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11 protocols using phi 5600

1

Characterization of V2O5·nH2O/CNT Films

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The morphologies of V2O5·nH2O/CNT films before and after cycles were examined on scanning electron microscopes (SEM, 6335F and TESCAN VEGA3) and a transmission electron microscope (TEM, JEOL 2100F). Spectrum imaging of electron energy loss spectroscopy (EELS) was carried out under 200 kV accelerating voltage with a 13 mrad convergence angle for the optimal probe condition. Energy dispersion of 0.7 eV per channel and 21 mrad collection angle were set up for EELS; HAADF images were acquired with an 89 mrad inner angle simultaneously. The crystalline phases of the materials were detected on an X-ray diffraction (XRD) system (Rigaku SmartLab) with Cu Ka radiation source. To determine the water and CNT content in V2O5·nH2O/CNT, thermogravimetric and differential thermal analysis (TGA-DTA) was conducted in the temperature range of 25-600°C at a heating rate of 10°C min−1 under N2 and air atmosphere, respectively. X-ray photoelectron spectroscopy (XPS, PHI5600 by Physical Electronics, Inc.) was conducted using monochromatic Al Ka X-ray at 14 kV. The solubilities of V2O5·nH2O in different electrolytes were measured by inductively coupled plasma mass spectrometry (ICP-MS).
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2

XPS Analysis of Surface Composition

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Quantitative chemical composition was analyzed by an X-ray photoelectron spectrometer (XPS; PHI 5600, multi technique system, Physical Electronics, USA). The XPS spectra was obtained with an Al Kα excitation source (ht1/41486.6 eV) and a take-off angle of 45 at a passing energy of 187.85 eV. All the spectra were obtained after sputtering the coating surface with argon ions to remove possible surface contamination.
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3

Characterization of Neuromorphic Device

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The neuromorphic device was analyzed with the KEYSIGHT B2902A source measuring unit. The XPS spectrum was measured by a PHI 5600 (Physical Electronics) with an Al X-ray monochromator, which uses photoelectrons excited by X-ray emission for surface characterization up to a depth of 2–5 nm. FTIR was performed using a Bruker I.F.S. The Raman spectrum was measured by a HORIBA LabRAM HR confocal spectrometer equipped with an 800-nm-long monochromator. The He-Cd laser was shined on the surface of the sample with an excitation wavelength of 325 nm.
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4

X-ray Photoelectron Spectroscopy Analysis Protocol

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X-ray photoelectron spectroscopy (XPS) data were recorded on a multi-surface analysis system (PHI 5600, Physical Electronics, Chanhassen, MN, USA) with a monochromatic AlKα X-ray source (1486.6 eV). Sample spot sizes varied from 200 to 400 µm in diameter. The pass energies of exciting radiations were set at 187 and 45 eV for survey and elemental scans, respectively. The energy and emission currents of the electrons were 4 eV and 0.35 mA, respectively. Energy resolution was at 0.7 eV with a chamber pressure of 5 × 10−10 torr. Spectral calibration was determined by setting the C 1s component at 285.0 eV. All data acquisition was processed with a PC-based Advantage software (version 1.85, Advantage Software Co., Stuart, FL, USA). The surface composition was determined by using the manufacturer’s sensitivity factors. Curve fitting of the spectrum was accomplished using a nonlinear least-squares method. A Gaussian function was assumed for the curve fitting. The deconvolution of carbon, oxygen, and nitrogen peaks was processed with MagicPlot software (version 2.5.1, MagicPlot Systems, St. Petersburg, Russia).
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5

Comprehensive Material Characterization

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Samples morphology was characterized by scanning electron microscope (SEM, FE-SEM 4800SEM, Hitachi, Japan) coupled with an energy-dispersive X-ray Spectroscope (EDAX Genesis, fitted to the SEM chamber), while their chemical composition and chemical state was investigated by using X-ray photoelectron spectroscopy (XPS, PHI 5600, Physical Electronics, US)—peaks were shifted to C1s 284.8eV.
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6

Characterization of Nanostructured Materials

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Transmission electron microscopy (TEM) was performed on a FEI Tecnai G2 F20 S-TWIN (Hillsboro, OR, USA) operated at 200 kV. X-ray photoelectron spectroscopy (XPS, Physical Electronics PHI 5600, Chanhassen, MN, USA) measurement was carried out with a multi-technique system using an Al monochromatic X-ray at a power of 350 W. Nitrogen adsorption/desorption isotherms were measured at 77 K using a Micromeritics TriStar II 3020 analyzer (Norcross, GA, USA). Before the measurements, the samples were outgassed for 12 h in the degas port of the adsorption apparatus, at 473 K for the calcined samples. The total surface area was analyzed with the well-established Brunauer-Emmett-Teller (BET) method, and the pore size distribution was calculated on the basis of adsorption branches of nitrogen isotherms using the Barrett-Joyner-Halenda (BJH) method.
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7

Characterization of g-C3N4 Photocatalyst

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The concentrations of free chlorine were determined by a DPD colorimetric method. 39 Concentrations of CBZ, NB, BA and DMOB were determined by a reverse phase UPLC (VP series, Shimadzu) equipped with a Waters symmetry C18 column (4.6 mm × 150 mm, 5 μM particle size; Waters) and a UV detector. The flow rate was 1.0 mL/min and the mobile phase was a mixture of water (pH 3, adjusted using phosphoric acid) and methanol (55/45, v/v %). 40 The detection limits of CBZ, NB and BA are 0.06, 0.10, 0.04 and 0.13 μM, respectively.
Before and after reactions the g-C3N4 was subjected to material characterization. The surface morphology of the g-C3N4 samples were characterized by SEM. The elemental composition of the g-C3N4 were obtained by XPS (PHI 5600, Physical Electronics Inc., Al Kα radiation (1486.8 eV), USA). The optical properties of the g-C3N4 were characterized by UV-Vis diffuse reflection spectroscopy (UV-vis DRS, PerlomElmer Lambda 950, USA).
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8

Characterization of Sensor Morphologies

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The morphologies of sensors were characterized using a field-emission scanning electron microscopy (SEM, JSM-7100). An optical microscope (Olympus LC30) was used to characterize the morphological variations during the loading/unloading cycles. The X-ray photoelectron spectroscopy (XPS, PHI5600, Physical Electronics) was used to quantitatively measure the chemical compositions of CNTs with and without PDA treatment. The electrical conductivity was measured using a four-point probe method (Ecopia HMS-5500). The electromechanical performance of sensors was evaluated on a universal testing machine (MTS I2) where a digital multimeter (34970A Data Acquisition/Data Logger Switch Unit, Agilent) was used to continuously record the corresponding resistance changes with strains.
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9

X-ray Photoelectron Spectroscopy of Bioemulsifier

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XPS analysis was carried
out on a bioemulsifier film deposited
on a glass slide by using a PHI5600 photoelectron spectrometer (Physical
Electronics, Eden Prairie, MN, USA) to reveal the chemical states
of the elements in BSP-1–BSP-4 fractions. The emitted photoelectrons
were detected by a hemispherical analyzer set at an angle of 45°.
The total acquisition time was 2 min and 0.3 s. Core-level spectroscopy
with a constant pass energy mode of 20 eV was equipped with an energy
step size of 0.05 eV.26 (link) Data analysis was
performed by XPS PEAK 4.1 software.
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10

Copper Oxide/Carbon Nanocomposite Characterization

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The binding energies of the copper oxide/carbon in the nanocomposite were determined by X-ray photoelectron spectroscopy (XPS, ULVAC-PHI, Inc. PHI5600). Al K radiation (hv = 1486.6 eV) was employed for the photoelectron excitation. The preparation of the sample for XPS analysis was carried out in the glove-box. The sample was dried in the glove-box before studying, and after drying it was placed in a special container for XPS measurement.
The structure of copper oxide/carbon nanocomposite was characterized using a Ranishaw’s inVia Reflex Raman microscope.
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