1998
DOI: 10.1016/s0550-3213(98)00013-3
|View full text |Cite
|
Sign up to set email alerts
|

Supersymmetric Yang-Mills theory and Riemannian Geometry

Abstract: We introduce new local gauge invariant variables for N = 1 supersymmetric Yang-Mills theory, explicitly parameterizing the physical Hilbert space of the theory. We show that these gauge invariant variables have a geometrical interpretation, and can be constructed such that the emergent geometry is that of N = 1 supergravity: a Riemannian geometry with vector-spinor generated torsion. Full geometrization of supersymmetric Yang-Mills theory is carried out, and geometry independent divergences associated to the i… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

0
4
0

Year Published

2000
2000
2014
2014

Publication Types

Select...
5

Relationship

0
5

Authors

Journals

citations
Cited by 7 publications
(4 citation statements)
references
References 21 publications
0
4
0
Order By: Relevance
“…I have presented here a method by which the Gauss law (8) can be solved in the case of the SU(3) algebra using the ansatz (9). The fact that the l.h.s.…”
Section: Discussionmentioning
confidence: 99%
“…I have presented here a method by which the Gauss law (8) can be solved in the case of the SU(3) algebra using the ansatz (9). The fact that the l.h.s.…”
Section: Discussionmentioning
confidence: 99%
“…Towards the end of the nineties Schiappa adapted these local gauge-invariant variables for supersymmetric gauge theory [41]. An independent variation of this school was pursued by Slizovskiy and Niemi [38].…”
Section: The Hidden-spatial-geometry Schoolmentioning
confidence: 99%
“…The second school uses a Grassmannian manifold to represent gauge fields using a type of gauge-theory embedding [35,36,3,13,15,17,9,11,10,49,5,6,47,48,51,44,45,22,16,21,14,4,39,12] [ 34,27,30]. The third school introduces alternative variables for gauge theory that uncover a hidden spatial metric which reproduces the gauge fields [23,19,20,33,28,29,41,38,53]. Each of the schools start with a different geometrical representation which then faithfully maps onto the traditional gauge fields A µ .…”
Section: Introductionmentioning
confidence: 99%
“…If we define J ai by (18), any solution of (27) satisfies the equations of motion (5) by the identification (22). Moreover, if the energy momentum tensor (25) satisfies the conservation law ∇ i T ij = 0, the solution of the equation ( 27) also satisfies the Bianchi identity (6).…”
mentioning
confidence: 99%