Improper and non-orthochronous group

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SUMMARY

The discussion clarifies that the equation (Λ00)2 – (Λ11)2 – (Λ22)2 – (Λ33)2 = 1 is incorrect for a group that is neither proper nor orthochronous. The correct formulation is given by the equation ημν Λμρ Λνσ = ηρσ, which defines the full Lorentz group O(1,3). The special Lorentz group, denoted as SO(1,3), has the constraint that det(Λμν) = +1. The orthochronous Lorentz group O(1,3)↑ requires that Λ00 ≥ 1, while the proper orthochronous Lorentz group SO(1,3)↑ represents the fundamental symmetry of nature alongside space-time translations, forming the proper orthochronous Poincaré group.

PREREQUISITES
  • Understanding of Lorentz transformations
  • Familiarity with group theory concepts
  • Knowledge of Minkowski space
  • Basic principles of special relativity
NEXT STEPS
  • Study the properties of the Lorentz group O(1,3)
  • Explore the significance of the special Lorentz group SO(1,3)
  • Learn about the proper orthochronous Poincaré group
  • Investigate applications of Lorentz transformations in physics
USEFUL FOR

Physicists, mathematicians, and students studying relativity, group theory, or theoretical physics will benefit from this discussion, particularly those interested in the symmetries of space-time.

PRANAV UPADHYAY
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will it be correct to say
00)2 – (Λ11)2 – (Λ22)2 – (Λ33)2 = 1

if Λ - group is neither proper nor orthochronous
 
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That's never correct. What you mean is
$$\eta_{\mu \nu} {\Lambda^{\mu}}_{\rho} {\Lambda^{\nu}}_{\sigma}=\eta_{\rho \sigma},$$
which defines the full Lorentz group ##\mathrm{O}(1,3)##.

The special Lorentz group has the additional constraint that ##\mathrm{det} ({\Lambda^{\mu}}_{\nu})=+1##. The corresponding subgroup is called ##\mathrm{SO}(1,3)##.

Then there is the orthochronous Lorentz group ##\mathrm{O}(1,3)^{\uparrow}##, for which ##{\Lambda^{0}}_0 \geq 1##.

Finally there's the subgroup which is the part that is continuously connected with the idendity, and that's the proper orthochronous Lorentz group. It consists of all orthochronous special Lorentz transformations, forming the group ##\mathrm{SO}(1,3)^{\uparrow}##, and it's the group that is describes a fundamental symmetry of nature (together with the space-time translations it's the symmetry group of Minkowski space that is realized as a symmetry group of nature, the proper orthochronous Poincare group).
 
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