1123581321 Posted October 28, 2010 Share Posted October 28, 2010 I was wondering, is supergravity the result of adding supersymmetry to the graviton... Link to comment Share on other sites More sharing options...
timo Posted October 28, 2010 Share Posted October 28, 2010 That is one (very informal) way to think of it. In practice, I've never seen symmetries being introduced to an already-quantized model, so at the point where susy comes in, no such thing as the graviton exists in the theory, but only some crude notion of "gravity", at best. Supersymmetry is kind of special in an additional way since it already is an extended version of the concept which (in naive approaches) later gives rise to gravitons. It's more like supergravity being the result of adding gravitons to supersymmetry. Link to comment Share on other sites More sharing options...
ajb Posted October 29, 2010 Share Posted October 29, 2010 A much better way to think of supergravity is as the localisation or gauging of supersymmetry. Doing so almost automatically gives you a supersymmetric theory that includes gravity. Link to comment Share on other sites More sharing options...
Severian Posted October 29, 2010 Share Posted October 29, 2010 Yes, that is how I think of it. Local supersymmetry. In fact, it is so elegant, I find it hard to believe that it is not correct (at least on some level). Link to comment Share on other sites More sharing options...
1123581321 Posted October 29, 2010 Author Share Posted October 29, 2010 what is 'gauge' in physics, or a least in the sense that it is being used... Link to comment Share on other sites More sharing options...
ajb Posted October 29, 2010 Share Posted October 29, 2010 what is 'gauge' in physics, or a least in the sense that it is being used... You have global and local symmetries. Global: No dependence on the location on spacetime. Local: Dependence of the location on spacetime. To make sense of local symmetries an extra field is required: a gauge field. This field can be though of as compensating for the "ill effects" that arise when you make the symmetry depend on the location. More technically, gauge fields allow us to construct covariant derivatives. When localising supersymmetry we have to introduce the graviton and it's superpartner the gravitino. Link to comment Share on other sites More sharing options...
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