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The Chern–Simons one-form and gravity on a fuzzy space
The one-dimensional N × N -matrix Chern–Simons action is given, for large N and for slowly varying fields, by the ( 2 k + 1 ) -dimensional Chern–Simons action S CS , where the gauge fields in S CS parametrize the different ways in which the large N limit can be taken. Since some of these gauge field...
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Published in: | Nuclear physics. B 2006-08, Vol.750 (3), p.321-333 |
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Main Author: | |
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: | The one-dimensional
N
×
N
-matrix Chern–Simons action is given, for large
N
and for slowly varying fields, by the
(
2
k
+
1
)
-dimensional Chern–Simons action
S
CS
, where the gauge fields in
S
CS
parametrize the different ways in which the large
N
limit can be taken. Since some of these gauge fields correspond to the isometries of the space, we argue that gravity on fuzzy spaces can be described by the one-dimensional matrix Chern–Simons action at finite
N
and by the higher dimensional Chern–Simons action when the fuzzy space is approximated by a continuous manifold. |
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ISSN: | 0550-3213 1873-1562 |
DOI: | 10.1016/j.nuclphysb.2006.06.009 |