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Confinement and strings in MQCD
We study aspects of confinement in the M-theory fivebrane version of QCD (MQCD). We show heavy quarks are confined in hadrons (which take the form of membrane-fivebrane bound states) for N = 1 and softly broken N = 2 SU( N) MQCD. We explore and clarify the transition from the exotic physics of the l...
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Published in: | Nuclear physics. B 1998-03, Vol.513 (1), p.87-118 |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | We study aspects of confinement in the M-theory fivebrane version of QCD (MQCD). We show heavy quarks are confined in hadrons (which take the form of membrane-fivebrane bound states) for
N = 1 and softly broken
N = 2
SU(
N) MQCD. We explore and clarify the transition from the exotic physics of the latter to the standard physics of the former. In particular, the many strings and quark-antiquark mesons found in
N = 2 field theory by Douglas and Shenker are reproduced. It is seen that in the
N = 1 limit all but one such meson disappears while all of the strings survive. The strings of softly broken
N = 2,
N = 1, and even non-supersymmetric
SU(
N) MQCD have a common ratio for their tensions as a function of the amount of flux they carry. We also comment on the almost BPS properties of the Douglas-Shenker strings and discuss the brane picture for monopole confinement on
N = 2 QCD Higgs branches. |
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ISSN: | 0550-3213 1873-1562 |
DOI: | 10.1016/S0550-3213(97)00651-2 |