% 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{Bauer:201172,
author = {Bauer, G. S.},
title = {{O}verview on spallation target design concepts and related
materials issues},
journal = {Journal of nuclear materials},
volume = {398},
number = {1-3},
issn = {0022-3115},
address = {Amsterdam [u.a.]},
publisher = {Elsevier Science},
reportid = {FZJ-2015-03477},
pages = {19 - 27},
year = {2010},
abstract = {From a modest beginning of a few kW of beam power
spallation sources have now evolved into systems that must
be able to handle several MW, mostly delivered in short
pulses of less than microsecond duration. The high radiation
field and high instantaneous heat deposition which
spallation targets, in particular for the new high power
sources, are subject to have led to several different design
concepts which aim at circumventing or reducing the
deleterious effects on the materials in the targets.
Efficient cooling and high neutron source density are
competing requirements which can be best reconciled by
moving the target material out of the reaction zone and
removing the heat elsewhere before returning the material
back into the proton beam. One option is the use of a
flowing liquid metal, which has been the method of choice in
most of the recent spallation source designs, but requires
solutions to a variety of new problems, such as liquid metal
corrosion, cavitation erosion and e.g. in the case of PbBi,
or Pb, high temperature gradients. Using a rotating solid
target is an option in certain cases but still has to cope
with the instantaneous load levels. While it may help to
keep the average heat load and radiation damage in the
target material low and thus extend the target life time by
more than an order of magnitude, it still has its own design
and materials issues. Opportunities to carry out research in
this field are rather limited because the effects can hardly
be simulated off line and, apart from spallation targets in
operation, almost no facilities are available.},
cin = {JCNS-2 / PGI-4 / JARA-FIT},
ddc = {530},
cid = {I:(DE-Juel1)JCNS-2-20110106 / I:(DE-Juel1)PGI-4-20110106 /
$I:(DE-82)080009_20140620$},
pnm = {422 - Spin-based and quantum information (POF2-422) / 424 -
Exploratory materials and phenomena (POF2-424) / 542 -
Neutrons (POF2-542) / 544 - In-house Research with PNI
(POF2-544) / 54G - JCNS (POF2-54G24)},
pid = {G:(DE-HGF)POF2-422 / G:(DE-HGF)POF2-424 /
G:(DE-HGF)POF2-542 / G:(DE-HGF)POF2-544 /
G:(DE-HGF)POF2-54G24},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000276533100005},
doi = {10.1016/j.jnucmat.2009.10.005},
url = {https://juser.fz-juelich.de/record/201172},
}