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Monkey Cutaneous SAI and RA Responses to Raised and Depressed Scanned Patterns: Effects of Width, Height, Orientation, and a Raised Surround

by David Blake Kenneth, David T. Blake, Steven, S. Hsiao, David T, Kenneth O. Johnson, Kenneth O. Johnson - Journal of Neurophysiology , 1997
"... this paper. Stimuli were scanned from proximal from 160 impulses / s (ips) for the 7.0 mm wide square to to distal on the distal pad of 1 of the digits at 30 g force and 40 mm/s. 275 ips for the 0.8 mm wide square. The comparable range Patterns were shifted 0.2 mm orthogonal to the scanning directio ..."
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this paper. Stimuli were scanned from proximal from 160 impulses / s (ips) for the 7.0 mm wide square to to distal on the distal pad of 1 of the digits at 30 g force and 40 mm/s. 275 ips for the 0.8 mm wide square. The comparable range Patterns were shifted 0.2 mm orthogonal to the scanning direction between for the RA mean rate profiles was 120 -- 170 ips. The peak scans. A : spatial event plot (SEP) . Action potential data at the tops of SEPs came earlier in the stimulus sequence than those lower in the raster. rates evoked by the falling edges were less variable partly Similarly, the scanning direction in the displays is from left to right; thus because the falling peak rates were less than the rising rates ticks at the left of the plot represent action potentials evoked by the leading and partly because the falling responses didn't emerge as edge of the stimulus and ticks to the right, the trailing edge. B : instantaneous separate entities until the squares were

Height Width

by Josef Frisch, Allison Chang, Valentin Decker, Eric Doyle, Leif Eriksson, Linda Hendrickson, Wall Thickness , 2006
"... The small beam sizes at the interaction point of a X-band linear collider require mechanical stabilization of the final focus magnets at the nanometer level. While passive systems provide adequate performance at many potential sites, active mechanical stabilization is useful if the natural or cultur ..."
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The small beam sizes at the interaction point of a X-band linear collider require mechanical stabilization of the final focus magnets at the nanometer level. While passive systems provide adequate performance at many potential sites, active mechanical stabilization is useful if the natural or cultural ground vibration is higher than expected. A mechanical model of a room temperature linear collider final focus magnet has been constructed and actively stabilized with an accelerometer based system. PROTOTYPE SYSTEM One option for the warm linear collider is to use a permanent magnet final focus. The small beam sizes at the IP of the linear collider require nanometer scale stabilization of the final doublets. Passive stabilization, interferometer based stabilization, and inertial stabilization have been considered. This paper describes a prototype of the inertial stabilization system. The prototype system is designed to have mechanical properties similar to an actual permanent magnet final doublet and support raft, but is constructed somewhat differently, figure 1. It is referred to as the “extended object ” to distinguish it from an earlier prototype consisting of a simple suspended block. [1]

Chapter 304 Traffic Regulations

by unknown authors , 2008
"... Regulations as to width, height and length of vehicles. ..."
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Regulations as to width, height and length of vehicles.

Length Width Height Wheelbase Weight Distribution  Front      Rear      Total Wheel Size  Front      Rear Frontal area Steering Front      Rear Braking Front      Rear      Both

by Frame Material, Estimated Cd , 2011
"... Number of wheels Vehicle Dimensions (please use inches,  pounds) ..."
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Number of wheels Vehicle Dimensions (please use inches,  pounds)

Pyramidal implementation of the Lucas Kanade feature tracker

by Jean-yves Bouguet - Intel Corporation, Microprocessor Research Labs , 2000
"... grayscale value of the two images are the location x = [x y] T, where x and y are the two pixel coordinates of a generic image point x. The image I will sometimes be referenced as the first image, and the image J as the second image. For practical issues, the images I and J are discret function (or ..."
Abstract - Cited by 308 (0 self) - Add to MetaCart
arrays), and the upper left corner pixel coordinate vector is [0 0] T. Let nx and ny be the width and height of the two images. Then the lower right pixel coordinate vector is [nx − 1 ny − 1] T. Consider an image point u = [ux uy] T on the first image I. The goal of feature tracking is to find

7 The height, length and width of

by Alberto Corsín Jiménez
"... social theory ..."
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social theory

WIDTHS AND HEIGHTS OF (0,1)-MATRICES

by D. R. Fulkerson, H. J. Ryser , 1962
"... ..."
Abstract - Cited by 4 (1 self) - Add to MetaCart
Abstract not found

TRACES, TERM RANKS, WIDTHS AND HEIGHTS

by D. R. Fulkerson, H. J. Ryser , 1960
"... ..."
Abstract - Cited by 1 (0 self) - Add to MetaCart
Abstract not found

new calculations of the barrier height and width

by Sergei Skokov, Shengli Zou, A Joel M. Bowman, Thomas C. Allison, Donald G. Truhlar, Yongjing Lin, D B. Ramach, Bruce C. Garrett, Benjamin J. Lynch C , 2000
"... + HCl reaction and ..."
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+ HCl reaction and

On the asymptotic joint distribution of height and width in random trees

by Svante Janson - STUDIA SCI. MATH. HUNGAR , 2008
"... It has been known for a long time that the height and width of a random labelled rooted tree, or of any other conditioned Galton Watson tree, after suitable normalizations converge to the same limit distribution. Moreover, Chassaing, Marckert and Yor [7] have proved joint convergence of height and w ..."
Abstract - Cited by 4 (2 self) - Add to MetaCart
It has been known for a long time that the height and width of a random labelled rooted tree, or of any other conditioned Galton Watson tree, after suitable normalizations converge to the same limit distribution. Moreover, Chassaing, Marckert and Yor [7] have proved joint convergence of height
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