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21 protocols using auriga fib sem

1

Morphology of RIT-SM Solid Dispersions

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Scanning electron micrographs were obtained to determine the morphology of RIT-SM solid dispersions. Samples, including pure RIT, pure RIT plus powdered SM (RIT-SM mixture), freeze-dried RIT-SM 0.1, 300 and 500 systems and freeze-dried RIT previously dispersed in ethanol (RIT-EtOH), were placed on the cover slides using double sticky copper tape prior to imaging. Subsequently, samples were imaged with a Zeiss Auriga FIB-SEM using a secondary electron detector (SE2). Parameters were 0.5 kV accelerating voltage and ~2–4 mm working distance. Magnifications were 300 – 60,000 X. The SEM images were processed using ImageJ (Ver Java 1.6.0_20, National Institutes of Health).
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2

Comprehensive Characterization of PAAS Photonic Film

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The surface and cross-section morphologies of the PAAS photonic film were taken using the SEM (Carl Zeiss Auriga FIB-SEM) with an acceleration voltage of 5 kV. An image processing software (ImageJ) was utilized to analyze those SEM images for the size distribution of PAAS film. The TGA curves were characterized from 20 °C to 300 °C with a temperature scanning rate of 5 °C min−1 by Bruker TG 50. DSC analysis was carried out on a TA Instruments SDT Q600 from 18 °C to 350 °C under a heating rate of 5 °C min−1. A thermal camera (FLIR C5) was used to take infrared images. An ellipsometer (J.A. Woolam, M200DI) was employed to extract the complex refractive indices of PAAS. The hardness of the PAAS sample was examined by the VTSYIQI Shore D durometer. The tensile strength was performed with the upper fixture moving downward at a constant velocity of 5 mm min−1. The thermal conductivity of the PAAS film was characterized by Hot Disk TPS 2500 s.
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3

Microscopic Structural Analysis of TMD Composites

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Transmission electron microscope (TEM) images were digitally acquired by the use of a Phillips CM100 operated at 100 kV. Raman spectroscopy was performed by a Horiba Jobin Yvon LabRam ARAMIS confocal Raman microscope using a He-Ne laser (approx. 632.8 nm). Energy dispersive spectra (EDS) were collected using a Zeiss Gemini scanning electron microscope (SEM) at 10–30 keV. To observe the layered electrode morphology cross-section, a focused Ga+ ion beam (Zeiss Auriga FIB-SEM) was used to cut notches at the edges of the exfoliated TMD composite structures.
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4

3D Cell Culture Histological Analysis

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After culturing cells for 7 and 14 days, the 3D culture samples were removed from the culture chambers and fixed with 4% PFA. Fixed samples were not decalcified and sent to the Histology Core Facility at the New Jersey Medical School of Rutgers University for paraffin embedding and sectioning. The samples were cut into histological sections of 10-μm thick. Sections were stained with hematoxylin and eosin (H&E, Sigma-Aldrich) and 4′,6-diamidino-2-phenylindole (DAPI, Sigma-Aldrich) to examine cell distribution under a fluorescent microscope (Nikon Ti). Parallel samples were used for sclerostin and ALP immunostainings as described above. Some of the samples were dehydrated in sequential ethanol solutions with increasing concentrations from 50% to 100% with gold-coating and directly visualized under a scanning electron microscope (SEM, Zeiss Auriga FIB-SEM, CA, USA).
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5

Atom-Probe Analysis of Oxygen-Rich Clusters

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The same atom-probe data sets as reported in ref. 33 were utilized for the calculation of GB excess using ‘cylinder method'. Briefly, atom-probe specimens were prepared inside a Zeiss Auriga FIB/SEM by a lift-out approach51 (link). Atom-probe data were acquired using a Cameca LEAP 4000X Si operated in voltage-pulsing mode at 40 K, with pulsing voltage being 20% of d.c. bias voltage, and evaporation rate kept at 1% of the pulsing rate of 200 kHz (ref. 33 ). Data reconstruction and visualization were performed using IVAS software (Cameca). O+, AlO+ and minor amount of O2+, O2+, AlO2+, AlO2+ and AlO22+ were identified in the mass spectrum as O-containing species. Analysis of O-rich clusters was facilitated by means of Voronoi volume distribution through custom MATLAB (Mathworks Inc.) programs.52 (link)
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6

Characterization of CuO@MnO2 Composites

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The crystallography and chemical composition of the as-prepared products were investigated by powder X-ray diffraction (XRD, D/max 1200, Cu K) and Fourier transform infrared spectroscopy (FTIR, Nicolet 5DXC). The morphologies of the CuO@MnO2 composites were observed with focused ion beam (Zeiss Auriga FIB/SEM). Microstructures were characterized by transmission electron microscopy (TEM), high-resolution TEM, and energy-dispersive x-ray spectroscopy (EDS) using JEOL JEM-2010F electron microscope operated at 200 kV. The nitrogen adsorption-desorption isotherms were measured at 77 K using micrometritics ASAP 2020 sorptometer. Specific surface area was determined with Brunauer-Emmett-Teller (BET) equation, and the distribution of pore size was calculated from the adsorption curve by the Barrett–Joyner–Halenda (BJH) method.
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7

Characterization of Plasmonic AuNFs

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TEM images were obtained with an FEI Titan Themis 200 TEM at an acceleration voltage of 200 kV. SEM images were obtained a Zeiss Auriga FIB-SEM. UV–vis–NIR absorption spectra were performed with a Shimadzu UV-3600 spectrophotometer. Using Beer’s law (A/L = αC), the AuNFs’ extinction coefficient was extracted from the slope of a plot of A/L versus concentration (C). The optical extinction per cell length (A/L) was determined from the optical extinction intensity at 1064 nm. The size, polydispersity index, and zeta potential of nanoparticles were determined by dynamic light scattering (Zetasizer 3000HS; Malvern Instruments, Worcestershire, UK). FTIR spectra were recorded in a range of 400–4000 cm−1 at a 0.5–4 cm−1 resolution with a Bruker Vertex 80v vacuum FTIR spectrometer. A 1064 nm multimode pump laser (Shanghai Connect Fiber Optics Co. Ltd.) was used as the irradiation source for NIR-II photothermal effect. For in vitro PAT, HA-4-ATP-AuNFs at different concentrations (0, 0.1, 0.2, 0.4, 0.8, and 1 mg mL−1) were added into 200 μL tubes for PA signal detection using a PA instrument (VisualSonics Vevo 2100 LAZR systems) with an excitation wavelength of 1200 nm.
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8

Microstructural Analysis of Tissue-Engineered Scaffolds

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BMSC/Mb, ADSC/Mb, or C2C12 were seeded on PCL-collagen I-nanoscaffolds at a density of 3 × 105 cells and allowed to proliferate for 7 days bevor differentiation was induced with standard differentiation medium for 28 days. Microstructural analysis of the seeded scaffolds was performed using an Auriga Fib-SEM (Zeiss, Oberkochen, Germany) as described previously [8 (link), 21 (link)]. Probes were sputter-coated with gold for 1 min using an EMITECH-K550 sputter coater at an operating pressure of 7 × 102 bar and a deposition current of 20 mA.
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9

Comprehensive Characterization of Prepared Materials

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X-ray photoelectron spectroscopy (Kratos XSAM800, XPS), the powder X-ray diffraction (D/max 2500, Cu Kα, XRD) and thermosgravimetric analyzer-differential scanning calorimeter (NETZSCH STA 449C, TGA-DSC) were used to characterize the crystallinity and components of prepared materials. Morphological structure was analyzed by scanning electron microscopy (Zeiss Auriga FIB/SEM). The detailed structures of the materials were collected by transmission electron microscopy (FEI TECNAI G2 F20, TEM).
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10

Structural and Compositional Analysis of NiMgAl LDHs

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The crystallographic structure and phase composition of as-obtained samples were analyzed by the Rigaku D/max-2500 XRD using a Cu Kα radiation source (λ = 1.5406 Å). The morphological investigations of these samples were conducted by focused ion beam (Zeiss Auriga FIB/SEM) equipped with an energy dispersive X-ray spectrometer (EDS) attachment with an acceleration voltage of 5 kV. The lattice information on nanoscale was collected by high-resolution transmission electron microscopy (HRTEM, Zeiss Libra 200) with an acceleration voltage of 200 kV. Specific surface area and porosity of NiMgAl LDHs were determined by N2 adsorption–desorption isotherms at 77 K using micromeritics Gemini VII. The information of chemical states was analyzed by the Thermo ESCALAB 250Xi X-ray photoelectron spectrometer (Al Kα, 1486.6 eV) at the scope range from 0 to 1350 eV.
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