Improper and non-orthochronous group

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In summary, the equation Λ00^2 - Λ11^2 - Λ22^2 - Λ33^2 = 1 is never correct. The correct equation is ημνΛμρΛνσ = ηρσ, which defines the full Lorentz group O(1,3). The special Lorentz group has an additional constraint, det(Λμν) = +1, and is called SO(1,3). The orthochronous Lorentz group O(1,3)^↑ has the constraint Λ00 ≥ 1. The proper orthochronous Lorentz group, which is continuously connected to the identity, is the
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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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1. What is an improper group?

An improper group is a mathematical concept that describes a group of transformations that includes both proper and improper transformations. Proper transformations preserve the orientation of objects, while improper transformations do not.

2. What is a non-orthochronous group?

A non-orthochronous group is a type of improper group that includes transformations that do not preserve the direction of time. This means that objects can appear to move backwards in time after undergoing these transformations.

3. How are improper and non-orthochronous groups used in science?

Improper and non-orthochronous groups are used in scientific fields such as physics, chemistry, and crystallography to describe the symmetries and transformations of objects and systems. They are also used in mathematical models to study the behavior of complex systems.

4. What are some examples of improper and non-orthochronous groups?

One example of an improper group is the symmetry group of a regular hexagon, which includes both rotations and reflections. An example of a non-orthochronous group is the Lorentz group, which describes the symmetries of space and time in special relativity.

5. How do improper and non-orthochronous groups differ from proper and orthochronous groups?

The main difference between improper and proper groups is the inclusion of improper transformations, which do not preserve the orientation of objects. Similarly, non-orthochronous groups differ from orthochronous groups in that they include transformations that do not preserve the direction of time. Proper and orthochronous groups only include transformations that preserve both orientation and time direction.

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