Poincaré group is semi-product of translations and Lorentz-group

In summary: Lorentz transformation, satisfying the axiom.In summary, the proofs for the axioms of the semi-direct product of the Poincaré group show that the combination of translations and Lorentz transformations still preserves the structure of the original subgroups, and that any element in P can be decomposed into a translation and a Lorentz transformation. I hope this helps clarify the concept for you.
  • #1
aoner
11
0
Hi everybody,

Can somebody help me with the following proof.
Show that for the Poincaré group

[itex]P=T\odot L[/itex]

Where [itex]T[/itex] is the group of translations and [itex]L[/itex] is the Lorentz group and [itex]P[/itex] is the semi-direct product of the two subgroups

I know the axioms for a semi-direct product in this case are
  • [itex]T[/itex] is an invariant subgroup of [itex]P[/itex] while [itex]L[/itex] is any subgroup of [itex]P[/itex]
  • [itex]T\cap L=\{E\}[/itex], where [itex]E[/itex] is the identity of [itex]P[/itex]
  • For every element [itex]S[/itex] in [itex]P[/itex] we have an element [itex]{{S}_{1}}[/itex] of [itex]T[/itex] and an element [itex]{{S}_{2}}[/itex] of [itex]L[/itex] for which: [itex]S={{S}_{1}}\circ {{S}_{2}}[/itex]

How do I proof these axioms?
 
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  • #2




Thank you for your question. The Poincaré group is a fundamental concept in physics, and understanding its structure is crucial in many areas of research. I will try to provide a clear and concise explanation of the proofs for the axioms of the semi-direct product of the Poincaré group.

First, let's define the Poincaré group as the group of all transformations that leave the laws of physics invariant. This includes translations in space and time (T) and Lorentz transformations (L), which are rotations and boosts in space-time. The semi-direct product of these two subgroups (P) is a way to combine their elements to form a larger group that preserves the structure of the original subgroups.

Axiom 1: T is an invariant subgroup of P while L is any subgroup of P

To prove this axiom, we need to show that the elements of T and L, when combined, still form a valid transformation in P. This means that the composition of two elements from T and L should also be an element in P, and this composition should follow the group operation of P (in this case, composition of transformations). This can be easily shown by considering the composition of two translations or two Lorentz transformations, which will result in another translation or Lorentz transformation, respectively.

Axiom 2: T∩L={E}, where E is the identity of P

This axiom states that the only element common to both T and L is the identity element of P. To prove this, we need to show that there is no other element that belongs to both T and L. Since the elements of T and L are translations and Lorentz transformations, respectively, it is clear that they do not share any common elements except for the identity transformation, which is the composition of the identity translation and the identity Lorentz transformation.

Axiom 3: For every element S in P we have an element S1 of T and an element S2 of L for which: S=S1∘S2

This axiom states that any element in P can be decomposed into a translation and a Lorentz transformation. This can be proven by considering the composition of any element in P with an arbitrary element of T and L. Since T and L are invariant subgroups, the composition will still result in an element of P, and this element can be decomposed into a translation and a
 

1. What is the Poincaré group?

The Poincaré group is a mathematical concept that describes the symmetries of space and time. It is a collection of transformations, such as rotations and translations, that leave the laws of physics unchanged.

2. How is the Poincaré group related to translations and Lorentz group?

The Poincaré group is a semi-product of translations and the Lorentz group, which means that it is a combination of the two groups. It includes both spatial translations and transformations that preserve the speed of light, known as Lorentz transformations.

3. What is the significance of the Poincaré group in physics?

The Poincaré group plays a crucial role in understanding the fundamental laws of physics, particularly in the context of special relativity. It allows us to describe the symmetries of space and time, which are essential in formulating physical theories.

4. How is the Poincaré group used in theoretical physics?

The Poincaré group is used in theoretical physics to study the properties of physical systems and their symmetries. It is an important tool for understanding the behavior of particles and fields in space and time, and it allows for the development of mathematical models to describe these systems.

5. Are there any other applications of the Poincaré group besides physics?

Yes, the Poincaré group has applications in other fields such as mathematics, computer science, and engineering. It is used in areas such as image and signal processing, robotics, and pattern recognition. It also has connections to other branches of mathematics, such as group theory and differential geometry.

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