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Jsm 6300f

Manufactured by JEOL
Sourced in Japan, United States

The JSM-6300F is a scanning electron microscope (SEM) manufactured by JEOL. The core function of this instrument is to provide high-resolution imaging of samples by scanning them with a focused electron beam.

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18 protocols using jsm 6300f

1

Scanning Electron Microscopy of HA Hydrogels

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The micromorphology of HA hydrogels (HA) and hESC-MSC/HA hydrogel composite (HA/hESC-MSC) were observed by SEM assay with an accelerating voltage of 5 kV as recently reported [44 (link)]. Briefly, samples were washed with 1 × PBS, fixed in 4% paraformaldehyde (Sigma-Aldrich, St Louis, USA) for 2 h and thereafter in 1% OsO4 for 2 h. Then, they were progressively dehydrated in a series of alcohols after rewashing with 1 × PBS, vacuum-dried, and coated with gold for observation and photograph with the Scanning electron microscope (JEOL JSM-6300F, USA).
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2

Scanning Electron Microscopy Techniques

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SEM measurements were performed with a field emission microscope JSM-6300F (JEOL, Tokyo, Japan). The energy of the exciting electrons was mostly 5 keV. Beside the detector for secondary electrons (SEI), Everhart-Thornley type, the system is equipped with different detector types (semiconductor and YAG type) for backscattered electrons.
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3

Characterization and Compressive Analysis of Porous Aluminum Composites

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The characteristics of the cross-sectioned surface of the developed Al foam composite were examined using a scanning electron microscope (SEM) and electron dispersive X-ray (EDX). The surface morphology, topography, and elemental composition associated with the matrix and reinforcement reaction were observed. The SEM result using the JEOL JSM-6300F (Tokyo, Japan) was used to determine the nature of particle distribution, particle size variation, and surface morphology of the Al foam composite samples. Archimedes’ principle was applied to measure the porosity and density of porous samples. Uniaxially compressive tests were performed on porous composite samples with a crosshead speed of 0.5 mm/min at room temperature and load cell of 30 kN (Dartec model 3500 universal testing machine). For the compressive response analysis, the average of three samples was determined. The area under the stress–strain curves determined the energy absorption capacity (W) of the resulting porous Al composites using the following equation [46 (link)]: W=0εσ dε
where σ and ε are the compression stress and strain, respectively.
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4

SEM Analysis of Particle Dispersions

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SEM measurements were performed with a field emission microscope JSM-6300F (JEOL, Tokyo, Japan). The energy of the exciting electrons was mostly 5 keV. Beside the detector for secondary electrons (SEI), Everhart-Thornley type, the system is equipped with different detector types (semiconductor and YAG type) for backscattered electrons. The sample preparation was done by the deposition of 10 µL droplets of the particle dispersion on polished amorphous carbon substrates (sigradur) and dried in air. Because of the low atomic number of carbon this strategy helps to increase the imaging contrast.
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5

Quantifying Corneal Stromal Surface Roughness

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The corneoscleral buttons were then dissected and the flap gently cut off. The specimens were fixed in formaldehyde 10% and processed for scanning electron microscopy (SEM). Briefly, washing in BSS for 5 minutes was followed by dehydration in ascending concentrations of ethanol (25%, 50%, 75% and 100%, ten minutes each), followed by infiltration with three changes of hexamethyldisilazane (HMDS) each lasting for 10 minutes. The samples were allowed to slowly air-dry overnight. They were then coated with 20 nm of gold by resistive thermal evaporation and examined (JEOL JSM-6300F, Tokyo, Japan) at 5 kV and 10 mm working distance. SEM photos were taken at 1000× magnification, at three different locations within the ablated bed.
Smoothness of the ablated bed was then evaluated based on the texture analysis of the SEM images [2] (link). Image texture, defined as variations in the pixel intensities (variations in the gray-levels), was analyzed using the Haralick texture contrast parameter [25] . The usefulness of this parameter has been well documented in biomedical sciences [26] (link), and more specifically, for the quantification of corneal stromal surface roughness as observed on a SEM image [27] (link). The Haralick contrast parameter was computed for each SEM image (Matlab R2009b version). Haralick contrast values increase with roughness.
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6

Scanning Electron Microscopy of Kafirin Microparticles

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The freeze-dried kafirin microparticle samples were mounted onto carbon tabs and coated with 10 nm of platinum using a sputter coater (Baltec MED 020, Leica Microsystems, Wetzlar, Germany). The samples were then viewed at 5 kV and a working distance of 8 mm using a field emission scanning electron microscope JSM 6300F (JEOL, Tokyo, Japan) [4 (link),23 (link),25 (link)].
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7

SEM Analysis of Invertase-Onion Membranes

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A scanning electron microscope (Model JEOL JSM-6300 F, Tokyo, Japan; 2–5 kV with Auto Fine Coater, JEOL-JFC-1600E Ion Sputtering Device) was used to study modified invertase-onion membranes. During SEM analysis, onion membrane(s) were mounted on stubs and coated with Au/Pd. SEM micrographs of both the invertase immobilized and those that were blank were taken at various magnifications.
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8

SEM Analysis of RNG Particles

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SEM measurements of the RNG were performed with a field emission microscope JSM-6300F (JEOL, Tokyo, Japan). The energy of the exciting electrons was mostly 5 keV. Beside the detector for secondary electrons (SEI) the system is equipped with different detector types (semiconductor and YAG type) for backscattered electrons. The sample preparation was done by the deposition of 10 μL droplets of the particle dispersion on polished amorphous carbon substrates (sigradur) and dried in air. Because of the low atomic number of carbon this strategy helps to increase the imaging contrast.
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9

SEM Imaging with Enhanced Topography

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SEM measurements were performed with a field emission microscope JSM-6300F (JEOL, Tokyo, Japan) and FEI Helios NanoLab G3 UC (ThermoFisher, Nederland). The energy of the exciting electrons was mostly 5 keV. In order to enhance the surface sensitivity and in this manner the topographical impression some of the micrographs were taken at a stage tilt of 45°. Besides the detector for secondary electrons (SEI), Everhart-Thornley type, the system is equipped with different detector types (semiconductor and YAG type) for backscattered electrons.
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10

Electrochemical Analysis of Biological Samples

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All the electrochemical measurements (the square wave voltammetry (SWV) and cyclic voltammetry (CV)) were performed by a multichannel AUTOLAB potentiostat PGSTAT302N obtained from Metrohm, Netherlands. The potentiostat was connected to a personnel computer and operated by the Nova 1.11 software. Dual screen-printed carbon electrodes (C1110) were purchased from Metrohm DropSens. (Spain). Each electrode includes a silver reference electrode, one carbon counter electrode and two elliptic carbon working electrodes. The electrodes were connected to the potentiostat via a specific connector purchased from Metrohm DropSens and are capable of detecting two signals simultaneously, allowing (differential) measurements of two samples (the control and the patient samples). Scanning electron microscopy images were taken using JEOL JSM-6300F at a working distance of 4.8 mm with an acceleration voltage of 5 kV, and magnification = 50,000×.
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