A dynamic temperature mapping system with a 320x256 pixels frame size and 100kHz sampling rate

2008 ◽  
Author(s):  
M. Riccio ◽  
G. Breglio ◽  
A. Irace ◽  
P. Spirito
Keyword(s):  
Sampling Rate ◽  
Frame Size ◽  
Temperature Mapping ◽  
Dynamic Temperature ◽  
Mapping System

An equivalent time temperature mapping system with a 320×256pixels full-frame 100kHz sampling rate

2007 ◽  
Vol 78 (10) ◽  
pp. 106106 ◽  
Author(s):  
M. Riccio ◽  
G. Breglio ◽  
A. Irace ◽  
P. Spirito
Keyword(s):  
Sampling Rate ◽  
Temperature Mapping ◽  
Equivalent Time ◽  
Mapping System

Automatic temperature mapping system based on holographic interferometry

1982 ◽  
Vol 18 (14) ◽  
pp. 623 ◽  
Author(s):  
G. Lucarini ◽  
F. Piazza ◽  
C. Morandi ◽  
A. Pierfederici
Keyword(s):  
Holographic Interferometry ◽  
Automatic Temperature ◽  
Temperature Mapping ◽  
Mapping System

Development of a continuous temperature mapping system using a deep body thermometer

2002 ◽  
Vol 26 (3) ◽  
pp. 123-125 ◽  
Author(s):  
T. Matsui ◽  
K. Hagisawa ◽  
T. Ishizuka ◽  
K. Matsumura ◽  
M. Ishihara ◽  
...  
Keyword(s):  
Temperature Mapping ◽  
Mapping System ◽  
Deep Body ◽  
Continuous Temperature

Development of a temperature mapping system for 1.3-GHz 9-cell SRF cavities

2007 ◽  
Author(s):  
A. Canabal ◽  
J.D. Bowyer ◽  
P. Chacon ◽  
N. A. Gillespie ◽  
M.A. Madrid ◽  
...  
Keyword(s):  
Temperature Mapping ◽  
Mapping System ◽  
Srf Cavities

The extended Fourier algorithm: Application in discrete optics and electron holography

1994 ◽  
Vol 52 ◽  
pp. 918-919
Author(s):  
E. Voelkl ◽  
L. F. Allard
Keyword(s):  
Fourier Transform ◽  
Fourier Transforms ◽  
Sampling Rate ◽  
Electron Holography ◽  
Optical Bench ◽  
Fourier Space ◽  
Ccd Cameras ◽  
Simulated Image ◽  
Initial Sampling ◽  
Fourier Algorithm

The conventional discrete Fourier transform can be extended to a discrete Extended Fourier transform (EFT). The EFT allows to work with discrete data in close analogy to the optical bench, where continuous data are processed. The EFT includes a capability to increase or decrease the resolution in Fourier space (thus the argument that CCD cameras with a higher number of pixels to increase the resolution in Fourier space is no longer valid). Fourier transforms may also be shifted with arbitrary increments, which is important in electron holography. Still, the analogy between the optical bench and discrete optics on a computer is limited by the Nyquist limit. In this abstract we discuss the capability with the EFT to change the initial sampling rate si of a recorded or simulated image to any other(final) sampling rate sf.

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