Article ID | Journal | Published Year | Pages | File Type |
---|---|---|---|---|
10720811 | Nuclear Physics B | 2013 | 42 Pages |
Abstract
The use of chirally rotated boundary conditions provides a formulation of the Schrödinger functional that is compatible with automatic O(a) improvement of Wilson fermions up to O(a) boundary contributions. The elimination of bulk O(a) effects requires the non-perturbative tuning of the critical mass and one additional boundary counterterm. We present the results of such a tuning in a quenched setup for several values of the renormalized gauge coupling, from perturbative to non-perturbative regimes, and for a range of lattice spacings. We also check that the correct boundary conditions and symmetries are restored in the continuum limit.
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Physical Sciences and Engineering
Mathematics
Mathematical Physics
Authors
J. González López, K. Jansen, D.B. Renner, A. Shindler,