A Study of Low-Noise Preamplifier Systems for Use with Room Temperature Mercuric Iodide (Hgi2) X-Ray Detectors

1981 ◽  
Vol 28 (1) ◽  
pp. 579-582 ◽  
Author(s):  
J. S. Iwanczyk ◽  
A. J. Dabrowski ◽  
G. C. Huth ◽  
A. Del Duca ◽  
W. Schnepple
1980 ◽  
Author(s):  
J.S. Iwanczyk ◽  
A.J. Dabrowski ◽  
G.C. Huth ◽  
A. Del Duca ◽  
W. Schenpple

1982 ◽  
Vol 26 ◽  
pp. 325-330 ◽  
Author(s):  
Lawrence Ames ◽  
William Drummond ◽  
Jan Iwanczyk ◽  
Andrzej Dabrowski

AbstractThe performance of a room temperature mercuric iodide X-ray detector was investigated as a function of detector bias, amplifier time constant, and detector temperature. A Mn Kα line of 200 eV FWHM was obtained by using low noise electronics developed for Si(Li) detectors, including a cooled input PET. Measurements of the detector's resolution at various X-ray energies result in a Fano factor of 0.20.


1982 ◽  
Vol 16 ◽  
Author(s):  
John H. Howes ◽  
John Watling

ABSTRACTThis paper describes the fabrication of mercuric iodide nuclear radiation detectors suitable for X and gamma ray spectrometry at room temperature. The active area of the detectors studied are between 0.2 and 1.5cm sq and they are up to 0.5mm thick. The method of producing a stable electrical contact to the crystal using sputtered germanium has been studied. The X-ray resolution of a 1.5cm sq. area detector at 32 keV is 2.3 keV FWHM when operated at room temperature in conjunction with a time variant filter amplifier. A factor which is important in the fabrication of the detector is the surface passivation necessary to achieve a useful detector life.This type of detector has been used on a wavelength dispersive X-ray spectrometer for energy measurements between 10 and 100 keV. The advantages over the scintillation counter, more commonly used, is the improved resolution of the HgI2 detector and its smaller size. The analyser is primarily used for the detection of low levels of heavy metals on particulate filters. The detectors have also been used on an experimental basis for gamma ray backscatter measurements in the medical field.


1981 ◽  
Vol 25 ◽  
pp. 39-44 ◽  
Author(s):  
C. A. N. Conde ◽  
L. F. Requicha Ferreira ◽  
A. J. de Campos

AbstractA review of the basic physical principles of the gas proportional scintillation counter is presented. Its performance is discussed and compared with that of other room-temperature detectors in regard to applications to portable instruments for energy-dispersive X-ray fluorescence analysis. It is concluded that the gas proportional scintillation counter is definitely superior to all other room-temperature detectors, except the mercuric iodide (HgI2) detector. For large areas or soft X-rays it is also superior to the HgI2 detector.


1993 ◽  
Vol 302 ◽  
Author(s):  
P.F. Manfredi

ABSTRACTAfter reviewing the noise limits in room temperature preamplifiers based on discrete elements, the paper discusses some results obtained with monolithic circuits and the perspectives opened-up by active devices directly integrated on the chip of a silicon detector.


1993 ◽  
Vol 302 ◽  
Author(s):  
G. Bertuccio ◽  
P. Rehak ◽  
D.M. Xi

ABSTRACTA new circuital configuration for the charge amplifier is presented. By means of a double feedback loop, the input field-effect transistor can operate with its gate junction sligtly forward biased, collecting the detector current and discharging the feedback capacitor. The feedback resistor is so avoided and no resetting device or circuit is required for the preamplifier operation. The noise is limited by the input transistor, an equivalent noise charge of 19.5 r.m.s. electrons has been measured at room temperature by employing a commercial JFET.


1994 ◽  
Author(s):  
John M. Van Scyoc III ◽  
T. S. Gilbert ◽  
Tuviah E. Schlesinger ◽  
Ralph B. James

2016 ◽  
Vol 62 (3) ◽  
pp. 395-400
Author(s):  
Paweł Grochulski ◽  
Mirosław Cygler ◽  
Brian Yates

After a successful 10 years of operation, the Canadian Macromolecular Crystallography Facility 08ID-1 beamline will undergo an upgrade to establish micro-beam capability. This paper is mostly focussed on optics and computer simulations for ray tracing of the beamline. After completion, the focussed beam at the sample will have a much smaller size of 50 × 5 μm2 (H x V), allowing measurement of X-ray diffraction patterns from much smaller crystals than possible presently. The beamline will be equipped with a fast sample changer and an ultra-low noise photon counting detector, allowing shutter-less operation of the beamline. Additionally, it will be possible to perform in-situ room-temperature experiments.


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