% IMPORTANT: The following is UTF-8 encoded. This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.
@ARTICLE{Zhang:172372,
author = {Zhang, J. and Fretwurst, E. and Graafsma, H. and Klanner,
R. and Kopsalis, I. and Schwandt, J.},
title = {{S}tudy of {X}-ray radiation damage in the {AGIPD} sensor
for the {E}uropean {XFEL}},
journal = {Journal of Instrumentation},
volume = {9},
number = {05},
issn = {1748-0221},
address = {London},
publisher = {Inst. of Physics},
reportid = {PUBDB-2014-03701},
pages = {C05022},
year = {2014},
note = {Part of 15th International Workshop on Radiation Imaging
Detectors (IWORID2013)},
abstract = {The European X-ray Free Electron Laser (XFEL), currently
being constructed in Hamburg and planned to be operational
in 2017 for users, will deliver 27,000 fully coherent, high
brilliance X-ray pulses per second with duration less than
100 fs. The unique features of the X-ray beam pose major
challenges for silicon detectors used at the European XFEL
for imaging experiments, in particular a radiation tolerance
of silicon sensors for doses up to 1 GGy for 3 years of
operation at an operating voltage above 500 V.One of the
detectors under development at the European XFEL is the
Adaptive Gain Integrating Pixel Detector (AGIPD), which is a
hybrid detector system with ASICs bump-bonded to p+n silicon
pixel sensors. We have designed the silicon sensors for the
AGIPD, which have been fabricated by SINTEF and delivered in
the beginning of February 2013. To demonstrate the
performance of the AGIPD sensor with regard to radiation
hardness, mini-sensors with the same pixel and guard-ring
designs as the AGIPD together with test structures have been
irradiated at the beamline P11 of PETRA III with 8 keV and
12 keV monoenergetic X-rays to dose values up to 10 MGy. The
radiation hardness of the AGIPD sensor has been proven and
all electrical properties are within specification before
and after irradiation. In addition, the oxide-charge density
and surface-current density from test structures have been
characterized as function of the X-ray dose and compared to
previous measurements for test structures produced by four
vendors.},
cin = {DOOR / FS-DS / UNI/EXP / FS-PE},
ddc = {610},
cid = {I:(DE-H253)HAS-User-20120731 / I:(DE-H253)FS-DS-20120731 /
$I:(DE-H253)UNI_EXP-20120731$ / I:(DE-H253)FS-PE-20120731},
pnm = {PETRA Beamline P11 (POF2-54G14)},
pid = {G:(DE-H253)POF2-P11-20130405},
experiment = {EXP:(DE-H253)P-P11-20150101},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000340036100022},
doi = {10.1088/1748-0221/9/05/C05022},
url = {https://bib-pubdb1.desy.de/record/172372},
}