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- Data for: Rational design 2D/2D BiOCl/H+Ti2NbO7- heterojunctions for enhanced photocatalytic degradation activityThe detailed research data of the submitted manuscript.
- Data for: Investigate of Nano-Grinding of Monocrystalline Copper-Silicon Substrate: A Molecular Dynamic Studya data file including forces and temperature
- Data for: Influence of pulse duration and pulse frequency on micro-roughness for laser micro polishing (LµP) of stainless steel AISI 410Supplementary data for publication "Influence of pulse duration and pulse frequency on micro-roughness for laser micro polishing (LµP) of stainless steel AISI 410" Report of the conducted experiments and analyzed roughness spectra from WLI images.
- Data for: Oleic acid addition for enhancing the wet ball milling preparation of zirconium hydride (ZrH2) microparticles and the inhibition of surface oxidationthe origin data for ultrafine ZrH2 preparation
- Data for: Surface engineering of magnetic and mechanical properties of Ta/Pt/GdFeCo/IrMn/Pt heterostructures by femtosecond laser pulsesdata files of MOKE and nanohardness measurements for the main text and supporting materials
- Data for: Polyaniline nanowire arrays aligned in hydrogel polymer electrolyte for high performance flexible supercapacitorsMorphological and structural characterizations and electrochemical performance of polyaniline.
- Data for: Effects of Air Nonequilibrium Atmospheric-Pressure Plasma Jet Treatment on Characteristics of Polypropylene Film SurfacesFig. 3. (a) Waveform of the voltage applied to the twisted wires and (b)−(e) waveforms of discharge currents following into the cylinder electrode and the sample stage, IC and IS, for 3 and 10 l/min air plasma jets at a nozzle-to-sample distance of 1 mm. Fig. 4. RMS discharge currents flowing into the cylinder electrode and the sample stage, IC and IS, for air and Ar plasma jets generated at various nozzle-to-sample distances, as a function of gas flow rate. Fig. 5. Comparison between the spectra of light emitted from (a) air and (b) Ar plasma jets. The inset shows the Ar plasma spectrum magnified at the UV range of 280−400 nm in wavelength. Fig. 6. Contact angles of PP film surfaces treated with air and Ar plasma jets, as a function of treatment time. In each figure, the contact angle at zero treatment time corresponds to that of untreated PP film surface. Fig. 7. XPS spectra of C 1s regions of (a) untreated PP film surface, (b) 3 l/min air plasma-treated surface, (c) 10 l/min air plasma-treated surface, and (d) 3 l/min Ar plasma-treated surface, at a treatment time of 1 min and a nozzle-to-sample distance of 1 mm. (e) Comparison between chemical compositions of the plasma-treated surfaces. Fig. 8. XPS spectra of O 1s regions of (a) 3 l/min air plasma-treated surface, (b) 10 l/min air plasma-treated surface, and (c) 3 l/min Ar plasma-treated surface, at a nozzle-to-sample distance of 1 mm. (d) Comparison between the ratios of O=C to O−C of the plasma-treated surfaces. Fig. 9. SEM images of PP film surfaces treated with 3 and 10 l/min air plasma jets and with 3 l/min Ar plasma jet at a nozzle-to-sample distance of 1 mm. Fig. 10. Temperatures of PP film surfaces treated with air and Ar plasma jets, as a function of treatment time.
- Data for: Study on properties of anti-reflective and superhydrophobic films prepared by magical solThe raw data of Transmittance and superhydrophobicity.
- Data for: Enhanced bioactive and osteogenic activities of titanium by modification with phytic acid and calcium hydroxideTest results of basic physical properties of materials
- Data for: The adsorption performance of tetracyclines on magnetic graphene oxide: A novel antibiotics absorbentcounting process
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