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| | The Poincaré Group is the full set of transformations which leave the spacetime interval invariant. Just as in 3-dimensional space distance is preserved by translations and rotations, so in Minkowski space the transformations of the Poincaré Group preserve the spacetime interval. | | The Poincaré Group is the full set of transformations which leave the spacetime interval invariant. Just as in 3-dimensional space distance is preserved by translations and rotations, so in Minkowski space the transformations of the Poincaré Group preserve the spacetime interval. |
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| − | There are ten basic transformations in the Poincaré Group, and all other transformations may be written as combinations of these (for example, a translation followed by a rotation). In the language of [[group theory]], these ten elements are said to be [[generator|generators]] of the Poincaré Group, which thus has the structure of a ten-dimensional [[Lie group]]. Six of these are the familiar translations and rotations of space. In additional to translations of time, the Poincaré Group has three additional generators, corresponding to the Lorentz transformations. | + | There are ten basic transformations in the Poincaré Group, and all other transformations may be written as combinations of these (for example, a translation followed by a rotation). In the language of [[group theory]], these ten elements are said to be [[generator]]s of the Poincaré Group, which thus has the structure of a ten-dimensional [[Lie group]]. Six of these are the familiar translations and rotations of space. In additional to translations of time, the Poincaré Group has three additional generators, corresponding to the Lorentz transformations. |
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| − | ===Spatial translations===
| + | ==Spatial translations== |
| | *<math>T_x : (x, y, z, ct) = (x + \epsilon , y, z, ct)</math> | | *<math>T_x : (x, y, z, ct) = (x + \epsilon , y, z, ct)</math> |
| | *<math>T_y : (x, y, z, ct) = (x, y + \epsilon , z, ct)</math> | | *<math>T_y : (x, y, z, ct) = (x, y + \epsilon , z, ct)</math> |
| | *<math>T_z : (x, y, z, ct) = (x, y, z + \epsilon , ct)</math> | | *<math>T_z : (x, y, z, ct) = (x, y, z + \epsilon , ct)</math> |
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| − | ===Time Translations===
| + | ==Time Translations== |
| | *<math>T_t : (x, y, z, ct) = (x, y, z, ct + \epsilon )</math> | | *<math>T_t : (x, y, z, ct) = (x, y, z, ct + \epsilon )</math> |
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| − | ===Spatial Rotations===
| + | ==Spatial Rotations== |
| | *<math>R_x : (x, y, z, ct) = (x, cos \theta y + sin \theta z, - sin \theta y + cos \theta y, ct)</math> | | *<math>R_x : (x, y, z, ct) = (x, cos \theta y + sin \theta z, - sin \theta y + cos \theta y, ct)</math> |
| | *<math>R_y : (x, y, z, ct) = (cos \theta x + sin \theta z, y, - sin \theta x + cos \theta z, ct)</math> | | *<math>R_y : (x, y, z, ct) = (cos \theta x + sin \theta z, y, - sin \theta x + cos \theta z, ct)</math> |
| | *<math>R_z : (x, y, z, ct) = (cos \theta x + sin \theta y, - sin \theta x + sin \theta y, z, ct)</math> | | *<math>R_z : (x, y, z, ct) = (cos \theta x + sin \theta y, - sin \theta x + sin \theta y, z, ct)</math> |
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| − | ===Lorentzian Transformations===
| + | ==Lorentzian Transformations== |
| | *<math>L_x : (x, y, z, ct) = (x', y, z, ct')</math> | | *<math>L_x : (x, y, z, ct) = (x', y, z, ct')</math> |
| | *<math>L_y : (x, y, z, ct) = (x, y', z, ct')</math> | | *<math>L_y : (x, y, z, ct) = (x, y', z, ct')</math> |