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Anisotropy

Anisotropy refers to the directional dependence of a material's physical properties, such as optical, electrical, or mechanical characteristics.
It arises from the inherent structural or compositional asymmetry within the material.
Anisotropy is a fundamental concept in materials science and plays a crucial role in the design and optimization of a wide range of technologial applications, from photonics and electronics to structural engineering.
Understanding and characterizing anisotropy is essential for ensuirng the reliable performance and functionality of these systems.

Most cited protocols related to «Anisotropy»

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Publication 2006
Anisotropy Corpus Callosum Diffusion Fibrosis Mental Orientation Population Group
The total model structure factor comprises a number of contributions, where koverall is an overall scale factor, Ucryst is the overall anisotropic scale matrix (Sheriff & Hendrickson, 1987 ▶ ; Grosse-Kunstleve & Adams, 2002 ▶ ), h is a column vector with the Miller indices of a reflection and ht is its transpose, Fcalc are the structure factors computed from the atomic model, ksol and Bsol are flat bulk-solvent model parameters (Phillips, 1980 ▶ ; Jiang & Brünger, 1994 ▶ ), s2 = htG*h, where G* is the reciprocal-space metric tensor, and Fmask are structure factors calculated from a solvent mask (a binary function with zero values in the protein region and non-zeros values in the solvent region). The mask is computed using memory-efficient exact asymmetric units described in Grosse-Kunstleve et al. (2011 ▶ ). The mask-calculation parameters, rsolvent and rshrink, can be optimized in each refinement macro-cycle.
The structure factors from the atomic model, Fcalc, are computed using either fast Fourier transformation (FFT) or direct-summation algorithms (for a review, see Afonine & Urzhumtsev, 2004 ▶ ). Various X-ray and neutron scattering dictionaries are available (Neutron News, 1992 ▶ ; Maslen et al., 1992 ▶ ; Waasmaier & Kirfel, 1995 ▶ ; Grosse-Kunstleve, Sauter et al., 2004 ▶ ).
phenix.refine uses a very efficient and robust algorithm for finding the best values for ksol, Bsol and Ucryst. The details of the algorithm, as well as a comprehensive set of references to relevant works, have been described previously (Afonine et al., 2005b ▶ ). A radial-shell bulk-solvent model (Jiang & Brünger, 1994 ▶ ) is also available. In the case of refinement against twinned data, the total model structure factor is defined as where α is a twin fraction and is determined by minimizing the R factor using a simple grid search in the [0, 0.5] range with a step of 0.01 and the matrix T defines the twin operator.
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Publication 2012
Anisotropy Cloning Vectors Dietary Fiber Memory Protein Domain Radiography Reflex R Factors Solvents Twins
All the structures were solved by either Patterson or direct methods with SHELXS (Sheldrick, 2008 ▶ ). They were refined by full-matrix least squares against F2 using SHELXL-2014/3 with the help of the SHELXle graphical user interface (Hübschle et al., 2011 ▶ ). All non-H atoms were refined with anisotropic displacement parameters (ADPs). The H atoms were set to idealized positions and refined using a riding model with their isotropic displacement parameters constrained to be 1.5 times the equivalent isotropic displacements of the atoms to which they were attached for methyl H atoms and 1.2 times for all other H atoms. The bromine/chlorine disorder in 2 was treated with EADP/EXYZ constraints in SHELXL-2014/3. In compound 6 the chlorine/bromine disorder and the rotational disorder of the tertiary butyl group attached to N1 were refined using distance and ADP restraints.
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Publication 2015
Anisotropy Bromine Chlorine Displacement, Psychology
All other image processing operations were performed in the XMIPP package.18 (link) Prior to refinement, all data sets were normalized using previously described procedures.5 (link) MAP refinements and projection matching refinements in XMIPP were performed with similar settings where possible. Although the implementation of the MAP approach readily handles anisotropic CTF models, all refinements were performed with isotropic CTFs (without envelope functions) for the sake of comparison with XMIPP. All orientational searches, or integrations in the statistical approach, were performed over the full five dimensions, that is, three Euler angles and two translations. For both the thermosome and the GroEL refinements, the first 10 iterations were performed with an angular sampling of 7.5°, and subsequent iterations were performed with an angular sampling interval of 3.75°. Thermosome refinements were stopped after 15 iterations, and GroEL refinements, after 20. Translational searches were limited to ± 10 pixels in both directions in the first 10 iterations and to ± 6 pixels in the subsequent iterations. Although it is common practice in XMIPP to reduce computational costs by breaking up the orientational search into separate rotational and translational searches and to limit rotational searches to local searches around previously determined orientations, this was not done in the refinements presented here for the sake of comparison with the MAP approach. Refinements with angular sampling intervals as fine as 1° where such tricks were employed did not result in better reconstructions (results not shown).
The true resolution of the GroEL reconstructions was assessed by FSC with a published crystal structure (Protein Data Bank ID: 1XCK). This structure contains 14 unique monomers in its asymmetric unit. Each of these monomers was fitted separately into the reconstructions using UCSF Chimera,41 (link) and for each monomer, the equatorial, intermediate, and apical domains were allowed to move independently as rigid bodies. The resulting coordinates were converted to an electron density map that was symmetrized according to D7 symmetry. Optimization of the relative magnification between this map and the cryo-EM reconstructions revealed that the effective pixel size of the cryo-EM images was 2.19 Å, differing by 3% from the nominal value, and this value was used to generate all plots in Fig. 3.
Ribosome refinements were performed for 25 iterations with an angular sampling of 7.5° and translational searches of ± 10 pixels. To generate K = 4 unsupervised initial starting models from a single  80-Å low-pass filtered initial ribosome structure, during the first iteration, we divided the data set into four random subsets in a way similar to that described before.21 (link)
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Publication 2012
Anisotropy Chimera Electrons Human Body Mental Orientation Muscle Rigidity Protein Biosynthesis Reconstructive Surgical Procedures Ribosomes Thermosomes

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Publication 2016
Anisotropy Diffusion Fibrosis Mental Orientation

Most recents protocols related to «Anisotropy»

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Example 3

Alternatively or in addition to all of the foregoing as it relates to gray matter, the invention further contemplates that white matter fA (fractional anisotropy) can be employed in a manner analogous to the gray matter atrophy as discussed herein in various embodiments.

Diffusion Tensor Imaging (DTI) assesses white matter, specifically white matter tract integrity. A decrease in fA can occur with either demyelination or with axonal damage or both. One can assess white matter substructures including optic nerve and cervical spinal cord.

MRIs of brain including high cervical spinal cord to be done at month 6, 1 year, and 2 years. If a decrease in fA of 10% is observed in fA of 2 tracts, treat with estriol to halt this decrease. Alternatively if fA is decreased by 10% in only one tract but that tract is associated with clinical deterioration of the disability served by that tract, treat with estriol. Poorer scores in low contrast visual acuity would correlate with decreased fA of optic nerve, while poorer motor function would correlate with decreased fA in motor tracts in cervical spinal cord.

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Patent 2024
Anisotropy Atrophy Axon Brain Clinical Deterioration Copaxone Demyelination Disabled Persons Estriol Gray Matter Magnetic Resonance Imaging Multiple Sclerosis Optic Nerve Spinal Cords, Cervical Visual Acuity White Matter
Single crystal sized (0.35, 0.25, 0.20) mm3 was carefully selected to perform its structural analysis by X-ray diffraction. The crystallographic data were collected on a Bruker AXS CCD diffractometer at room temperature using graphite-monochromated Mo Kα radiation (λ = 0.71073 Å). All intensities were corrected for Lorentz, polarization and absorption effects.15 (link) The structural determination procedure was carried out using SHELXS97 program.16 The structure was solved by direct method and refined with full-matrix least squares methods based on F2 using SHELXL97.17 The space group was determined to be P21/n. A total of 54568 reflections were collected in the θ range 2.2–27.5°. In this structure, all non-hydrogen atoms were refined with anisotropic displacement parameters. H-atoms were set in calculated positions and treated as riding on their parent atom with constrained thermal parameters. The final discrepancy factors R1 and wR2 are 0.053 and 0.134, respectively. Crystal data of (C12H17N2)2ZnBr4 are given in Table 1. Molecular plots were made with ORTEP18 (link) and Diamond.19 Atomic coordinates anisotropic displacement parameters, tables for all bond distances, and angles have been deposited at the Cambridge Crystallographic Data Centre (deposition number: CCDC 2090035).
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Publication 2023
Anisotropy Crystallography Diamond Graphite Hydrogen Parent Radiotherapy Reflex X-Ray Diffraction
To determine whether the shape of B. napus seeds could be appropriately described by star-convex polygons, the accuracy of reconstruction of ground truth labels for a small subset of 10 3D sub-volumes from the ‘training’ dataset was explored. Accuracy of reconstructed seeds was assessed based on the mean intersection-over-union (IoU) of ground-truth seed labels compared to 3D star-convex polyhedra shape representations of the seed, predicted using the method described by Weigert et al. (2020) in which for each pixel inside a seed the distance to the object boundary is calculated along a fixed set of rays that are approximately evenly distributed on an ellipsoid representative of the seeds within the dataset (see Weigert et al., 2020 eq. 1). The sets of rays used in seed reconstruction were calculated as Fibonacci rays, defined using the method described by Weigert et al. (2020) , which were shown to be more accurate for reconstruction of 3D star-convex polyhedra than equidistant distributed rays and allowed for the potential anisotropy of seed to be taken into account. Reconstruction accuracy was investigated using a varying number of Fibonacci rays (8, 16, 32, 64, 96, and 128), as although Weigert et al. (2020) found a set of at least 64 rays was necessary to achieve accurate reconstruction of shape for cell nuclei, they suggested accurate reconstruction of less anisotropic or densely-packed objects may be possible with a smaller set of rays which would allow for less computational resources to be used in shape prediction.
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Publication 2023
Anisotropy Cell Nucleus Radiation Reconstructive Surgical Procedures
A StarDist-3D model with a U-Net backbone (Çicek et al., 2016 (link)) was trained to detect and segment individual B. napus seeds in 3D µCT sub-volumes from the labelled ‘training’ dataset using the pipeline described by Weigert et al. (2020) . Model training was performed using a Google Colab runtime with 25.46 GB and a single GPU (Bisong, 2019 (link)). The StarDist-3D model was configured to use 96 Fibonacci rays in shape reconstruction, and to take into account the mean empirical anisotropy, of all labelled seeds in the dataset along each axis as calculated using the method described by Weigert et al., 2020 (X-axis = 1.103448275862069, Y-axis anisotropy = 1.032258064516129, Z-axis anisotropy = 1.0). The training patch size, referring to the size of the tiled portion of the 3D sub-volumes in the ‘training’ within view of the neural network at any one time, was set to Z = 24, X= 96, and Y = 96 and training batch size set to 2. Training ran for 400 epochs with 100 steps per epoch and took 1.36 hours to complete (123ms/step).
Model validation was then performed by using the fine-tuned StarDist-3D algorithm to predict seed labels for all 3D µCT sub-volumes from the ‘validation’ dataset, which were then compared to the number and shape of seeds manually counted and labelled during annotation. Accuracy of seed detection and segmentation was then quantified for various levels of threshold τ, defined as the IoU between the predicted label and ground-truth label for each seed. The value of τ ranged between 0, where even a very slight overlap between predicted seeds and actual seeds counted as correctly predicted, and 1, where only predicted seed labels with pixel-perfect overlap with ground-truth labels counted as correctly predicted (Weigert et al., 2020 ).
Object detection accuracy was measured using the number of true positive results (TP), or number manually counted and labelled seeds that were correctly detected seeds, the number of false negative results (FN), or the number of manually counted and labelled seeds that were missed, the number of false positive results (FP), or number of objects other than seeds than were detected, recall, precision and F1-score. Recall related to the fraction of relevant objects that were successfully detected and was defined as:
Precision related to the fraction of all detected objects that were relevant and was defined as:
F1-score related to the harmonic mean of precision and recall, with the impact of precision and recall being given equal weight. F1-score was defined as:
The accuracy of seed segmentation, or the accuracy of seed size and shape prediction, for the validation dataset was determined based on the mean matched score, defined as the mean IoU between the predicted and actual shape of true positive results, the mean true score, defined as the mean IoU between the predicted and actual shape of true positive results normalised by the total number of ground-truth labelled seeds, and panoptic quality, as defined in Eq.1 of Kirillov et al., 2019 .
StarDist-3D models allow for specification of two values, the τ-threshold and the nms-threshold to optimize model output (Schmidt et al., 2018 ; Weigert et al., 2020 ). The τ-threshold refers to the minimum intersection-over-union between pairs of predicted and ground-truthed seeds required for detections to be classified as true positives, and can be set at 0.1 interval levels between 0.1 and 1 with 0.1 indicating a 10% overlap in the pixels within the predicted shape of a seed and the ground-truthed label and 1 respreseting a 100% overlap (Schmidt et al., 2018 ; Weigert et al., 2020 ). The nms-threshold, refers to the level of non-maximum suppression applied to the results of object detection and instance segmentation to prune the number of predicted star-convex polyhedra in ideally retain a single predicted shape for each true object, in this case each seed, within an image. The nms-threshold can be set at 0.1 interval levels between 0 and 1 with higher levels indicating more aggressive pruning of predicted shapes which therefore leads to fewer detections in the final model output. Therefore a higher nms-threshold is valuable in cases where the number of false positives expected in unfiltered model predictions is high. Both the τ-threshold and the nms-threshold for the fine-tuned StarDist-3D algorithm were set to optimal values based on the ‘validation’ dataset using the ‘optimize_thresholds’ function of StarDist (Schmidt et al., 2018 ).
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Publication 2023
Anisotropy Epistropheus EPOCH protocol Mental Recall Radiation Reconstructive Surgical Procedures Vertebral Column
For fMRI data, the pre-processing was performed using SPM12 (Wellcome Department of Imaging Neurosciences, University College London, UK, http://www.fil.ion.ucl.ac.uk/spm), and the statistical analyses of imaging data were performed using GRETNA (GRETNA v2.0) in Matlab R2021b. First, the first 10-time point-scanned images were removed owing to the instability of the magnetic field at the beginning of the scan. Second, all functional images were realigned to the first image to correct head movement. All participants met the criteria of < 2 mm translation and < 2° rotation in any direction. Otherwise, their data were excluded. Third, the functional images were normalized to the MNI space using DARTEL and resampled to a 3 × 3 × 3 mm3 voxel size62 (link). Fourth, we used an anisotropic 6-mm full-width half-maximum Gaussian kernel63 for spatial smoothing of the obtained images. Fifth, we detrended and removed linear trends. Sixth, we removed covariates, excluding white matter, grey matter, and cerebrospinal fluid influences. Seventh, 0.01‒0.08 Hz bandpass filtering was used to remove high and low-frequency signals. Eighth, we removed the FD_Threshold > 0.5 mm time points by “scrubbing” 1-time point before and 2-time points after. In summary, the pre-processing procedures included slice timing correction, realignment, normalization, smoothing, detrending, filtering, and scrubbing.
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Publication 2023
Anisotropy Cerebrospinal Fluid fMRI Gray Matter Head Movements Magnetic Fields Radionuclide Imaging White Matter

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More about "Anisotropy"

Anisotropy, the directional dependence of a material's physical properties, is a fundamental concept in materials science that plays a crucial role in the design and optimization of a wide range of technological applications.
This asymmetry within the material can arise from its inherent structural or compositional characteristics, affecting its optical, electrical, or mechanical behavior.
Understanding and characterizing anisotropy is essential for ensuring the reliable performance and functionality of systems in fields like photonics, electronics, and structural engineering.
Researchers utilize advanced analytical techniques and instrumentation, such as MATLAB, APEX-II CCD diffractometers, D8 Venture and APEX2 systems, Eclipse treatment planning software, D8 Quest diffractometers, SMART APEX CCD diffractometers, and FluoroMax-4 spectrofluorometers, to study and quantify anisotropic properties.
These tools and techniques enable scientists to gain insights into the anisotropic nature of materials, optimizing their design and application.
By incorporating this knowledge, engineers can develop innovative solutions that harness the unique properties of anisotropic materials, unlocking new possibilities in fields like optoelectronics, structural composites, and beyond.
Leveraging the understanding of anisotropy is crucial for advancing technological frontiers and ensuring the reliable performance of these critical systems.