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@ARTICLE{Bali:21703,
author = {Bali, G.S. and Collins, S. and Göckeler, M. and Horsley,
R. and Nakamura, Y. and Nobile, A. and Pleiter, D. and
Rakow, P.E.L. and Sternbeck, A. and Schäfer, A. and
Schierholz, G. and Zanotti, J.M.},
title = {{A} lattice study of the strangeness content of the
nucleon},
journal = {Progress in particle and nuclear physics},
volume = {67},
issn = {0146-6410},
address = {Oxford [u.a.]},
publisher = {Pergamon Press},
reportid = {PreJuSER-21703},
pages = {467 - 472},
year = {2012},
note = {This work was supported by the European Union (grant
238353, ITN STRONGnet) and by the DFG SFB/Transregio 55.
S.C. is supported by the Claussen-Simon-Foundation
(Stifterverband fur die Deutsche Wissenschaft), A.St. by the
EU IRG grant 256594 and J.Z. by the Australian Research
Council grant FT100100005. Computations were performed on
the SFB/TR55 QPACE supercomputers, the BlueGene/P (JuGene)
and the Nehalem cluster (JuRoPA) of the JSC (Julich), the
IBM BlueGene/L at the EPCC (Edinburgh), the SGI Altix ICE
machines at HLRN (Berlin/Hannover) and Regensburg's Athene
HPC cluster. The Chroma software suite [24] was used
extensively in this work.},
abstract = {We determine the quark contributions to the nucleon spin
Delta s, Delta u and Ad as well as their contributions to
the nucleon mass, the a-terms. This is done by computing
both, the quark line connected and disconnected
contributions to the respective matrix elements, using the
non-perturbatively improved Sheikholeslami-Wohlert Wilson
Fermionic action. We simulate n(F) = 2 mass degenerate sea
quarks with a pion mass of about 285 MeV and a lattice
spacing a approximate to 0.073 fm. The renormalization of
the matrix elements involves mixing between contributions
from different quark flavours. The pion-nucleon a-term is
extrapolated to physical quark masses exploiting the sea
quark mass dependence of the nucleon mass. We obtain the
renormalized value sigma(pi N) = (38 +/- 12) MeV at the
physical point and the strangeness fraction f(Ts) = sigma
s/m(N) = 0.012(14)(-3)(+10) at our larger than physical sea
quark mass. For the strangeness contribution to the nucleon
spin we obtain Delta s ((MS)) over bar(root 7.4 GeV) =
-0.020(10)(1). (C) 2012 Published by Elsevier B.V.},
keywords = {J (WoSType)},
cin = {JSC},
ddc = {530},
cid = {I:(DE-Juel1)JSC-20090406},
pnm = {Scientific Computing (FUEK411) / 411 - Computational
Science and Mathematical Methods (POF2-411) / STRONGNET -
Strong Interaction Supercomputing Training Network (238353)
/ PRECISION LATTICEQCD - Precision lattice QCD calculations
(256594)},
pid = {G:(DE-Juel1)FUEK411 / G:(DE-HGF)POF2-411 /
G:(EU-Grant)238353 / G:(EU-Grant)256594},
shelfmark = {Physics, Nuclear / Physics, Particles $\&$ Fields},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000303282200062},
doi = {10.1016/j.ppnp.2012.01.012},
url = {https://juser.fz-juelich.de/record/21703},
}