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@ARTICLE{Bernauer:301920,
author = {Bernauer, Jan and Diefenbach, J. and Elbakian, G. and
Gavrilov, G. and Goerrissen, N. and Hasell, Douglas and
Henderson, Brian and Holler, Yorck and Karyan, Gevorg and
Ludwig, Joerg and Marukyan, H. and Naryshkin, Youri and
O'Connor, C. and Russell, Rebecca and Schmidt, Axel and
Schneekloth, U. and Suvorov, K. and Veretennikov, D.},
title = {{M}easurement and tricubic interpolation of the magnetic
field for the {OLYMPUS} experiment},
journal = {Nuclear instruments $\&$ methods in physics research / A},
volume = {823},
issn = {0168-9002},
address = {Amsterdam},
publisher = {North-Holland Publ. Co.},
reportid = {PUBDB-2016-02977},
pages = {9 - 14},
year = {2016},
note = {(c) Elsevier B.V. The arxiv v1 version matches with the
post referee version.},
abstract = {The OLYMPUS experiment used a 0.3T toroidal magnetic
spectrometer to measure the momenta of outgoing charged
particles. In order to accurately determine particle
trajectories, knowledge of the magnetic field was needed
throughout the spectrometer volume. For that purpose, the
magnetic field was measured at over 36,000 positions using a
three-dimensional Hall probe actuated by a system
oftranslation tables. We used these field data to fit a
numerical magnetic field model, which could be employed to
calculate the magnetic field at any point in the
spectrometer volume. Calculations with this model were
computationally intensive; for analysis applications where
speed was crucial, we pre-computed the magnetic field and
its derivatives on an evenly spaced grid so that the field
could be interpolated between grid points. We developed a
spline-based interpolation scheme suitable for SIMD
implementations, with a memory layout chosen to minimize
space and optimize the cache behavior to quickly calculate
field values.This scheme requires only one-eighth of the
memory needed to storenecessary coefficients compared with a
previous scheme (Lekien and Marsden, 2005 [1]). This method
was accurate for the vast majority of the spectrometer
volume, though special fits and representations were needed
to improve the accuracy close to the magnet coils and along
the toroidal axis.},
cin = {OLYMP},
ddc = {530},
cid = {I:(DE-H253)OLYMP-20120731},
pnm = {611 - Fundamental Particles and Forces (POF3-611)},
pid = {G:(DE-HGF)POF3-611},
experiment = {EXP:(DE-H253)OLYMPUS-20150101},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000374661600002},
doi = {10.1016/j.nima.2016.03.115},
url = {https://bib-pubdb1.desy.de/record/301920},
}