dc.contributor.author |
ANANTH, SUDARSHAN |
en_US |
dc.contributor.author |
Brink, Lars |
en_US |
dc.contributor.author |
MALI, MAHENDRA |
en_US |
dc.date.accessioned |
2019-03-15T11:25:58Z |
|
dc.date.available |
2019-03-15T11:25:58Z |
|
dc.date.issued |
2015-08 |
en_US |
dc.identifier.citation |
Journal of High Energy Physics, 2015,153. |
en_US |
dc.identifier.issn |
1126-6708 |
en_US |
dc.identifier.issn |
1029-8479 |
en_US |
dc.identifier.uri |
http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/2258 |
|
dc.identifier.uri |
https://doi.org/10.1007/JHEP08(2015)153 |
en_US |
dc.description.abstract |
We show that the Hamiltonian of ( N=1 , d = 10) super Yang-Mills can be expressed as a quadratic form in a very similar manner to that of the ( N=4 , d = 4) theory. We find a similar quadratic form structure for pure Yang-Mills theory but this feature, in the non-supersymmetric case, seems to be unique to four dimensions. We discuss some consequences of this feature |
en_US |
dc.language.iso |
en |
en_US |
dc.publisher |
Springer Nature |
en_US |
dc.subject |
Yang-Mills |
en_US |
dc.subject |
Quadratic forms |
en_US |
dc.subject |
Supersymmetric gauge theory |
en_US |
dc.subject |
Extended Supersymmetry |
en_US |
dc.subject |
Field Theories |
en_US |
dc.subject |
Higher Dimensions |
en_US |
dc.subject |
2015 |
en_US |
dc.title |
Yang-Mills theories and quadratic forms |
en_US |
dc.type |
Article |
en_US |
dc.contributor.department |
Dept. of Physics |
en_US |
dc.identifier.sourcetitle |
Journal of High Energy Physics |
en_US |
dc.publication.originofpublisher |
Foreign |
en_US |