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1 sing the Fourier transform of the RVFV MP-12 tomogram.
2 ent gated acquisition of the second-day rest tomogram.
3 ordinates of candidate-macromolecules in the tomogram.
4 nuclear pore complex obtained from a single tomogram.
5 tching known structures to the cryo electron tomogram.
6 f 9 subvolumes of the adhesin extracted from tomograms.
7 he perinuclear space as seen in the electron tomograms.
8 oteins, averaged 70-79 trimers per virion in tomograms.
9 ings were verified in the postimplant serial tomograms.
10 g both perfusion and function from perfusion tomograms.
11 site using cross-sectional film-based linear tomograms.
12 those from oblique radiographs and computed tomograms.
13 iginal digitized tomograms and the deblurred tomograms.
14 creasing the SNR of cryoEM images and cryoET tomograms.
15 ation between monomeric and dimeric AuNPs in tomograms.
16 late matching to find molecular complexes in tomograms.
17 ratio, using the knowledge learned from raw tomograms.
18 re local membrane thickness in cryo-electron tomograms.
19 enges in visualization and interpretation of tomograms.
20 icient macromolecule localization method for tomograms.
21 volume and low signal-to-noise ratio of the tomograms.
22 ly relevant information from cryo-soft X-ray tomograms.
23 cquisition and minutes-long 3D ptychographic tomograms.
24 ng, are encoded in three-dimensional (3D) RI tomograms.
25 the residual artifacts in the reconstructed tomograms.
26 pre-discharge and 30-day abdominal computed tomograms.
27 d the resolution and the interpretability of tomograms.
28 g methods for detection of complexes in cell tomograms.
29 step in a visual proteomics analysis of cell tomograms.
30 lassification of complexes inside whole-cell tomograms.
31 aled by visualization and segmentation of 3D tomograms.
32 model fit to a reconstruction from electron tomograms.
33 d layer (LSL) were delineated in 2D sagittal tomograms.
34 occurring protein complexes in cryo electron tomograms.
35 resolution and low signal-to-noise ratio in tomograms.
36 known macromolecular complexes in whole cell tomograms.
37 y unknown protein complexes in cryo electron tomograms.
38 ark the results with 3D template matching of tomograms acquired on identical sample locations and ide
39 hieving a resolution of 54 nm full-pitch and tomogram acquisition times of 30 min to two hours, we va
40 postsynaptic signatures, and the subsequent tomograms allow for the identification of key features o
42 applicability using realistically simulated tomograms, allowing for the inclusion of noise and disto
44 workflow readily integrates within existing tomogram analysis pipelines and, when applied across exp
45 advances in cryo-electron tomography and sub-tomogram analysis(2,3) to visualize the structural dynam
47 dges in lower-resolution electron microscopy tomograms and by "mapping" the functional effects of gen
49 o XRF 2D single-slice tomography data and 3D tomograms and is particularly relevant for, but not limi
51 firmed by visual inspection of electron cryo-tomograms and power spectra of single projection views,
54 s characteristic of cryo-electron tomography tomograms and the sheer size of tomographic datasets.
58 rdiograms with Doppler, myocardial perfusion tomograms, and treadmill exercise or pharmacological tes
63 We calculated a 16 angstrom resolution sub-tomogram average of the matrix protein (M) layer that fo
67 particle asymmetric reconstructions and sub-tomogram averages, with intermediate evidence that can a
70 ure of herpesvirus capsids determined by sub-tomogram averaging from nuclei of eukaryotic cells, achi
72 Here, using electron cryo-tomography and sub-tomogram averaging of intact Legionella pneumophila, Pse
73 ryo-ET resolution either by some form of sub-tomogram averaging or template matching, respectively pr
75 Here we use cryo-electron tomography and sub-tomogram averaging to derive the intact structure of the
76 own, we use cryo-electron tomography and sub-tomogram averaging to determine the molecular organizati
77 ynamic biological assemblies, we combine sub-tomogram averaging with atomistic molecular dynamics (MD
79 rety or as individual tiles suitable for sub-tomogram averaging, enabling efficient data processing a
90 potential, we show that 3D refractive index tomograms can capture subtle morphological differences a
95 tion in electrical conductivity shown in the tomograms correlate well with diesel removal from the sa
97 ogram averages calculated from cryo-electron tomograms (cryo-ET) of crowded cellular environments is
100 a series of 6 to 11 apical echocardiographic tomograms, depending on heart rate, in 11 patients.
101 a bracelet-like ring structure for which 4D tomograms display different modes of motion, such as bre
104 lls and molecular specificity within cryo-ET tomograms, ExoSloNano expands the proteome available to
106 We provided a sequence-specific cryo-ET tomogram fitting of DNA minicircles, registering the seq
107 er, preparing extensively annotated cellular tomograms for training macromolecule localization method
108 cross-bridges through the three-dimensional tomogram from their origins on 14.5-nm-spaced shelves al
109 dentification of individual molecules within tomograms from cryoET is challenging because of sample c
110 e, we achieve high quality energy-dispersive tomograms from low dose, noisy datasets using a dedicate
111 d model that infers multiple 3D fluorescence tomograms from RI measurements of the corresponding subc
112 ubcellular features in 120 platelet electron tomograms from these two groups showed statistically sig
114 Through subtomogram averaging and subsequent tomogram-guided sub-particle reconstruction, we determin
115 m 99mTc-sestamibi myocardial perfusion gated tomograms have demonstrated a high degree of accuracy an
116 nsmission Electron Tomography, the resulting tomograms have excellent (de-)focus and alignment proper
117 -0.58 +/- 1.36 mm) compared to the deblurred tomograms (height: -0.58 +/- 1.16 mm; width: 0.37 +/- 0.
119 amework for simulating crowded cryo-electron tomogram images including non-deformable macromolecular
120 This enables users to simulate cryo-electron tomogram images with non-deformable macromolecular compl
123 s for realistically simulating cryo electron tomograms including noise and image distortions due to t
124 sually handled by segmenting the constituent tomograms independently through time with 3D convolution
127 ryoEM community for improving micrograph and tomogram interpretability and accelerating analysis.
128 Automated software transformed cinematic tomograms into images demonstrating uniform appearance o
130 cryo-electron tomography (cryo-ET) images or tomograms is crucial for determining their in situ struc
131 high-resolution signal preserved in the raw tomograms is currently limited by a number of technical
133 ing of macromolecular complexes found within tomograms is known as subtomogram averaging, and this te
134 alization of macromolecules in cryo-electron tomograms is one of the key procedures to unravel struct
135 plex tens of illumination angles in a single tomogram, markedly increasing the volumetric imaging rat
141 ransport at the pore scale, built upon X-ray tomograms of a porous medium at different degrees of liq
144 ients of an ESCRT cargo protein and electron tomograms of Arabidopsis thaliana endosomes to measure c
149 ly be good enough to allow interpretation of tomograms of cells, organelles, bacteria and viruses in
150 Here, we present a framework for simulating tomograms of cellular environments at high crowding leve
151 g the procedure to phantom data and electron tomograms of cellular samples significantly improved the
152 rom the statistical analysis of cryoelectron tomograms of cristae vesicles isolated from Drosophila f
153 hods it is crucial to realistically simulate tomograms of crowded cellular environments, which can th
160 -band, we have used subtomogram averaging of tomograms of rat cardiac muscle in which subtomograms ar
161 his issue, we have scrutinized cryo-electron tomograms of rat hippocampal neurons for the occurrence
164 the RV capsid protein with the cryoelectron tomograms of RV particles established a low-resolution s
165 isting FDTD algorithm by comparing simulated tomograms of single and multiple cylindrical scatterers
170 ing to generate a dataset of 1,829 annotated tomograms of the green alga Chlamydomonas reinhardtii, w
174 lexes, in tens of thousands of electron cryo-tomograms of ~90 bacterial species that we have collecte
175 chnique that is used to produce 3D pictures (tomograms) of complex objects such as asymmetric viruses
176 lating regions or particles of interest from tomograms, organizing them into related groups, and rend
177 ents using biorealistic models guided by our tomograms predict that clustering AMPARs within PSD nano
181 present a method to correct aberrations in a tomogram rather than the beam of a broadband optical int
182 of the limited tilt range; consequently, the tomograms reconstructed using these methods are distorte
184 ment, contrast transfer function estimation, tomogram reconstruction, particle picking, high-resoluti
189 alternative methods in full and undersampled tomogram recovery, but with less significant performance
195 g a cluster of 136 tau filaments in a single tomogram revealed the polypeptide backbone conformation
196 +) spark mass relative to control, while the tomograms revealed both proteins shifted the tetramers i
198 l comparisons of individual particles in the tomograms revealed that a majority of the complexes have
200 osin subfragment 1 atomic structure into the tomogram reveals that 90 degrees target zone bridges sha
201 gned molecular subvolumes extracted from the tomogram reveals that the vast majority of molecules sho
202 agnetic resonance imaging, positron emission tomogram scan and connectivity studies in anesthesia and
204 ion that included chest radiograph, computed tomogram scans, radionuclide imaging, diagnostic cardiac
207 Its application to high-resolution cellular tomograms should also help identify differently oriented
216 y for 60 degrees samples of 11-13 short-axis tomograms spanning the entire heart, from which regional
217 d severely changed in averaged cryo-electron tomograms, suggesting that NDK5 is crucial for the intac
218 fast (short-duration) transmission computed tomogram (TCT), acquired immediately before or after the
219 lized by crystal structures and cryoelectron tomograms, the critical gp41-interactive region of gp120
221 ET method for localizing objects within cryo-tomograms to beyond the diffraction limit of the light m
222 onents, and use ligand-oriented cryoelectron tomograms to define component mobility in the viral spik
223 study retrospectively analyzed conventional tomograms to estimate the prognostic value of the cross-
225 showed perfusion defects on the post-stress tomogram underwent gated acquisition of the second-day r
226 ) acquisition technique that collects apical tomograms using a continuously internally rotating trans
229 plate-free classification of oversampled sub-tomograms was used to analyze cryo-electron tomograms of
230 e magnetic catheter, guided by a 3D computed tomogram, was successfully navigated to all pulmonary ve
232 s scaling analysis on ChromSTEM mass density tomograms, we observed that chromatin forms spatially we
235 ular horizontal and vertical long axis gated tomograms were generated for 116 studies chosen on the b
239 ferences in visual acuity, optical coherence tomograms were recorded in some patients to visualize ce
240 We demonstrate in the domain of time series tomograms which are typically undersampled to allow more
241 eter-free reconstruction method for ion beam tomograms with high accuracy is developed for low-densit
242 for sub-tomogram averaging, IsoNet generates tomograms with significantly reduced resolution anisotro