Mid Sweden University

miun.sePublications
Change search
CiteExportLink to record
Permanent link

Direct link
Cite
Citation style
  • apa
  • ieee
  • modern-language-association-8th-edition
  • vancouver
  • Other style
More styles
Language
  • de-DE
  • en-GB
  • en-US
  • fi-FI
  • nn-NO
  • nn-NB
  • sv-SE
  • Other locale
More languages
Output format
  • html
  • text
  • asciidoc
  • rtf
The high speed, high dynamic range camera AGIPD
Deutsches Elektronen-Synchrotron DESY, 22607 Hamburg, Germany .
Deutsches Elektronen-Synchrotron DESY, 22607 Hamburg, Germany .
Deutsches Elektronen-Synchrotron DESY, 22607 Hamburg, Germany .
Mid Sweden University, Faculty of Science, Technology and Media, Department of Electronics Design.
Show others and affiliations
2013 (English)In: IEEE Nuclear Science Symposium Conference Record, IEEE conference proceedings, 2013, p. Art. no. 6829504-Conference paper, Published paper (Refereed)
Abstract [en]

The European X-Ray Free Electron Laser (XFEL) will provide ultra short, highly coherent X-ray pulses which will revolutionize scientific experiments in a variety of disciplines spanning physics, chemistry, materials science, and biology. One of the differences between the European XFEL and other free electron laser sources is the high pulse frequency of 4.5 MHz. The European XFEL will provide pulse trains, consisting of up to 2700 pulses separated by 220 ns (600 μs in total) followed by an idle time of 99.4 ms, resulting in a supercycle of 10 Hz. Dedicated fast 2D detectors are being developed, one of which is the Adaptive Gain Integrating Pixel Detector (AGIPD). AGIPD is based on the hybrid pixel technology. The design goals of the recently produced, radiation hard Application Specific Integrated Circuit (ASIC) with dynamic gain switching amplifiers are (for each pixel) a dynamic range of more than 10 4 12.4 keV photons in the lowest gain, single photon sensitivity in the highest gain, an analog memory capable of storing 352 images, and operation at 4.5 MHz frame rate. A vetoing scheme allows to maximize the number of useful images that are acquired by providing the possibility to overwrite any previously recorded image during the pulse train. The AGIPD will feature a pixel size of (200 μm)2 and a silicon sensor with a thickness of 500 μm. The image data is read out and digitized between pulse trains. © 2013 IEEE.

Place, publisher, year, edition, pages
IEEE conference proceedings, 2013. p. Art. no. 6829504-
Series
IEEE Nuclear Science Symposium Conference Record, ISSN 1095-7863
Keywords [en]
2D detector, AGIPD, Hybrid Pixel Detector, XFEL
National Category
Electrical Engineering, Electronic Engineering, Information Engineering
Identifiers
URN: urn:nbn:se:miun:diva-22612DOI: 10.1109/NSSMIC.2013.6829504Scopus ID: 2-s2.0-84904203753ISBN: 9781479905348 (print)OAI: oai:DiVA.org:miun-22612DiVA, id: diva2:754609
Conference
2013 60th IEEE Nuclear Science Symposium and Medical Imaging Conference, NSS/MIC 2013; Seoul; South Korea; 27 October 2013 through 2 November 2013; Category numberCFP13NSS-ART; Code 106171
Note

CODEN: 85OQA

Available from: 2014-10-10 Created: 2014-08-20 Last updated: 2021-04-29Bibliographically approved

Open Access in DiVA

No full text in DiVA

Other links

Publisher's full textScopus

Authority records

Graafsma, Heinz

Search in DiVA

By author/editor
Graafsma, Heinz
By organisation
Department of Electronics Design
Electrical Engineering, Electronic Engineering, Information Engineering

Search outside of DiVA

GoogleGoogle Scholar

doi
isbn
urn-nbn

Altmetric score

doi
isbn
urn-nbn
Total: 519 hits
CiteExportLink to record
Permanent link

Direct link
Cite
Citation style
  • apa
  • ieee
  • modern-language-association-8th-edition
  • vancouver
  • Other style
More styles
Language
  • de-DE
  • en-GB
  • en-US
  • fi-FI
  • nn-NO
  • nn-NB
  • sv-SE
  • Other locale
More languages
Output format
  • html
  • text
  • asciidoc
  • rtf