35) UV–visible spectrometer. XPS measurements were carried
out with Kratos Axis Ultra DLD. All spectra were calibrated to the
binding energy of the C 1s peak at 285 eV.
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7

Comprehensive Characterization of Material Samples

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The crystal structures of the samples were characterized by using an X-ray diffractometer (XRD) (AXS D8 Advanced XRD, Germany) with Cu-Ka radiation. The microstructures were observed by using a high-resolution transmission electron microscope (HRTEM) (JEOL JEM 2010, Japan). X-ray photoelectron spectroscopy (XPS) measurements were made on a Kratos AXIS Ultra DLD (Kratos, Japan) spectrometer with a charge neutralizer to gain information on the chemical binding energy of the samples. The C 1s peak at 284.6 eV of the adventitious carbon was referenced to rectify the binding energies. Raman measurement was carried out using a Raman spectroscopy (HORIBA Jobin Yvon LabRAM HR, France). The power of the laser was 10 mW, and the laser excitation was 488 nm. Scans were taken on an extended range (100–3000 cm−1), and the exposure time was 2 s.
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8

Characterization of Perovskite Catalyst Powders

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Phase structures of the as-prepared catalyst powders were determined by XRD on Bruker (D8 Focus, Cu Kα radiation). Program FullProf was employed for the diffraction refinement. SEM images were performed on a SU-8010 SEM, whereas high resolution TEM images equipped with EDS were conducted on a Tecnai G2 F20 U-TWIN TEM. XPS measurements of the catalysts were carried out on a Kratos Axis Ultra DLD instrument. The obtained XPS spectra were calibrated by referencing C 1 s to 284.6 eV, and simulated using the XPSPEAK41 software. We analyzed the specific surface areas by Brunauer Emmet Teller (BET) system with N2 as the adsorptive medium. Approximately 2.0 g samples were weighed and degassed at 250 °C for 4 h before nitrogen physisorption at the temperature of liquid nitrogen (77 K). The ability of perovskites to adsorb OH after exposure to water (100% humidity) at room temperature for 2 h was estimated from the Fourier transform infrared spectra (FTIR, Nicolet iS50, Thermo Scientific America). Oxygen temperature programmed desorption (O2-TPD) measurement was surveyed to analysis the oxygen desorption properties.
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9

Comprehensive Characterization of Nanopowders and Polymer Composites

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The structural properties of the nanopowders and the polymer composites
were investigated using an X-ray diffractometer (MiniFlex 2, Rigaku,
equipped with Nickel-filtered Cu Kα radiation (λ = 0.1564
nm) operated at 30 V and 15 mA in the 2θ range of 10–30°
at a scanning speed of 1.8°/min) and an Fourier transform infrared
(FTIR) spectrometer (PerkinElmer Spectrum 400 spectrophotometer in
the range of 400–4000 cm–1 with a resolution
of 2 cm–1). The surface morphology was studied using
a scanning electron microscope (SEM, XL-30E Philips Co., Holland)
and a transmission electron microscope (TEM, FEI TECNAI G2 TEM). The ζ-potential measurements to determine the surface
charge on the nanoparticles were performed by dispersing the nanoparticles
in water using a Zetasizer Nano (Malvern) analyzer. X-ray photoelectron
spectrum was recorded using Kratos Axis Ultra DLD. The dielectric
properties were tested by broad-band dielectric/impedance spectroscopy
(Novocontrol) in the frequency range of 10–107 Hz.
The piezoelectric device fabrication and the testing system were similar
to our previous reports.2 (link),26 (link),27 (link)
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10

Characterization of Ceramic Electrolyte Materials

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The results of XRD
were characterized using an X’Pert PRO (PANalytical, Netherlands)
instrument with Cu Kα radiation with a 0.02° step at room
temperature. The prepared CEMs were analyzed by X-ray photoelectron
spectroscopy (XPS, Kratos AXIS Ultra DLD, Japan). Also, the anode
was mono [Al (Mono)] (45 W). The morphologies of the prepared CEMs
were characterized using scanning electronic microscopy (SEM) (Hitachi
S-4800) at an accelerating voltage of 15 kV.
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