Geodetic support for an absolute calibration experiment of a high-precision radio altimeter

2021 ◽  
Vol 65 (5) ◽  
pp. 505-516
Author(s):  
Langeman I.P. ◽  
◽  
Kupriyanov A.O. ◽  
Morozov D.A. ◽  
Kuznetsov D.A. ◽  
...  

Представлено геодезическое обеспечение экспериментального исследования по выполнению калибровки высокоточного радиовысотомера. Рассмотрены организационные и методические аспекты исследования, конструкция водомерного буя. Приводятся результаты вычислений высоты морской топографической поверхности и поправки за поперечный уклон геоида.

2004 ◽  
Vol 27 (3-4) ◽  
pp. 657-681 ◽  
Author(s):  
J. J. MARTINEZ-BENJAMIN ◽  
M. MARTINEZ-GARCIA ◽  
S. GONZALEZ LOPEZ ◽  
A. NUÑEZ ANDRES ◽  
F. BUILL POZUELO ◽  
...  

1998 ◽  
Vol 5 (3) ◽  
pp. 756-758 ◽  
Author(s):  
C. Fujikawa ◽  
T. Kawachi ◽  
K. Ando ◽  
N. Yamaguchi ◽  
T. Hara

Absolute calibration of a soft X-ray spectrograph has been performed using a white beam of synchrotron radiation. The calibrated spectrograph was a flat-field grazing-incidence spectrograph with an X-ray CCD detector for X-ray laser research. Absolute sensitivity of the spectrograph system can be obtained from transmitted spectra using filters made of several different materials, each providing an absorption-edge wavelength standard. The absolute sensitivity determined in this work shows nearly the same behaviour with wavelength as that in another calibration experiment using a laser-produced plasma as an X-ray source.


2016 ◽  
Vol 595 ◽  
pp. A108 ◽  
Author(s):  
A. Crouzier ◽  
F. Malbet ◽  
F. Henault ◽  
A. Léger ◽  
C. Cara ◽  
...  

2015 ◽  
Vol 584 ◽  
pp. 012020 ◽  
Author(s):  
Yana V Gladysheva ◽  
Ilya V Zhivotovsky ◽  
Dmitry G Denisov ◽  
Nikolay V Baryshnikov ◽  
Valery E Karasik ◽  
...  

Author(s):  
J. C. Russ ◽  
T. Taguchi ◽  
P. M. Peters ◽  
E. Chatfield ◽  
J. C. Russ ◽  
...  

Conventional SAD patterns as obtained in the TEM present difficulties for identification of materials such as asbestiform minerals, although diffraction data is considered to be an important method for making this purpose. The preferred orientation of the fibers and the spotty patterns that are obtained do not readily lend themselves to measurement of the integrated intensity values for each d-spacing, and even the d-spacings may be hard to determine precisely because the true center location for the broken rings requires estimation. We have implemented an automatic method for diffraction pattern measurement to overcome these problems. It automatically locates the center of patterns with high precision, measures the radius of each ring of spots in the pattern, and integrates the density of spots in that ring. The resulting spectrum of intensity vs. radius is then used just as a conventional X-ray diffractometer scan would be, to locate peaks and produce a list of d,I values suitable for search/match comparison to known or expected phases.


Author(s):  
K. Z. Botros ◽  
S. S. Sheinin

The main features of weak beam images of dislocations were first described by Cockayne et al. using calculations of intensity profiles based on the kinematical and two beam dynamical theories. The feature of weak beam images which is of particular interest in this investigation is that intensity profiles exhibit a sharp peak located at a position very close to the position of the dislocation in the crystal. This property of weak beam images of dislocations has an important application in the determination of stacking fault energy of crystals. This can easily be done since the separation of the partial dislocations bounding a stacking fault ribbon can be measured with high precision, assuming of course that the weak beam relationship between the positions of the image and the dislocation is valid. In order to carry out measurements such as these in practice the specimen must be tilted to "good" weak beam diffraction conditions, which implies utilizing high values of the deviation parameter Sg.


Author(s):  
Klaus-Ruediger Peters

Differential hysteresis processing is a new image processing technology that provides a tool for the display of image data information at any level of differential contrast resolution. This includes the maximum contrast resolution of the acquisition system which may be 1,000-times higher than that of the visual system (16 bit versus 6 bit). All microscopes acquire high precision contrasts at a level of <0.01-25% of the acquisition range in 16-bit - 8-bit data, but these contrasts are mostly invisible or only partially visible even in conventionally enhanced images. The processing principle of the differential hysteresis tool is based on hysteresis properties of intensity variations within an image.Differential hysteresis image processing moves a cursor of selected intensity range (hysteresis range) along lines through the image data reading each successive pixel intensity. The midpoint of the cursor provides the output data. If the intensity value of the following pixel falls outside of the actual cursor endpoint values, then the cursor follows the data either with its top or with its bottom, but if the pixels' intensity value falls within the cursor range, then the cursor maintains its intensity value.


1991 ◽  
Vol 1 (12) ◽  
pp. 1669-1673 ◽  
Author(s):  
Hans Gerd Evertz ◽  
Martin Hasenbusch ◽  
Mihail Marcu ◽  
Klaus Pinn ◽  
Sorin Solomon

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