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Agilent 5500 afm

Manufactured by Agilent Technologies
Sourced in United States

The Agilent 5500 AFM is an atomic force microscope designed for high-resolution imaging and analysis of surface topography at the nanoscale level. It utilizes a sharp probe tip to scan the surface of a sample, providing detailed information about the sample's physical and chemical properties.

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18 protocols using agilent 5500 afm

1

Surface Morphology of PLA-C Films

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Morphology of surface of PLA-C films casted on PTFE, glass, and silicone disks was evaluated by using an atomic force microscope (AFM) (Agilent AFM 5500, Agilent Technologies, California, CA, USA) operating at room temperature. Rectangular silicon cantilevers used have a nominal spring constant of 0.2 N m−1 (ESPA-V2/Sb doped Si, Bruker, Billerica, MA, USA).
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2

Characterization of Cr8O21 Powder and Electrodes

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Powder X-ray diffraction (XRD, Rigaku M2400, Rigaku Co., Tokyo, Japan) was used to characterize the crystal structure of the Cr8O21 powder with Cu Kα radiation. Scanning electron microscope (SEM, S-4800, Hitachi Inc., Tokyo, Japan) and transmission electron microscope (TEM, Philips Tecnai G2 F20, FEI Co., Hillsboro, OR, USA) were used to characterize the morphology and microstructure of both the powder and the electrodes. X-ray photoelectron spectroscopy (XPS, Axis Ultra DLD, Shimadzu-Kratos Co. Ltd., Kanagawa, Japan) was used to derive information on the bonding state of the samples. Fourier transform infrared spectroscopy (FTIR, Nicolet 6700, Thermo Fisher, Waltham, MA, USA) was used to characterize the change of PEO-based membrane. Surface profiler (P-l6+, KLA-Tencor, Milpitas, CA, USA) and atomic force microscope (AFM, Agilent AFM5500, Agilent Technologies, Inc., Santa Clara, CA, USA) in tapping mode at 512 Hz were used to calibrate the thickness of 100-ALD-Al2O3 coated on a silicon plate.
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3

Topographical Analysis of PLA Films

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Surface topography of the PLA films was evaluated using an atomic force microscope (AFM) (Agilent AFM 5500, Agilent Technologies, California, CA, USA) operating at room temperature and in contact mode. Rectangular cantilevers (FMV-PT, Bruker, Billerica, MA, USA) were used with a nominal spring constant of 75 kHz and a force constant of 2.8 N/m. Images were taken for two scanning lengths (50 × 50 μm2 and 25 × 25 μm2) and in each scanning area, topographical, deflection and friction images were acquired. Experiments were performed in triplicate, studying three different films for each condition. Roughness is a scale-dependent function and therefore all comparisons were made with the mean roughness parameter (Sa) always obtained from 50 × 50 μm2 images. Results are presented as mean values and standard deviations.
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4

Characterizing Passive Films by CSAFM and XPS

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CSAFM measurements of passive films before and after hydrogen charging were performed using Agilent 5500 AFM (Agilent Technologies, USA) with the current sensing mode. In addition to the current maps measured by CSAFM, current-voltage curves were acquired by setting the probe tip in contact with the passive films at different locations in ferrite and austenite phases of the current maps, which were done at least 10 times at different locations of the specimen and representative curves were picked out. The equipment was located in a clean room at a constant temperature of 25 °C and relative humidity of about 25%. The probes used in MFM measurements were Bruker magnetic probes (MESP) with force constant of 2.8 N/m, while the probes in CSAFM measurements were AppNano conductive Pt-coated silicon tips with a force constant of 2.8 N/m and a tip radius of 40 nm.
The chemical composition of the passive films formed before and after hydrogen charging was investigated with XPS with a monochromatic Al Ka radiation source and a pass energy of 25 eV. The depth profiling was performed using an Ar+ gun with a beam energy of 3 kV and a beam current of 1 μA. The curve fitting was performed using the commercial software XPS Peak, version 4.1, which contains the Shirley background subtraction and Gaussian-Lorentzian tail functions, to achieve better spectra fitting.
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5

Characterization of DBM Nanoparticles

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Following synthesis of the DBM nanoparticles, the nanoparticles were characterized through several experiments to confirm their size, shape, surface, and morphological features. The shape and surface morphology of the DBM nanoparticles was determined using atomic force microscopy (AFM). DBM nanoparticles were suspended in distilled water, then a drop of suspension was placed on the glass coverslip, air-dried, and scanned using AFM (Agilent 5500 AFM, USA). Also, the ultra-structural nature and morphological distinctiveness of DBM nanoparticles have been investigated and confirmed using field emission scanning electron microscopy (FESEM) Philips JSM- 6360LA instrument (Philips, Eindhoven, Netherlands).
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6

Intermittent AFM Imaging with Silicon Tips

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Intermittent contact mode images were obtained using an Agilent (5500) AFM with silicon tips (Budget Sensors).
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7

Morphological Characterization of tHCR and gHCR

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Morphological characterization of assembly and disassembly of tHCR and gHCR was carried out using AFM. Ten-microliter samples (1:1 diluted by 20 mM magnesium chloride) were spread onto a freshly cleaved mica slice, followed by 30-s incubation at room temperature (RT). The mica slice was then washed with double-distilled water and dried with nitrogen immediately following AFM imaging. All AFM images were acquired using an Agilent 5500 AFM (Agilent Technologies) in tapping mode. NSC-15/Al BS tips with a nominal spring constant of 40 N m−1 and a resonant frequency of approximately 325 kHz were used.
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8

Comprehensive Characterization of Nanomaterials

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The X-ray diffraction patterns were recorded on a Bruker D8 Advance X-ray diffractometer with Ni filtered Cu Kα radiation at 40 kV and 40 mA. Ultraviolet–visible diffuse reflectance (ultraviolet–visible diffuse reflectance spectrum) spectra were obtained with a self-supporting sample disk on a ultraviolet–visible spectrophotometer (Cary 500), where BaSO4 was used as a reflectance standard. TEM images were obtained using a JEOL model JEM 2010 EX instrument at an accelerating voltage of 200 kV. AFM images were recorded using Agilent 5,500 AFM (Agilent Technologies, USA). All the images were acquired using tapping mode under ambient conditions (ca. 40−50% relative humidity, 25 °C temperature). The used Si cantilevers/tips (Bruker) have a spring constant of 40 N m−1 and a resonance frequency of 300 kHz. During an AFM experiment, sample was dispersed in ethanol using an ultrasonic bath for 20 min and then the dispersion was diluted in ethanol. A drop of the above diluted dispersion was deposited on a new cleaved mica surface and dried in air. The instrument parameters (set point, amplitude, scan size, scan speed and feedback control) were adjusted for the best resolution of images. Electron spin resonance spectra were obtained over Bruker ESP 300 E electron paramagnetic resonance spectrometer.
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9

Atomic Force Microscopy of Surfaces

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AFM measurements were carried out in a tapping mode on the Agilent 5500 AFM (USA) and NTEGRA Prima AFM (NT-MDT, Russia) in air using standard probes PPP-NCH (Nanosensors, Switzerland) with the force constant about 42 Nm−1 and the radius of curvature 10 nm. Scan rate was 1 Hz. At least ten frames of 1÷25 μm2 were obtained in each experiment.
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10

Nanostructure Characterization via AFM Imaging

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The dried samples were prepared by depositing three droplets of sample solution on the freshly cleaved mica surface and dried via different methods, as depicted in Figure 1. The morphologies of nanostructures on mica were imaged using an Agilent 5500 AFM (Agilent Technologies) with a multipurpose XYZ closed-loop scanner. Rotated monolithic silicon probes with aluminum reflex coating (BudgetSensors, Tap-300G, resonance frequency ∼300 kHz, tip radius of curvature <10 nm, force constant 40 N/m) were used to record topographic, amplitude, and phase images with 512 × 512 pixel resolution. Imaging under dry conditions allowed us to achieve high resolution in the Z dimension and observe one peptide thick protofibrils. Gwyddion and ImageJ packages were used to analyze the AFM results. Quantitative analysis methods are provided in the Supporting Information.
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