What Is the Euclidean Analog of the Poincaré Group?

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SUMMARY

The Poincaré group consists of all continuous transformations in Minkowski space that preserve the inner product, specifically translations and the restricted Lorentz group, which includes proper orthochronous Lorentz transformations such as rotations and boosts. In contrast, the Euclidean group comprises translations and the orthogonal group, which includes rotations and rotoreflections. The subgroup E+(n) corresponds to translations and the special orthogonal group, paralleling the relationship between the Poincaré group and Minkowski space. The full Poincaré group, which includes discontinuous transformations, has four connected components and is sometimes referred to as the restricted Poincaré group.

PREREQUISITES
  • Understanding of Minkowski space and its properties
  • Familiarity with the Poincaré group and Lorentz transformations
  • Knowledge of Euclidean space and the Euclidean group
  • Basic concepts of group theory and connected components
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  • Research the properties of the Poincaré group in detail
  • Explore the structure and applications of the Euclidean group
  • Study the implications of discontinuous transformations in physics
  • Investigate the relationship between the restricted and full Poincaré groups
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Mathematicians, physicists, and students studying theoretical physics, particularly those interested in the geometry of spacetime and group theory applications in physics.

Rasalhague
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Benjamin Crowell writes here, "The discontinuous transformations of spatial reflection and time reversal are not included in the definition of the Poincaré group, although they do preserve inner products."

http://www.lightandmatter.com/html_books/genrel/ch02/ch02.html

So, if I've understood this, the Poincaré group consists of all continuous transformations in Minkowski space that preserve the inner product: (1) translations and (2) the restricted Lorentz group (proper orthochronous Lorentz transformations in Minkowski space, i.e. rotations and boosts).

Is there a name for the corresponding set of transformations in Euclidean space? I gather the Euclidean group consists of (1) translations and (2) the orthogonal group (rotations and rotoreflections). It has a subgroup E^{+}\left ( n \right ) consisting of translations and the special orthogonal group (rotations). This E^{+}\left ( n \right ) is to Euclidean space what the Poincaré group is to Minkowski space, isn't it?

Is there a name or conventional symbol for the set of transformations in Minkowski space corresponding to the Euclidean group (translations together with the full Lorentz group), and does it form a group too?
 
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Rasalhague said:
Benjamin Crowell writes here, "The discontinuous transformations of spatial reflection and time reversal are not included in the definition of the Poincaré group, although they do preserve inner products."

http://www.lightandmatter.com/html_books/genrel/ch02/ch02.html

So, if I've understood this, the Poincaré group consists of all continuous transformations in Minkowski space that preserve the inner product: (1) translations and (2) the restricted Lorentz group (proper orthochronous Lorentz transformations in Minkowski space, i.e. rotations and boosts).

This exclusion in non-standard. Similar to the Lorentz group, the full Poincare group has four connected components. Benjamin Crowell defines the "Poincare group" to be the connected component of the Poincare group that contains the identity.
Rasalhague said:
Is there a name or conventional symbol for the set of transformations in Minkowski space corresponding to the Euclidean group (translations together with the full Lorentz group), and does it form a group too?

Yes, it's called the Poincare group.
 
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Thanks, George!

I see that what Benjamin Crowell calls "the Poincaré group" is sometimes referred to as "the restricted Poincaré group".
 

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