{ "id": "hep-th/9711179", "version": "v2", "published": "1997-11-24T20:14:01.000Z", "updated": "1998-10-07T13:23:35.000Z", "title": "Matrix Theory, U-Duality and Toroidal Compactifications of M-Theory", "authors": [ "C. M. Hull" ], "comment": "28 Pages, Phyzzx Macro. Minor corrections", "journal": "JHEP 9810:011,1998", "doi": "10.1088/1126-6708/1998/10/011", "categories": [ "hep-th" ], "abstract": "Using U-duality, the properties of the matrix theories corresponding to the compactification of M-theory on $T^d$ are investigated. The couplings of the $d+1$ dimensional effective Super-Yang-Mills theory to all the M-theory moduli is deduced and the spectrum of BPS branes in the SYM gives the corresponding spectrum of the matrix theory.Known results are recovered for $d\\le 5$ and predictions for $d>5$ are proposed. For $d>3$, the spectrum includes $d-4$ branes arising from YM instantons, and U-duality interchanges momentum modes with brane wrapping modes.For $d=6$, there is a generalised $\\th $-angle which couples to instantonic 3-branes and which combines with the SYM coupling constant to take values in $SL(2,\\R)/U(1)$, acted on by an $SL(2,\\Z)$ subgroup of the U-duality group $E_6(\\Z)$. For $d=4,7,8$, there is an $SL(d+1)$ symmetry, suggesting that the matrix theory could be a scale-invariant $d+2$ dimensional theory on $T^{d+1} \\times \\R$ in these cases, as is already known to be the case for $d=4$; evidence is found suggesting this happens for $d=8$ but not $d=7$.", "revisions": [ { "version": "v2", "updated": "1998-10-07T13:23:35.000Z" } ], "analyses": { "keywords": [ "matrix theory", "toroidal compactifications", "u-duality interchanges momentum modes", "dimensional effective super-yang-mills theory", "bps branes" ], "tags": [ "journal article" ], "publication": { "publisher": "IOP", "journal": "J. High Energ. Phys." }, "note": { "typesetting": "TeX", "pages": 28, "language": "en", "license": "arXiv", "status": "editable", "inspire": 451504 } } }