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Dimension 5

Manufactured by Veeco
Sourced in United States

The Dimension V is a precision scanning probe microscope (SPM) designed for advanced materials characterization. It provides high-resolution imaging and metrology capabilities for a wide range of applications. The core function of the Dimension V is to enable users to acquire detailed topographical and nanoscale data on a variety of samples.

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10 protocols using dimension 5

1

Characterization of EG/PANI Composite Materials

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The morphologies of the materials were characterized by scanning electron microscopy (SEM) on a ZEISS Sigma 300. The thickness of the EG was determined using an atomic force microscope (AFM) on a Veeco dimension V. X-ray photoelectron spectroscopy (XPS) was conducted on a Thermo Scientific K-Alpha instrument (Waltham, MA, USA) to analyze the nitrogen and carbon atoms within the EG and the EG/PANI composite. The XPS peak-fitting program XPSPEAK 4.1 was used for the spectra processing. Raman spectra were obtained with a Raman system (Renishaw, UK) using a 514.5 nm laser as the light source to characterize the EG. X-ray diffraction (XRD) measurements were examined using a Smart lab 9 kW with Cu-Kα radiation (λ = 0.15406 nm) to analyze the crystal structure of EG. Fourier-transform infrared (FTIR) spectroscopy was performed on a Thermo Scientific Nicolet iS20 instrument to confirm the structure of the EG/PANI composite.
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2

Characterization of Graphene and Diamond Thin Films

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The surface morphology of the various films measured over 10 μm × 10 μm and 1 μm × 1 μm regions was measured using scanning atomic force microscopy (AFM, Veeco Dimension V) in tapping mode for the H-terminated NDs. The chemical composition and bonding states of the films were characterized using Fourier transfer infrared spectrometry (FTIR, Perkin Elmer Spectrum One) in transmission mode and X-ray photoelectron spectroscopy (XPS, Thermo Scientific) with the Al K α line as the exciting source. A micro Raman spectroscopy system (Renishaw Invia) operating at 514.5 nm was used to study the film microstructure, where the laser output power used was 1 mW. Impedance spectroscopy was applied in the range of 0.1 Hz to 10 MHz in a vacuum at elevated temperature from room temperature to 500 C using an Autolab electrochemical system. Hall Effect measurements (1T electromagnet, Lakeshore Cryogenics System) were performed to determine graphene carrier mobilities using the “van der Pauw” method, where by four Ohmic metal contacts (10 nm Ti-300 nm Au) were placed on the topside of the graphene layers at room temperature.
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3

Copolymer Film Surface Roughness Analysis

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The surface roughness of the copolymer films was determined using a Dimension V (Veeco Instruments, USA) atomic force microscope (AFM). Surface roughness is reported as root mean square (Rq) values which was determined using the inbuilt function in the NanoScope software (Version 1.20).
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4

Structural and Transport Characterization

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The θ–2θ diffraction data measurements are done on a Bruker D8 Discover diffractometer CuKα1 (λ = 1.54 Å). Temperature-dependent electrical transport measurements are carried out in Physical Property Measurement system (Quantum Design) utilizing a four probe geometry. The surface morphology analysis of the various films are characterized on an atomic force microscope (AFM, Dimension V, Veeco).
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5

Selective Al Deposition on Graphene Cantilever Film

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An e-beam evaporation system (Anelva L-400EK) was used to deposit the Al nanofilm (10 nm thick at 0.5 Å/s) on GCF through a shadow mask to avoid depositing Al on suspending CNTs. The thickness was measured in situ by using a quartz crystal sensor, which was calibrated by using an atomic force microscope (AFM; Veeco Dimension V). According to Tavernarakis et al. (40 (link)), if CNT is decorated by metal nanoparticles, it might be visible in an optical microscope. However, the CNT suspension thread of the torsion balance is invisible in optical microscope. There might be some Al deposition on the part adjacent to GCF, but the other parts of suspended CNT are free of Al deposition according to the scanning electron microscopy (SEM) images.
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6

Atomic Force Microscopy of TCPS and Glass

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Atomic force microscopy (AFM) measurements were carried out using a Veeco Dimension V instrument with aluminum-coated silicon AFM probes (resonant frequency 190 kHz). The system was operated in tapping mode with a VT-103-3K acoustic/vibration isolation system and a VT-102 vibration isolation table at room temperature in air. AFM was performed on Tissue Culture Polystyrene (TCPS) (Costar 3527, Corning, 24 well plate), glass H–ND monolayers. Scan sizes of 2 μm were taken and root mean square of the roughness (Rq) was calculated using Nanoscope Software 6.1.3. AFM Images were post processed with a median filter (3 × 3 kernel) using MATLAB 2012a software to remove noise and measurement artifacts.
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7

Characterization of Thin Layers using Light Microscopy and AFM

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Light microscopy was used to investigate the morphologies of obtained layers. For this purpose, we used IX71 (Olympus, Shinjuku, Japan) microscope operating in reflection mode and the Dimension V (Veeco, Plainview, New York, NY, USA) atomic force microscope (AFM) operating in tapping mode. The first technique was used to determine morphological changes at the micrometer-scale level. It provided a fast and rough estimation of samples morphologies. The insight into the morphology at the nanoscale level was assured by AFM microscopy. This technique allowed us to obtain images of high resolution, up to several nanometers; however, this technique is relatively slow and prone to distortions if scanning is fast and height amplitudes are significant. Both techniques are complementary to the research described in this article.
The thicknesses of layers were determined at the end of all measurements using a Dektak 3 (Veeco, Plainview, New York, NY, USA) profilometer. In this case, central regions of layers were removed using a scalpel to expose the surfaces of glass slides, and then the profilometer measured the depth of such a formed scratch.
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8

Detecting Prostate Microparticles by AFM

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To detect prostate microparticles in patient plasma samples, anti-PSMA mouse IgG2b-PE (clone 3/E7) was added to 20μL of patient plasma. Negative isotype stained controls consisted of mouse isotype control IgG2b-PE (Beckman Coutler Inc.) added to 20μL of patient plasma. Gates for each microparticle population were established by analyzing the isotype control first, modifying the gains for each PMT as necessary, and then analyzing the antibody labeled samples.
For microparticles generated in vitro, these were isolated by FACS as previously described in [12 (link)], in which PSMA+ve and zsGreen+ve co-expressing microparticle events were sorted onto cleaved mica coverslips (Ted Pella Inc. Redding, CA) to isolate prostate microparticles whilst eliminating non-target EVs and serum protein. After sorting 1000-3000 events onto the mica coverslips, samples were allowed to dry in 50 mL Falcon tubes for 5 minutes at 70°C before imaging with atomic force microscopy (AFM). No washing of the samples was performed. Images were acquired with tapping mode AFM (Dimension V, Veeco Inc.). Rectangle cantilevers with nominal spring constant of 40 N/m and tip radius of < 10 nm were used to acquire high resolution topographic images. All measurements were done at low driving force to avoid damaging samples.
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9

Characterization of Bi2O2CO3 Catalyst

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The X-ray diffraction patterns of the samples were carried out on the Bruker X-ray diffractometer (XRD, D8 Advance) using Cu Kα. An Autosorb-iQA3200-4 sorption analyzer (Quantatech Co., USA) based on N2 adsorption/desorption was used to measure the Brunauer–Emmett–Teller specific (BET) surface area. The surface morphology and thickness of the Bi2O2CO3 samples were examined with a field emission scanning electron microscope (FESEM, Hitachi S4800), transmission electron microscope (TEM, JEM-2100F), and atomic force microscope (AFM, Dimension V, Veeco). The surface chemical valences of the Bi2O2CO3 catalyst were analysed with an ESCALAB 250 X-ray photoelectron spectroscope (XPS). The UV-visible diffuse reflectance spectra were measured with a Hitachi UV-3310. The photoluminescence (PL) spectra were collected on a Hitachi F4600 fluorescence spectrophotometer, using a Xe lamp (excitation at 365 nm) as the light source.
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10

Electrospun PEUU/Dacron Fiber Characterization

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PEUU or Dacron fibers were electrospun over a TGZ3 calibration grating (NT-MDT, Moscow, Russia ) and imaged by AFM (Dimension V, Veeco, Santa Barbara, CA) in tapping mode with a k=61N/m ACL cantilever (AppNano, Mountain View, Ca) to assess the dimensions of the suspended fibers. To precisely evaluate the applied load, the cantilever spring constant was measured using the vibration resonance method incorporated in the AFM proprietary software. Force-distance curves were performed on each imaged fiber as described in [40 ], in a regimen of small deflections. Curves were then converted to force-displacement and the curves at the middle point of the channels were averaged for comparison with the FEM simulations.
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