Understanding Lie Groups: SO(1,1) and Dimensionality

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SUMMARY

SO(1,1) is a Lie group that preserves a hyperbolic product defined by the equation a² - b² = a'² - b'², distinguishing it from SO(2), which preserves the Euclidean dot product a² + b² = a'² + b'². The notation SO(m,n) generalizes this concept, indicating m minus signs and n plus signs, applicable to vectors of dimension m+n. The dimensionality of a Lie group corresponds to the number of generators, confirming that SO(1,1) has one generator, similar to SO(2). This framework is particularly relevant in the context of Special Relativity, where the Lorentz group is represented as SO(1,3).

PREREQUISITES
  • Understanding of Lie groups and their properties
  • Familiarity with the notation SO(m,n)
  • Knowledge of hyperbolic geometry and its applications
  • Basic concepts of Special Relativity
NEXT STEPS
  • Study the properties and applications of the Lorentz group SO(1,3)
  • Explore the geometric interpretations of SO(1,1) and SO(2)
  • Learn about the generators of Lie groups and their significance
  • Investigate the role of Lie groups in theoretical physics
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Mathematicians, physicists, and students interested in advanced topics in geometry and theoretical physics, particularly those focusing on Special Relativity and Lie group theory.

qtm912
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I am familiar with what SO(2) means for example but am unclear what SO(1,1) refers to. This came up in a classical physics video lecture when lie groups were discussed and the significance of the notation was glossed over.
Second question: is the dimensionality of such a group the same as the number of generators?
 
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SO(2) has an interpretation as rotations that preserve the dot product in two dimensions. So a^2 + b^2 = a'^2 + b'^2 where a' and b' are the result of applying an element of SO(2) to the two component vector with components a and b.

SO(1,1) is also preserves such a product, but it's not the usual dot product you are familiar with. Rather, it says that a^2 - b^2 = a'^2 - b'^2 (notice the minus sign). So extending this notation, SO(m,n) would be m minus signs and n plus signs, and acts of vectors of dimension m+n. This is most useful in Special Relativity, where the lorentz group is SO(1,3).

I think the dimension of a group is the number of generators, but I don't remember for sure.
 
DimReg said:
SO(2) has an interpretation as rotations that preserve the dot product in two dimensions. So a^2 + b^2 = a'^2 + b'^2 where a' and b' are the result of applying an element of SO(2) to the two component vector with components a and b.

SO(1,1) is also preserves such a product, but it's not the usual dot product you are familiar with. Rather, it says that a^2 - b^2 = a'^2 - b'^2 (notice the minus sign). So extending this notation, SO(m,n) would be m minus signs and n plus signs, and acts of vectors of dimension m+n. This is most useful in Special Relativity, where the lorentz group is SO(1,3).

I think the dimension of a group is the number of generators, but I don't remember for sure.

Thank you very much, it is clear now
 

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