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Dektakxt surface profiler

Manufactured by Bruker

The DektakXT surface profiler is a high-resolution profiling instrument designed to measure surface topography and roughness. It uses a precise stylus to scan the sample surface and generate detailed profiles and measurements. The DektakXT is capable of providing accurate and repeatable data on a wide range of sample types and surfaces.

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5 protocols using dektakxt surface profiler

1

Comprehensive Materials Characterization of SEBS Nanocomposites

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The Fourier transformed
infrared spectroscopy (FTIR) test of SEBS, MA-g-SEBS,
and their nanocomposites were conducted on a Perkin-Elmer 1000 FTIR
spectrometer. Raman spectra were measured on a ThermoFisher/DXR. The
X-ray diffraction (XRD) measurement was carried out on a Rigaku D/Max
2550 (Cu Kα, λ = 1.5418 Å) with a 2θ scan configuration
in the range of 5°–40°. X-ray photoelectron spectroscopy
(XPS) experiment was performed on a Shimadzu-Kratos (AXIS Ultra).
Typical tapping-mode atomic force microscope (AFM) measurements were
taken on a SIINT NanoNavi E-Sweep, with which not only the single-layer
GO platelets were observed but also the microscopic surface roughness
of the hybrid films was measured. Macroscopic surface roughness of
the films was obtained from a Bruker DektakXT Surface Profiler. The
sandwich structure of the LBL assembled films was observed using a
JEOL JSM-7401F scanning electron microscope at an acceleration voltage
of 5 kV, and all the samples were fractured after immersion in liquid
nitrogen for a few minutes. Dynamic mechanical analysis (DMA) was
carried out using a NETZSCH DMA 242 C/1/G instrument. The tensile
tests were conducted on a MTS Criterion Model 43 universal testing
machine, with a crosshead speed of 500 mm/min at the temperature of
25 °C.
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2

Characterization of Printed TiO2 Films

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The thickness and the roughness of the printed TiO2 films were measured using a Bruker Dektak XT surface profiler (a stylus radius of 12.5 μm, a stylus force of 2 mg, a scan speed of 100 μm s−1, and a scan resolution of 0.33 μm). The Raman spectroscopy measurements were performed using a Renishaw inVia Raman spectrometer equipped with a laser with a 514.5 nm excitation wavelength and 0.5 mW power. A 100× objective and a grating of 2400 g mm−1 were used. Surface morphology was visualized using scanning electron microscopy (Zeiss Gemini Ultra55).
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3

Characterization of Polymeric Materials

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Steady-state photoabsorption spectra
were recorded using a Jasco V-570 UV–vis spectrophotometer.
The molecular weight (weight-averaged: Mw) and polydispersity index (PDI) of polymers were measured using
the size exclusion chromatography (gel permeation chromatography:
GPC, a Shimadzu Corp. LC-20AT/CBM-20A/CTO-20A/ SPD-M20A) with polystyrene
standards in hot chloroform (40 °C) as an eluent. Photoelectron
yield spectroscopy (PYS) of the polymer films on indium–tin–oxide
(ITO) glass was performed using Bunko Keiki BIP-KV2016K. 2D-GIXD experiments
were performed on the beam line BL46XU at the SPring-8 (12.39 keV,
λ = 1 Å X-ray). The 2D-GIXD patterns were monitored with
a 2D image detector (Pilatus 300 K). Atomic force microscopy (AFM)
was performed using a Bruker Innova AFM microscope. Differential scanning
calorimetry (DSC) was carried out using a Netzsch DSC204F1 Phoenix
differential scanning calorimeter under N2 at 10 °C
min–1 (sample weight ∼2 mg). Thicknesses
of the polymer and blend films were measured using a Bruker Dektak
XT surface profiler. Xe-flash time-resolved microwave conductivity
(TRMC) was performed for the polymer:PCBM films prepared on a quartz
substrate. The microwave frequency and excitation light were ∼9
GHz and a white light from a Xe-lamp (pulse width ∼ 10 μs).
The details are in the reference.70 (link)
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4

Thin Film Thickness Measurement

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The thickness
of the thin
films was determined with a Bruker DekTak XT surface profiler. The
scan length was set to 1000 μm over the time duration of 3 s
with the hills and valleys scanning profile. The diamond stylus had
a radius of 12.5 μm, and the employed force was 3 mg. The measured
profile was then used to determine the thickness. Each layer thickness
has been determined by averaging six measurements on three different
spots on the thin films.
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5

Dispersion and Deposition of SWCNTs

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In a round bottom flask, 100 mg SWCNT was added to 100 mL 1,2dichloroethane. The mixture was cooled with an ice bath and fully dispersed in an ultrasonic homogenizer at a power of 95 W for 90 min. Then 1.0 mL of the formed dispersion was transferred to a glass vial containing the polymers and the vial was sonicated at 0 °C for 2 h. The dosage of the polymer depends on the doping ratio. The resulting gellike mixtures were added to clean glass substrates in a dropwise manner until the substrates were fully covered, and the thin films would be ready for subsequent characterizations after solvent evaporation. The abovementioned doping method could eliminate the undesired effects resulting from the soluble impurities adsorbed by SWCNTs including residual reactants, soluble oligomers or free metal ions. The length and the width of the as-prepared films were both 15 mm and the thickness was measured on a Bruker DektakXT surface profiler with a diamondtipped stylus whose radius was 2.5 μm.
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