Difference between revisions of "Poincare group"

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The Poincaré Group consists of 10 [[Mathematics|mathematical]] transformations that can be applied to different coordinates of the [[space]]-[[time]] graph (x, y, z, ct), but do not affect the "spacetime interval". The "spacetime interval" is roughly the 4-D equivalent of 3-D "distance".
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The '''Poincaré Group''' consists of 10 [[Mathematics|mathematical]] transformations that can be applied to different coordinates of the [[space]]-[[time]] graph (x, y, z, ct), but do not affect the "spacetime interval". The "spacetime interval" is roughly the 4-D equivalent of 3-D "distance".
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<br><br>
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The Poincaré Group is a "symmetry group" because the spacetime interval remains invariant.
 
The Poincaré Group is a "symmetry group" because the spacetime interval remains invariant.
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<br><br>
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These transformations are:
 
These transformations are:
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<br><br>
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Spatial translations:
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===Spatial translations===
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<br> <math>T_x : (x, y, z, ct) = (x + \epsilon , y, z, ct)</math>
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*<math>T_x : (x, y, z, ct) = (x + \epsilon , y, z, ct)</math>
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<br> <math>T_y : (x, y, z, ct) = (x, y + \epsilon , z, ct)</math>
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*<math>T_y : (x, y, z, ct) = (x, y + \epsilon , z, ct)</math>
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<br> <math>T_z : (x, y, z, ct) = (x, y, z + \epsilon , ct)</math>
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*<math>T_z : (x, y, z, ct) = (x, y, z + \epsilon , ct)</math>
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<br><br>
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Time Translations:
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===Time Translations===
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<br> <math>T_t : (x, y, z, ct) = (x, y, z, ct + \epsilon )</math>
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*<math>T_t : (x, y, z, ct) = (x, y, z, ct + \epsilon )</math>
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<br><br>
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Spatial Rotations:
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===Spatial Rotations===
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<br> <math>R_x : (x, y, z, ct) = (x, cos \theta y + sin \theta z, - sin \theta y + cos \theta y, ct)</math>
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*<math>R_x : (x, y, z, ct) = (x, cos \theta y + sin \theta z, - sin \theta y + cos \theta y, ct)</math>
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<br> <math>R_y : (x, y, z, ct) = (cos \theta x + sin \theta z, y, - sin \theta x + cos \theta z, ct)</math>
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*<math>R_y : (x, y, z, ct) = (cos \theta x + sin \theta z, y, - sin \theta x + cos \theta z, ct)</math>
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<br> <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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*<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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<br><br>
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Lorentzian Transformations:
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===Lorentzian Transformations===
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<br> <math>L_x : (x, y, z, ct) = (x', y, z, ct')</math>
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*<math>L_x : (x, y, z, ct) = (x', y, z, ct')</math>
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<br> <math>L_y : (x, y, z, ct) = (x, y', z, ct')</math>
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*<math>L_y : (x, y, z, ct) = (x, y', z, ct')</math>
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<br> <math>L_z : (x, y, z, ct) = (x, y, z', ct')</math>
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*<math>L_z : (x, y, z, ct) = (x, y, z', ct')</math>
  
 
[[Category:Physics]]
 
[[Category:Physics]]
 
[[Category:Mathematics]]
 
[[Category:Mathematics]]

Revision as of 06:39, August 1, 2009

The Poincaré Group consists of 10 mathematical transformations that can be applied to different coordinates of the space-time graph (x, y, z, ct), but do not affect the "spacetime interval". The "spacetime interval" is roughly the 4-D equivalent of 3-D "distance".

The Poincaré Group is a "symmetry group" because the spacetime interval remains invariant.

These transformations are:

Spatial translations

  • Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle T_y : (x, y, z, ct) = (x, y + \epsilon , z, ct)}
  • Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle T_z : (x, y, z, ct) = (x, y, z + \epsilon , ct)}

Time Translations

  • Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle T_t : (x, y, z, ct) = (x, y, z, ct + \epsilon )}

Spatial Rotations

  • Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle R_x : (x, y, z, ct) = (x, cos \theta y + sin \theta z, - sin \theta y + cos \theta y, ct)}
  • Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle R_y : (x, y, z, ct) = (cos \theta x + sin \theta z, y, - sin \theta x + cos \theta z, ct)}
  • Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle R_z : (x, y, z, ct) = (cos \theta x + sin \theta y, - sin \theta x + sin \theta y, z, ct)}

Lorentzian Transformations

  • Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle L_x : (x, y, z, ct) = (x', y, z, ct')}
  • Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle L_y : (x, y, z, ct) = (x, y', z, ct')}
  • Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle L_z : (x, y, z, ct) = (x, y, z', ct')}