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Dive into the research topics where S. Krieg is active.

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Featured researches published by S. Krieg.


Science | 2008

Ab Initio Determination of Light Hadron Masses

S. Durr; Z. Fodor; J. Frison; C. Hoelbling; R. Hoffmann; Sandor D. Katz; S. Krieg; T. Kurth; L. Lellouch; Thomas Lippert; Kalman Szabo; G. Vulvert

More than 99% of the mass of the visible universe is made up of protons and neutrons. Both particles are much heavier than their quark and gluon constituents, and the Standard Model of particle physics should explain this difference. We present a full ab initio calculation of the masses of protons, neutrons, and other light hadrons, using lattice quantum chromodynamics. Pion masses down to 190 mega–electron volts are used to extrapolate to the physical point, with lattice sizes of approximately four times the inverse pion mass. Three lattice spacings are used for a continuum extrapolation. Our results completely agree with experimental observations and represent a quantitative confirmation of this aspect of the Standard Model with fully controlled uncertainties.


Physical Review Letters | 2013

Isospin splittings in the light baryon octet from lattice QCD and QED

Sz. Borsanyi; S. Durr; Z. Fodor; Julien Frison; C. Hoelbling; Sandor D. Katz; S. Krieg; Th. Kurth; L. Lellouch; Th. Lippert; Antonin Portelli; Alberto Ramos; Alfonso Sastre; Kalman Szabo

While electromagnetic and up-down quark mass difference effects on octet baryon masses are very small, they have important consequences. The stability of the hydrogen atom against beta decay is a prominent example. Here, we include these effects by adding them to valence quarks in a lattice QCD calculation based on Nf=2+1 simulations with five lattice spacings down to 0.054 fm, lattice sizes up to 6 fm, and average up-down quark masses all the way down to their physical value. This allows us to gain control over all systematic errors, except for the one associated with neglecting electromagnetism in the sea. We compute the octet baryon isomultiplet mass splittings, as well as the individual contributions from electromagnetism and the up-down quark mass difference. Our results for the total splittings are in good agreement with experiment.


Computer Physics Communications | 2005

Numerical methods for the QCD overlap operator: III. Nested iterations

Nigel Cundy; J. van den Eshof; Andreas Frommer; S. Krieg; Thomas Lippert; Katrin Schäfer

The numerical and computational aspects of chiral fermions in lattice quantum chromodynamics are extremely demanding. In the overlap framework, the computation of the fermion propagator leads to a nested iteration where the matrix vector multiplications in each step of an outer iteration have to be accomplished by an inner iteration; the latter approximates the product of the sign function of the hermitian Wilson fermion matrix with a vector. In this paper we investigate aspects of this nested paradigm. We examine several Krylov subspace methods to be used as an outer iteration for both propagator computations and the Hybrid Monte-Carlo scheme. We establish criteria on the accuracy of the inner iteration which allow to preserve an a priori given precision for the overall computation. It will turn out that the accuracy of the sign function can be relaxed as the outer iteration proceeds. Furthermore, we consider preconditioning strategies, where the preconditioner is built upon an inaccurate approximation to the sign function. Relaxation combined with preconditioning allows for considerable savings in computational efforts up to a factor of 4 as our numerical experiments illustrate. We also discuss the possibility of projecting the squared overlap operator into one chiral sector.


Physical Review D | 2012

Nucleon scalar and tensor charges from lattice QCD with light Wilson quarks

Jeremy Green; John W. Negele; Andrew Pochinsky; Sergey Syritsyn; Michael Engelhardt; S. Krieg

We present 2+1 flavor Lattice QCD calculations of the nucleon scalar and tensor charges. Using the BMW clover-improved Wilson action with pion masses between 150 and 350 MeV and three source-sink separations between 0.9 and 1.4 fm, we achieve good control over excited-state contamination and extrapolation to the physical pion mass. As a consistency check, we also present results from calculations using unitary domain wall fermions with pion masses between 300 and 400 MeV, and using domain wall valence quarks and staggered sea quarks with pion masses between 300 and 600 MeV.


Journal of High Energy Physics | 2014

Charmonium spectral functions from 2+1 flavour lattice QCD

Szabolcs Borsanyi; Stephan Dürr; Zoltan Fodor; C. Hoelbling; Sandor D. Katz; S. Krieg; Simon Mages; Daniel Nogradi; Attila Pasztor; A. Schäfer; Kalman Szabo; B. C. Toth; Norbert Trombitás

A bstractFinite temperature charmonium spectral functions in the pseudoscalar and vector channels are studied in lattice QCD with 2+1 flavours of dynamical Wilson quarks, on fine isotropic lattices (with a lattice spacing of 0.057fm), with a non-physical pion mass of mπ ≈ 545 MeV. The highest temperature studied is approximately 1.4Tc. Up to this temperature no significant variation of the spectral function is seen in the pseudoscalar channel. The vector channel shows some temperature dependence, which seems to be consistent with a temperature dependent low frequency peak related to heavy quark transport, plus a temperature independent term at ω > 0. These results are in accord with previous calculations using the quenched approximation.


Physical Review D | 2010

The ratio FK/Fpi in QCD

S. Durr; S. Krieg; Alberto Ramos; C. Hoelbling; Sandor D. Katz; Thomas Lippert; Z. Fodor; Kalman Szabo; L. Lellouch; T. Kurth

We determine the ratio F K /F π in QCD with N f = 2 + 1 flavors of sea quarks, based on a series of lattice calculations with three different lattice spacings, large volumes, and a simulated pion mass reaching down to about 190 MeV. We obtain F K /F π = 1.192(7) stat (6) sys . This result is then used to give an updated value of the Cabibbo-Kobayashi-Maskawa) matrix element |V us |. The unitarity relation for the first row of this matrix is found to be well observed.


Physical Review D | 2014

Nucleon electromagnetic form factors from lattice QCD using a nearly physical pion mass

Jeremy Green; John W. Negele; Andrew Pochinsky; Sergey Syritsyn; Michael Engelhardt; S. Krieg

We present lattice QCD calculations of nucleon electromagnetic form factors using pion masses


Physical Review D | 2015

High-precision calculation of the strange nucleon electromagnetic form factors

Jeremy Green; Stefan Meinel; Michael Engelhardt; S. Krieg; Jesse Laeuchli; John W. Negele; Kostas Orginos; Andrew Pochinsky; Sergey Syritsyn

m_pi


Physical Review D | 2017

Up, down, and strange nucleon axial form factors from lattice QCD

Jeremy Green; Nesreen Hasan; Stefan Meinel; Michael Engelhardt; S. Krieg; Jesse Laeuchli; John W. Negele; Kostas Orginos; Andrew Pochinsky; Sergey Syritsyn

= 149, 202, and 254 MeV and an action with clover-improved Wilson quarks coupled to smeared gauge fields, as used by the Budapest-Marseille-Wuppertal collaboration. Particular attention is given to removal of the effects of excited state contamination by calculation at three source-sink separations and use of the summation and generalized pencil-of-function methods. The combination of calculation at the nearly physical mass


Computer Physics Communications | 2009

Numerical methods for the QCD overlap operator IV: Hybrid Monte Carlo

Nigel Cundy; S. Krieg; Guido Arnold; Andreas Frommer; Thomas Lippert; K. Schilling

m_pi

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Kalman Szabo

University of Wuppertal

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Z. Fodor

Eötvös Loránd University

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C. Hoelbling

University of Wuppertal

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L. Lellouch

Aix-Marseille University

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Thomas Lippert

Forschungszentrum Jülich

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S. Durr

Forschungszentrum Jülich

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Sandor D. Katz

Eötvös Loránd University

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T. Kurth

University of Wuppertal

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Andrew Pochinsky

Massachusetts Institute of Technology

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John W. Negele

Massachusetts Institute of Technology

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