By L. Marton (ed.)
This quantity includes overview articles overlaying a extensive diversity of themes in photo processing and research. the themes lined contain photo research - which has united and harmonized a bunch of heterogeneous fabric; modern methods to the Fourier remodel; quantity theoretic transforms, that are rather beautiful for discrete, finite signs; using the Wigner distribution - which encodes either spatial and spectral details, for photograph filtering; and functions of the idea that of knowledge power. those up to date surveys are meant to supply the reader with entry to the newest ends up in the super energetic box of photograph technology.
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Extra resources for Advances in Electronics and Electron Physics, Vol. 35
In Fig. 46 Anode Fici. 22. Westburg’s potential distribution plots for argon at 97 p and 1700 V during first 160 nsec of secondary wave propagation with A1 cathode in tube 146 cm long. Asterisks indicate zero time which is the instant the potential begins to change a t the first plasma probe. From (38) with permission of PItys. Rev. 28 RICHARD G . 23. Electrical field and reduced field (Ejp) distributions during the first 100 nsec of secondary wave propagation as derived from curves in Fig. 22.
25 Torr. After Mills, Naraghi a n d Fowler (51) with permission of Phjs. FINids. et at. found that precursor breakdown is under a n entirely new regime, with the attenuation not only as much as 30 times greater but increasing slightly with applied voltage rather than decreasing as i n the electrostatic apparatus. 95 m-' within the experimental error. N o clear distinction was found between proand antiforce precursors in this respect. 38. Velocity vs. 65 Torr. Numbers on each curve are attenuation in m - ' .
I 1 3 106 (V/rn/Torr) FIG. 18. Antiforce wave velocities vs. applied potential in helium. 98. Y. Fhids. 30. 8, by Latimer. Mills, and Day (32) in a situation similar to this one, but quasistatic. It depends on taking the ratio of the intensities of two emission lines. When the excitation of gas atoms is due solely to random electron collisions, and multiple processes such as excitation transfer or excitation from the metastable states are negligible, the intensity ratio of two spectral lines, as measured by the signal S from a photomultiplier tube, is given by SjklSim = ( Q j r l l > I ( Qimzl> (3) or SjklSlm == < .
Advances in Electronics and Electron Physics, Vol. 35 by L. Marton (ed.)