NUCLEAR
Nuclear Physics B389 (1993) 445—510 P H Y S I CS B
North-Holland ________________
The hadron spectrum in QCD with dynamical
staggered fermions
The MT~ Collaboration
R. Altmeyer a,b K.D. Born a M. Göckeler a,c R. Horsley a,c E. Laermann cd
and G. Schierholz b,c
a Inst itut für Theoretische Physik, RWTHAachen, Sommerfeldstrasse, D-5100 Aachen, Germany
b Deutsches Elektronen-Synchrotron DESY Notkestrasse 85, D-2000 Hamburg 52, Germany
Gruppe Theorie der Elementarteilchen, Höchstleistungsrechenzentrum HLRZ,
c / o Forschungszentrum Jülich, D-51 70 Jülich, Germany
a Fakultât für Physik, Unit ersitàt Bielefeld, Postfach 8640, D-4800 Bielefeld 1, Germany
Received 14 April 1992
(Revised 15 July 1992)
Accepted for publication 4 August 1992
The hadron spectrum has been calculated in a large scale simulation of QCD with dynamical
staggered fermions on a 16~ ~‘<24 lattice at m = 0.01 and /3 = 5.35 and 5.15. Special emphasis is
placed on flavour symmetry restoration, for which we observe a substantial improvement
between the two /3-values. The results at the lower /3-value provide a scale for the critical
temperature on an eight time slice lattice. In addition to the spectrum we investigate chiral
properties and calculate the chiral condensate and f,~ in the chiral limit.
1. Introduction
As is well known, the only way to compute the low-energy properties of QCD
from first principles is by means of the lattice regularization and numerical
simulations. The drawback of this method is that it breaks almost all continuous
symmetries, and only for small enough lattice constants can one hope that the
broken symmetries will get restored dynamically. It is therefore important to
compute, first of all, the known masses and matrix elements of the low-lying
hadron states and to demonstrate the correctness of the lattice techniques. It is
needless to say that the successful calculation of these quantities would also
provide a major test of QCD.
In this paper we describe a lattice QCD calculation of the hadron spectrum with
four flavours of dynamical staggered fermions. The calculation is done on a
16~x 24 lattice using the exact hybrid Monte Carlo algorithm for 13 = 5.35 and
5.15. We differ from other recent large-scale hadron-mass calculations [1—4] either
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