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Spatial geometry of hamiltonian gauge theories
The Hamiltonians of SU(2) and SU(3) gauge theories in 3+1 dimensions can be expressed in terms of gauge invariant spatial geometric variables, i.e., metrics, connections and curvature tensors which are simple local functions of the non-Abelian electric field. The transformed Hamiltonians are local....
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| Lenguaje: | eng |
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1994
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| Acceso en línea: | https://dx.doi.org/10.1016/0920-5632(95)00121-O http://cds.cern.ch/record/267042 |
| _version_ | 1780886733848576000 |
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| author | Freedman, Daniel Z. |
| author_facet | Freedman, Daniel Z. |
| author_sort | Freedman, Daniel Z. |
| collection | CERN |
| description | The Hamiltonians of SU(2) and SU(3) gauge theories in 3+1 dimensions can be expressed in terms of gauge invariant spatial geometric variables, i.e., metrics, connections and curvature tensors which are simple local functions of the non-Abelian electric field. The transformed Hamiltonians are local. New results from the same procedure applied to the SU(2) gauge theory in 2+1 dimensions are also given. |
| id | cern-267042 |
| institution | Organización Europea para la Investigación Nuclear |
| language | eng |
| publishDate | 1994 |
| record_format | invenio |
| spelling | cern-2670422023-03-14T16:35:46Zdoi:10.1016/0920-5632(95)00121-Ohttp://cds.cern.ch/record/267042engFreedman, Daniel Z.Spatial geometry of hamiltonian gauge theoriesGeneral Theoretical PhysicsThe Hamiltonians of SU(2) and SU(3) gauge theories in 3+1 dimensions can be expressed in terms of gauge invariant spatial geometric variables, i.e., metrics, connections and curvature tensors which are simple local functions of the non-Abelian electric field. The transformed Hamiltonians are local. New results from the same procedure applied to the SU(2) gauge theory in 2+1 dimensions are also given.The Hamiltonians of $SU(2)$ and $SU(3)$ gauge theories in 3+1 dimensions can be expressed in terms of gauge invariant spatial geometric variables, i.e., metrics, connections and curvature tensors which are simple local functions of the non-Abelian electric field. The transformed Hamiltonians are local. New results from the same procedure applied to the $SU(2)$ gauge theory in 2+1 dimensions are also given.hep-th/9408052CERN-TH-7391-94CERN-TH-7391-94oai:cds.cern.ch:2670421994-08-09 |
| spellingShingle | General Theoretical Physics Freedman, Daniel Z. Spatial geometry of hamiltonian gauge theories |
| title | Spatial geometry of hamiltonian gauge theories |
| title_full | Spatial geometry of hamiltonian gauge theories |
| title_fullStr | Spatial geometry of hamiltonian gauge theories |
| title_full_unstemmed | Spatial geometry of hamiltonian gauge theories |
| title_short | Spatial geometry of hamiltonian gauge theories |
| title_sort | spatial geometry of hamiltonian gauge theories |
| topic | General Theoretical Physics |
| url | https://dx.doi.org/10.1016/0920-5632(95)00121-O http://cds.cern.ch/record/267042 |
| work_keys_str_mv | AT freedmandanielz spatialgeometryofhamiltoniangaugetheories |