Method for characterizing stability of nano material
A technology of nanomaterials and stability, which is applied in the field of characterizing the stability of nanomaterials, can solve problems such as limited application of insulators and semiconductor surfaces, damage of sample surfaces and probes, and generation of transverse shear force, etc., to achieve intuitive and easy-to-use characterization results Good control and stability
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Embodiment 1
[0052] (1) The prepared reduced graphene oxide is placed in a beaker equipped with absolute ethanol, and after ultrasonic dispersion, pipette the dispersed suspension and drop it on a silicon wafer (silicon single-sided polished wafer), at room temperature Dry naturally to obtain the nanomaterial to be tested;
[0053] (2) The nanomaterial to be measured obtained in step (1) is fixed on the sample stage of the AFM, and the above-mentioned fixed is tapped with the peak force of the AFM probe in the tapping mode (cantilever resonance frequency is 2kHz) under atmospheric and room temperature conditions. The sample is scanned in situ to obtain its topography; the peak force is constant at 0.33nN, the scanning range is 5μm×5μm, and the scanning rate is 1.98Hz. The results are as follows: figure 1 , where a-e are the graphene topography observed by in-situ AFM, and f corresponds to the topography height change at the position of the white line in picture e;
[0054] (3) analyze the...
Embodiment 2
[0059] (1) The prepared two-dimensional V 2 The C MXene material was placed in a beaker filled with absolute ethanol, and after ultrasonic dispersion, the dispersed suspension was pipetted with a dropper and dropped onto a silicon wafer (silicon single-sided polished wafer), and dried naturally at room temperature to obtain the nanometer to be tested. Material;
[0060] (2) The nanomaterial to be measured obtained in step (1) is fixed on the sample stage of the AFM, and the above-mentioned fixed is tapped with the peak force of the AFM probe in the tapping mode (cantilever resonance frequency is 2kHz) under atmospheric and room temperature conditions. The sample is scanned in situ to obtain its topography; the peak force is constant at 0.26nN, the scanning range is 5μm×5μm, and the scanning rate is 1.98Hz. A topography map is obtained every 4 minutes and 19 seconds. The results are as follows figure 2 , where a-k are the two-dimensional material V observed by in-situ AFM 2 ...
Embodiment 3
[0066] (1) The prepared two-dimensional V 2 The C MXene material was placed in a beaker filled with absolute ethanol, and after ultrasonic dispersion, the dispersed suspension was pipetted with a dropper and dropped onto a silicon wafer (silicon single-sided polished wafer), and dried naturally at room temperature to obtain the nanometer to be tested. Material;
[0067] (2) The nanomaterial to be measured obtained in step (1) is fixed on the sample stage of the AFM, and the above-mentioned fixed is tapped with the peak force of the AFM probe in the tapping mode (cantilever resonance frequency is 2kHz) under atmospheric and room temperature conditions. Scan the sample in situ to obtain its topography; first keep the peak force at 0.26nN constant, observe in situ for a period of time, then increase the peak force to 1.33nN, and continue to observe the same area in situ; scanning range 5μm× 5μm, scan rate 1.98Hz, acquire a topography map every 12 minutes and 57 seconds, the resu...
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