CuttingPlane: An Efficient Algorithm for Three-Dimensional Spatial Skyline Queries Based on Dynamic Scan Theory

Author(s):  
Meng Zhao ◽  
Jing Yu
2020 ◽  
Vol 192 ◽  
pp. 105299 ◽  
Author(s):  
Marta Fort ◽  
J. Antoni Sellarès ◽  
Nacho Valladares

1999 ◽  
Vol 19 (3) ◽  
pp. 272-277 ◽  
Author(s):  
Manouchehr S. Vafaee ◽  
Ernst Meyer ◽  
Sean Marrett ◽  
T. Paus ◽  
Alan C. Evans ◽  
...  

To test the hypothesis that brain oxidative metabolism is significantly increased upon adequate stimulation, we varied the presentation of a visual stimulus to determine the frequency at which the metabolic response would be at maximum. The authors measured regional CMR O2 in 12 healthy normal volunteers with the ECAT EXACT HR+ (CTI/Siemens, Knoxville, TN, U.S.A.) three-dimensional whole-body positron emission tomograph (PET). In seven successive activating conditions, subjects viewed a yellow-blue annular checkerboard reversing its contrast at frequencies of 0, 1, 4, 8, 16, 32, and 50 Hz. Stimulation began 4 minutes before and continued throughout the 3-minute dynamic scan. In the baseline condition, the subjects began fixating a cross hair 30 seconds before the scan and continued to do so for the duration of the 3-minute scan. At the start of each scan, the subjects inhaled 20 mCi of 15O-O2 in a single breath. The CMR O2 value was calculated using a two-compartment, weighted integration method. Normalized PET images were averaged across subjects and coregistered with the subjects' magnetic resonance imaging in stereotaxic space. Mean subtracted image volumes (activation minus baseline) of CMR O2 then were obtained and converted to z statistic volumes. The authors found a statistically significant focal change of CMR O2 in the striate cortex (x = 9; y = −89; z = −1) that reached a maximum at 4 Hz and dropped off sharply at higher stimulus frequencies.


2019 ◽  
Vol 2 (3) ◽  
pp. 154-159
Author(s):  
Maxim Protasov ◽  
Dmitry Neklyudov ◽  
Leonid Nazarov

The paper deals with the three-dimensional travel-time tomography of the first arrivals. The model is represented by Chebyshev polynomials. This allows one to use a priori information about the model effectively and reduce the number of recoverable parameters to the required minimum. Also, such a model representation makes it possible to obtain a very efficient algorithm for solving the two-point ray-tracing problem for three-dimensional media, which is necessary for tomography. Examples of solving the three-dimensional cross-well tomography, as well as examples using tomography for the reconstruction of stress fields in the coal-rock mass are presented.


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