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45 protocols using avizo 9

1

3D Visualization and Quantification of Dopamine Neurons

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Color-coded depth projections of 3D images were created via ImageJ. Blinking signal in Fig. 2d was rendered in Imaris (Bitplane). We further used the Volume Rendering tool in Avizo 9.4 (Thermo Fisher Scientific Inc) for 3D visualization of whole brain dopamine neurons (Fig. 5). For single neuron segmentation, as depicted in Fig. 5, we used the Brush tool in the segmentation mode of Avizo 9.4 (Thermo Fisher Scientific Inc) to manually select the boundary of each single neuron to generate a single neuron boundary mask. We further used the arithmetic tool to intersect the original data with the manually segmented single neuron mask to generate single neuron images with the original gray scale. In Figs. 5d and 6, we used the Material Statistics module in Avizo 9.4 (Thermo Fisher Scientific Inc) to quantify the volume of the MB sectors, DPM neurons, and VMAT protein expression. This module calculates the voxel numbers inside a labeled area, which can be transformed into volumes by multiplying with a known voxel size in each image. We manually segmented the boundaries of the MB sectors using the Lasso tool in segmentation mode. We used the Magic Wand tool to select one seed within the DPM neuron and to determine a reasonable threshold for selecting the connecting voxels. We directly used the Threshold tool for whole-volume VMAT images, setting the lower bound to 78 (8-bit; 0-255).
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2

Quantitative 3D Image Analysis of Bone Regeneration

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Thermo Scientific Avizo 9.5 software (Huston, TX, USA) was used to filter, segment, and quantify all phases present in the image: new bone, biomaterial, connective tissue (CT), and background. Before segmentation, a non-local means filter was applied in order to reduce the reconstruction artifacts and facilitate targeting [34 (link)]. The attenuation of the X-ray beam when passed through the sample, depending on the density of each sample structure, resulted in differentiation in the grayscale images. Thus, we obtained different grayscale ranges for resident bone together with the newly formed bone, the biomaterial, the connective tissue, and the background.
The background was removed with an interactive threshold tool. In the first segmentation step, a quick segmentation was performed by single thresholding to create seeds attributed to each phase present in the image. The previously created seeds were the input for the fine-tuned watershed-based segmentation of the bone and biomaterial phases [35 (link)]. A Lasso 3D tool masked the new bone region located in the defect cavity, separating it from the pre-existing bone. CT was segmented using a magic wand tool, masking the corresponding threshold range. After the segmentation, all phases (pre-existing bone, new bone, biomaterial, and connective tissue) were visualized using Thermo Scientific Avizo 9.5.
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3

Micro-CT Imaging of Didinium Specimen

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Specimen DIP-S-0907 was scanned with a MicroXCT 400 (Carl Zeiss X-ray Microscopy Inc.) at the Institute of Zoology, Chinese Academy of Sciences. The entire animal (Fig. 1) was divided into seven scans that were combined to create a single model, and the scans were conducted with a beam strength of 60 kV, 8 W, and absorption contrast and a spatial resolution of 2.5464 μm. In addition, specimen DIP-S-0907 was imaged using propagation phase-contrast synchrotron radiation microtomography on the beamline 13W at the Shanghai Synchrotron Radiation Facility. The isotropic voxel size was 2.25 μm.
On the basis of the obtained image stacks, structures of the specimen were reconstructed and separated with Amira 5.4 (Visage Imaging). The subsequent volume rendering was performed with Avizo 9.0 (Thermo Fisher Scientific) and VG Studiomax 2.1 (Volume Graphics). The neonate C. ruffus was loaned from the Western Australian Museum (WAM R49553) and scanned with a SkyScan 1076 (Bruker MicroCT) at Adelaide Microscopy, University of Adelaide, Australia. The scan settings were 65 kV, 153 μA, no filter, and an isotropic voxel size of 8.7 μm. The reconstruction was carried out using the software NRecon (Bruker MicroCT), and the volume renderings were created in the software Avizo 9.0 (Thermo Fisher Scientific).
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4

Density Quantification of Fabricated Samples

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To assess the density
of fabricated samples, X-ray microcomputed
tomography (μCT) was performed with a transmission X-ray microscope
(Versa XRM-500, XRADIA). Imaging was performed at 4× magnification
on cylindrical samples of 6 mm diameter and 10 mm height with a total
of 1601 projections per sample. The reconstructed images were analyzed
using Avizo 9.5 software (Thermofischer Scientific). The first sample
fabricated with a lower ED was taken as the reference, and a systematic
procedure was followed for the digital image processing of reconstructed
3D volume for visualizing and quantifying the imperfections.
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5

MicroCT Analysis of Samples

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MicroCT measurements were performed by using a Micro-XCT400 Zeiss (Fig. 3) and Xradia 520 Versa Zeiss (Fig. S1) X-ray microscopes (Peasanton, California, USA). The samples were dried overnight under vacuum. A plastic pipette tip was used as sample container: the narrowest extremity of the pipette tip was melted and sealed using a flame. Subsequently, the dried sample was added to the tip. The tomographic images performed by the Micro-XCT400 Zeiss microscope were obtained by collecting 1200 projections over 180 deg at 40 KV and 200 µA. The final pixel size was 0.33 µm. The tomographic images performed by the Xradia 520 Versa Zeiss microscope were obtained by taking 1601 projections over 360 deg at 45 KV and 67 µA. The final pixel size was 0.613 µm. Collective 3D images of the samples were obtained. Subsequently, detailed analysis of several individual structures were performed by using the Avizo 9.5 software (Thermo Fisher Scientific Inc, USA).
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6

Micro-CT Analysis of Fixed Samples

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Fixed samples were scanned using a micro‐CT (μCT) SCANCO μCT50 scanner (SCANCO Medical AG, Brüttisellen, Switzerland; V1.28) at the University of Southern California Molecular Imaging Center. The μCT images were captured at a resolution of 10 μm under an X‐ray source of 90 kVp and 78 μA. Three‐dimensional reconstruction was done using AVIZO 9.5 software (Thermo Fisher Scientific).
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7

Characterizing MOF Structures via Micro-CT

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The MOFs were separated from the mother liquor by centrifugation and dried overnight under vacuum by a vacuum pump (Edwards RV12). A plastic pipette tip was used as a sample container: the narrowest extremity of the pipette tip was melted and sealed using a flame. Subsequently, the dried crystals were placed into the tip. Micro-CT data of the MOF obtained by the sonochemical–solvothermal crystallization were acquired with a Micro-XCT400 Zeiss X-ray microscope (Peasanton, California, USA). The tomographic images were obtained by taking 1200 projections over 180 deg at 40 KV and 200 µA. The final pixel sizes were 0.33 µm. Micro-CT data of the MOFs obtained by the solvothermal crystallization were acquired with a Xradia 520 Versa Zeiss X-ray microscope. The tomographic images were obtained by taking 2401 projections over 360 deg at 100 KV and 90 µA. The final pixel size was 0.39 µm. 3D images of the samples were collected for all the analyzed systems. Finally, several individual structures were analyzed in detail by using the Avizo 9.5 software (Thermo Fisher Scientific Inc, USA).
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8

Nanoscale 3D Imaging of Porous Materials

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Electron-transparent thin foils were prepared for (scanning) transmission electron microscopy ((S)TEM) by using a FEI Nova Nanolab focused ion beam - scanning electron microscope (FIB-SEM). The FIB-SEM was also used to acquire a slice-and-view series for 3D volume reconstructions. Slice imaging was carried out in backscattered electron mode at 2 kV and 0.84 nA with a voxel size of 8.33×8.33×20 nm³. All FIB-SEM nanotomography volumes were reconstructed and analysed using FEI Avizo 9. Pore channel diameters were obtained by using the cross-correlation diameter obtained via FEI Avizo 9. At the given microscope conditions, we determined a lower boundary limit of the detectable pore size of 50 nm for the analysed nanotomography volumes (Fig. 3B). Electron-transparent FIB foils were investigated in a FEI Talos F200X (S)TEM equipped with four energy-dispersive X-ray detectors (Super-X EDX). The FEI Talos F200X TEM information limit is 0.12 nm. All FIB-SEM and TEM analyses were carried out at the Microscopy Square, Utrecht University.
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9

Nanoscale 3D Imaging of Porous Materials

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Electron-transparent thin foils were prepared for (scanning) transmission electron microscopy ((S)TEM) by using a FEI Nova Nanolab focused ion beam - scanning electron microscope (FIB-SEM). The FIB-SEM was also used to acquire a slice-and-view series for 3D volume reconstructions. Slice imaging was carried out in backscattered electron mode at 2 kV and 0.84 nA with a voxel size of 8.33×8.33×20 nm³. All FIB-SEM nanotomography volumes were reconstructed and analysed using FEI Avizo 9. Pore channel diameters were obtained by using the cross-correlation diameter obtained via FEI Avizo 9. At the given microscope conditions, we determined a lower boundary limit of the detectable pore size of 50 nm for the analysed nanotomography volumes (Fig. 3B). Electron-transparent FIB foils were investigated in a FEI Talos F200X (S)TEM equipped with four energy-dispersive X-ray detectors (Super-X EDX). The FEI Talos F200X TEM information limit is 0.12 nm. All FIB-SEM and TEM analyses were carried out at the Microscopy Square, Utrecht University.
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10

Electron Microscopy for Nanomaterial Analysis

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Electron-transparent thin foils were prepared for (scanning) STEM by using an FEI Helios NanoLab G3 FIB-SEM. The FIB-SEM was also used to acquire several slice-and-view series for 3D volume reconstructions. Slice imaging was carried out in BSE mode at 3 kV and 3.2 nA with a pixel size of 8 × 8 nm2 (voxel size of 8 × 8 × 30 nm3). All FIB-SEM nanotomography volumes were reconstructed and analyzed using FEI Avizo 9. Thin foils were investigated in an FEI Talos F200X (S)TEM equipped with four energy-dispersive x-ray spectroscopy detectors (Super-EDX). All FIB-SEM and TEM analyses were carried out at the Electron Microscopy Square, Utrecht University.
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