Preliminary Results From A Single-Photon Imaging X-Ray Charge Coupled Device (CCD) Camera

Author(s):  
R. E. Griffiths ◽  
G. Polucci ◽  
A. Mak ◽  
S. S. Murray ◽  
D. A. Schwartz ◽  
...  
2004 ◽  
Vol 75 (10) ◽  
pp. 3705-3707 ◽  
Author(s):  
C. Stoeckl ◽  
W. Theobald ◽  
T. C. Sangster ◽  
M. H. Key ◽  
P. Patel ◽  
...  

2013 ◽  
Vol 11 (11) ◽  
pp. 110401-110404 ◽  
Author(s):  
Yonghong Yan Yonghong Yan ◽  
Lai Wei Lai Wei ◽  
Xianlun Wen Xianlun Wen ◽  
Yuchi Wu Yuchi Wu ◽  
Zongqing Zhao Zongqing Zhao ◽  
...  

1997 ◽  
Vol 7 (2) ◽  
pp. 3383-3386 ◽  
Author(s):  
S. Friedrich ◽  
K. Segall ◽  
M.C. Gaidis ◽  
C.M. Wilson ◽  
D.E. Prober ◽  
...  

2015 ◽  
Vol 22 (3) ◽  
pp. 729-735 ◽  
Author(s):  
M. P. Hertlein ◽  
A. Scholl ◽  
A. A. Cordones ◽  
J. H. Lee ◽  
K. Engelhorn ◽  
...  

Laser pump–X-ray probe experiments require control over the X-ray pulse pattern and timing. Here, the first use of pseudo-single-bunch mode at the Advanced Light Source in picosecond time-resolved X-ray absorption experiments on solutions and solids is reported. In this mode the X-ray repetition rate is fully adjustable from single shot to 500 kHz, allowing it to be matched to typical laser excitation pulse rates. Suppressing undesired X-ray pulses considerably reduces detector noise and improves signal to noise in time-resolved experiments. In addition, dose-induced sample damage is considerably reduced, easing experimental setup and allowing the investigation of less robust samples. Single-shot X-ray exposures of a streak camera detector using a conventional non-gated charge-coupled device (CCD) camera are also demonstrated.


2007 ◽  
Vol 78 (10) ◽  
pp. 103506 ◽  
Author(s):  
L. Labate ◽  
A. Giulietti ◽  
D. Giulietti ◽  
P. Köster ◽  
T. Levato ◽  
...  

2011 ◽  
Vol 681 ◽  
pp. 1-6 ◽  
Author(s):  
Denis Bouscaud ◽  
Raphaël Pesci ◽  
Sophie Berveiller ◽  
Etienne Patoor

A Kossel microdiffraction experimental set up is under development inside a Scanning Electron Microscope (SEM) in order to determine the crystallographic orientation as well as the inter- and intragranular strains and stresses. An area of about one cubic micrometer can be analysed using the microscope probe, which enables to study different kinds of elements such as a grain boundary, a crack, a microelectronic component, etc. The diffraction pattern is recorded by a high resolution Charge-Coupled Device (CCD) camera. The crystallographic orientation, the lattice parameters and the elastic strain tensor of the probed area are deduced from the pattern indexation using a homemade software. The purpose of this paper is to report some results achieved up to now to estimate the reliability of the Kossel microdiffraction technique.


2019 ◽  
Vol 90 (4) ◽  
pp. 043111 ◽  
Author(s):  
Andrea Lübcke ◽  
Julia Braenzel ◽  
Aurelie Dehlinger ◽  
Matthias Schnürer ◽  
Holger Stiel ◽  
...  

2001 ◽  
Vol 90 (7) ◽  
pp. 3645-3647 ◽  
Author(s):  
L. Li ◽  
L. Frunzio ◽  
C. Wilson ◽  
D. E. Prober ◽  
A. E. Szymkowiak ◽  
...  

1981 ◽  
Vol 4 (2) ◽  
pp. 195-197
Author(s):  
C. D. Mackay ◽  
D. Astili ◽  
M. J. Batty ◽  
D. L. Jauncey ◽  
A. E. Wright ◽  
...  

We present preliminary results from a programme designed to produce deep images of radio source fields drawn from the Parkes 2700 MHz and Molongolo 408 MHz catalogues using the charge-coupled-device (CCD) camera system built at the Institute of Astronomy, Cambridge. The programme is directed at a search both for faint extensions and nebulosity around radio QSOs and BL Lac objects and for faint objects in otherwise empty radio source fields; a detailed examination of the morphology of selected radio galaxies is also included.


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