✎ Poincare Group [The Physics Travel Guide]

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====== Poincare Group $ \quad \color{red}{P(1, 3)} = \color{blue}{T(4)} \color{magenta}{\rtimes} \color{green}{SO(1, 3)}$ ======

<tabbox Why is it interesting?> 
The double cover of the Poincare group is the fundamental spacetime symmetry of modern physics and is a crucial component of the [[models:standard_model|standard model of particle physics]].

The Poincare group is the set of all transformations that leave the speed of light invariant. Thus, the Poincare group yields all possible transformations between allowed frames of reference. This is incredibly useful, when we want to write down fundamental laws of nature. The fundamental laws should be valid in all allowed frames of reference, otherwise they would be quite useless.

In practice, we can use our knowledge of all transformations inside the Poincare group to write down equations that are invariant under all these transformations. These equations then hold in all allowed frames of reference. This is such a strong restriction on the possible equations that is is almost enough to derive the most important equations of fundamental physics: the Dirac equation, the Klein-Gordon equation and the Maxwell-Equations.

<blockquote>"//The Hilbert space of one-particle states is always an irreducible
representation space of the Poincare group. [...] **The construction of the unitary irreducible representations
of the Poincare group is probably the most successful part of special
relativity** (in particle physics, not in gravitation theory, for which it is a
disaster). **It permits us to classify all kinds of particles and implies the main
conservation laws (energy-momentum and angular momentum)**. [...] The translation generators are
responsible for the energy-momentum conservation laws, the rotation generators
of the conservation of angular momentum, and the boost generators
of the conservation of initial position.  //" from Reflections on the Evolution of Physical Theories by Henri Bacry</blockquote>

<blockquote>"//The enlargement of the Lorentz group to the Poincare group was proposed [ 13] as a way of describing the quantum states of relativistic particles without using the wave equations. The states of a free particle are then given by the unitary irreducible representations of the Poincare group.//" from [[http://www.sciencedirect.com/science/article/pii/0370269394001103|Deformed Poincare containing the exact Lorentz algebra]] by Alexandros A. Kehagias et. al.</blockquote>
<tabbox Layman>

<note tip>
Explanations in this section should contain no formulas, but instead colloquial things like you would hear them during a coffee break or at a cocktail party.
</note>
  
<tabbox Student> 
The $\color{red}{\text{Poincare group}}$ consists of $\color{blue}{\text{translations}}$ $\color{magenta}{\text{plus}}$ $\color{green}{\text{rotations and boosts}}$.

* A nice discussion can be found here {{ :advanced_tools:group_theory:darstellung-als-diff-operator.pdf |Representations of Lorentz and Poincar´e groups by Joseph Maciejko}} and
  * here: {{ :advanced_tools:group_theory:genial-massiv-und-masselos-besser-erklaert.pdf |Representations of the Poincar´e group Prahar Mitra}} and
  *  here: http://pages.cs.wisc.edu/~guild/symmetrycompsproject.pdf
  * see also page 211ff in [[https://web.physics.ucsb.edu/~mark/ms-qft-DRAFT.pdf|Quantum Field Theory]] by Mark Srednicki

----

** The Poincare Algebra **

\begin{eqnarray}
{}[J_i,J_j]&=&i \epsilon_{ijk}J_k,  \nonumber \\
{} [J_i,K_j]&=& i\epsilon_{ijk} K_k,  \nonumber \\
{} [K_i,K_j]&=& -i \epsilon_{ijk}J_k ,\nonumber \\
{} [J_i,P_0]&=&0, \nonumber \\
{} [J_i,P_j]&=& i\epsilon_{ijk} P_k,  \nonumber \\
{} [P_0,P_i]&=&0,  \nonumber \\
{} [K_i,P_0]&=&i  P_i, \nonumber \\
{}[K_i,P_j]&=& i\ P_0 \delta_{ij} , \label{c}
\end{eqnarray}

* For a modern discussion of the Poincare group, see D. Giulini, The Poincare group: Algebraic, representation-theoretic, and geometric
aspects.

</tabbox>

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