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@ARTICLE{Bali:19009,
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 Schäfer, A. and Schierholz, G. and
Sternbeck, A. and Zanotti, J.M.},
title = {{S}trange and light quark contributions to the nucleon mass
from lattice {QCD}},
journal = {Physical review / D},
volume = {85},
number = {5},
issn = {1550-7998},
address = {[S.l.]},
publisher = {Soc.},
reportid = {PreJuSER-19009},
pages = {054502},
year = {2012},
note = {We thank Peter Bruns and Ludwig Greil for discussion. This
work was supported by the European Union under Grant No.
238353 (ITN STRONGnet) and by the Deutsche
Forschungsgemeinschaft SFB/Transregio 55. Sara Collins
acknowledges support from the Claussen-Simon-Foundation
(Stifterverband fur die Deutsche Wissenschaft). Andre
Sternbeck was supported by the EU International
Reintegration Grant (IRG) No. 256594. James Zanotti was
supported by the Australian Research Council under Grant No.
FT100100005 and previously by the Science and Technology
Facilities Council under Grant No. ST/F009658/1.
Computations were performed on the SFB/TR55 QPACE
supercomputers, the BlueGene/P (JuGene) and the Nehalem
Cluster (JuRoPA) of the Julich Supercomputer Center, the IBM
BlueGene/L at the EPCC (Edinburgh), the SGI Altix ICE
machines at HLRN (Berlin/Hannover), and Regensburg's Athene
HPC cluster. We thank the support staffs of these
institutions. The Chroma software suite [38] was used
extensively in this work and gauge configurations were
generated using the BQCD code [39] on QPACE and BlueGenes.},
abstract = {We determine the strangeness and light quark fractions of
the nucleon mass by computing the quark line connected and
disconnected contributions to the matrix elements m(q)< N
vertical bar(q) over barq vertical bar N > in lattice QCD,
using the nonperturbatively 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 flavors. The
pion-nucleon sigma term is extrapolated to physical quark
masses exploiting the sea quark mass dependence of the
nucleon mass. We obtain the renormalized values sigma(pi N)
= (38 +/- 12) MeV at the physical point and f(Ts) =
sigma(s)/m(N) = 0.012(14)(-3)(+10) for the strangeness
contribution at our larger than physical sea quark mass.},
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 = {Astronomy $\&$ Astrophysics / Physics, Particles $\&$
Fields},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000300937900007},
doi = {10.1103/PhysRevD.85.054502},
url = {https://juser.fz-juelich.de/record/19009},
}