Non-compactness of Lorentz Group ?

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Discussion Overview

The discussion revolves around the properties of the Lorentz group, particularly its compactness. Participants explore definitions and implications of compactness in the context of the Lorentz group and related transformations, addressing both theoretical and conceptual aspects.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • One participant references Peskin's text, suggesting that the Homogeneous Lorentz group might be compact due to its finite number of generators (10), but questions arise regarding this assumption.
  • Another participant argues that the Poincare group, which includes translations and boosts, is non-compact, asserting that neither the Lorentz group nor the Galileo group is compact due to the nature of their transformations.
  • A participant explains that a Lie group is compact if it can be covered by a finite number of compact maps, noting that the Lorentz group requires a non-compact parameter set for boosts, specifically using rapidity as a parameter.
  • One participant attempts to argue for compactness by suggesting that relative velocities between inertial frames, which range from 0 to c, could define a compact set of transformations.
  • Another participant clarifies that the parameter space for Lorentz transformations does not include c, and thus the set of velocities [0, c) is not closed and therefore not compact, referencing the Heine-Borel theorem.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the compactness of the Lorentz group. While some argue it is non-compact based on established definitions and properties, others propose alternative interpretations that lead to confusion regarding the compactness criteria.

Contextual Notes

The discussion highlights limitations in understanding compactness, particularly in relation to the definitions of parameter sets and the implications of including or excluding certain boundary values (like c) in the context of Lorentz transformations.

jys34
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Hello, I'm studying the Lorentz group and their properties... and I have some question for them..

Peskin's text(p496) said that

"we are primarily interested in Lie algebras that have finite-dimensional Hermitian representations, leading to finite-dimensional unitary representations of the corresponding Lie group.

We will also assume that the number of generators is finite.

Such Lie algebras are called compact, because these conditions imply that the Lie group is a finite-dimensional compact manifold."


From this mentions of compactness,

I've thought that Homogeneous Lorentz group is compact because the number of generators of it is just 10(M_{\mu\nu},P_{\mu} 3 rotations, 3 boosts, 4 translations)



In Arfken and many other texts, However, they said that the Homogeneous Lorentz group is non-compact, because the limit of a sequence of rapidities going to infinity is no longer an element of the an element of the group. (Arfken, p278)

From the same reason, translation is non-compact, too.
(therefore, Poincare group is non-compact.)


What's wrong with my assumption for compactness of the Lorentz group?


I know that I have some misunderstanding for compactness and I need a help to figure it out...
 
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Peskin/Schroeder is sometimes (or better said often) pretty sloppy in the details. Of course, first of all we are interested in the Poincare group, if we like to do quantum theory in the relativistic realm, and the Poincare group for sure is not compact. The alone are not a compact Lie group, but neither is the Lorentz group (the same is true for the Galileo group, where also the translations and the Lorentz boosts are non-compact subgroups).

A Lie group is called compact if there is a compact parameter set which maps out the whole group (more precisely there should be a finite number of such compact maps which cover the whole group, i.e., make an atlas). Indeed, if you look at the Lorentz group (more precisely: the orthochronous proper Lorentz group, which makes the subgroup of the full Lorentzgroup that is continuously connected with the group identity) is not compact, because to get boosts in the x direction, you always need a non-compact parameter set to map this one-parameter subgroup. The natural choice is indeed rapdity:

\Lambda_z(\eta)=\begin{pmatrix}<br /> \cosh \eta &amp; -\sinh \eta &amp;0 &amp; 0 \\<br /> -\sinh \eta &amp; \cosh \eta &amp;0 &amp;0 \\<br /> 0 &amp; 0 &amp; 1 &amp;0 \\<br /> 0&amp; 0 &amp; 0 &amp; 1<br /> \end{pmatrix}, \quad \eta \in \mathbb{R}.

The first consequence of the Lorentz group not being compact is that there are no unitary finite-dimensional representations, except the trivial one, but there are unitary infinitely dimensional representations of the whole Poincare group, and these can be classified (Wigner 1939) and investigated whether they describe physical systems. Indeed, one finds representations describing massive and massless particles with integer and half-integer spin. This is the starting point for model building in high-energy physics (standard model etc.).

You find a quite complete description of the mathematics in my qft manuscript,

http://fias.uni-frankfurt.de/~hees/publ/lect.pdf

and of course in Weinberg's marvelous books (Quantum Theory of Fields). The unitary representations of the Poincare group are treated in the first chapters of volume 1. It's way better than Peskin/Schroeder in such fundamental issues!
 
The set of all Lorentz transformations forms a non-compact topological space, because it contains the orthocronous proper transformations which form a non-compact tolopogical space by the following argument. The subset of all boosts in an arbitrary direction can be homemorphically mapped onto R, which is non-compact in the usual topology. But the set of all boosts in a direction is a subset of all restricted Lorentz transformations. So the full Lorentz group contains a subset which is homeomorphic to R. So it must be non-compact.
 
hello,

I came to this same exact question this couple of days, not sure how useful it will be to post on a thread which seems inactive now, but still, quoting vanhees71

"A Lie group is called compact if there is a compact parameter set which maps out the whole group"

which is the rough definition of the compactness, then what about describing every Lorentz transformation with the parameter V (or V/c) of relative velocity of 2 inertial frames, which goes from 0 to c. then to every element of Lorentz group corresponds a number between 0 and c, so it seems to be compact, what's wrong here?
 
Is c included?
 
I guess I should make my point clearer.

What is a Lorentz transformation - it's a transformation of coordinates from one intertial frame to another, which moves with a uniform velocity V relatively to the first frame.
Different Lorentz transformations just correspond to different relative velocities V.

The question is, the velocities are limited from above by c, so the velocities themselves form a compact set, to every V corresponds a Lorentz transformation - then why is the Lorentz group non-compact?
 
c is not included in the parameter space for the set of Lorentz transformations that you considered, i.e., the parameter space is the half-open, half-closed interval of real numbers [0 , c). By the Heine-Borel theorem, a subset of the real numbers is compact if and only if the subset is closed and bounded. [0 , c) is not a closed subset of the real numbers, and thus is not compact.
 
ah, thanks, that explains it all
 

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