Is H a Lie Group with Subspace Topology from T^2?

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Discussion Overview

The discussion revolves around whether the subgroup ## H ##, defined within the torus ## \mathbb{T}^2 ##, can be considered a Lie group when given the subspace topology. Participants explore the implications of different topological structures on ## H ##, including its connectedness and the properties required for a set to qualify as a Lie group.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants argue that ## H ## is not a Lie group under the subspace topology due to its disconnected nature, particularly referencing the second component being a discrete set.
  • Others question how to change the topology of ## H ## to achieve connectedness and whether this can be done without altering the fixed irrational parameter ## a ##.
  • Several participants discuss the properties defining a Lie group, including being a finite-dimensional real smooth manifold and having smooth group operations.
  • There is mention of a potential topology for ## H ## that would make it homeomorphic to the real line, thus allowing it to be treated as a Lie group.
  • Some participants express confusion about the relationship between the defined set and the properties of topological groups, particularly regarding the continuity of functions across overlapping charts.
  • One participant suggests that the topology change could be formalized through a specific metric that defines distances in ## H ##, which differs from the subspace topology.

Areas of Agreement / Disagreement

Participants generally disagree on whether ## H ## can be made into a Lie group under the subspace topology, with some proposing alternative topologies while others maintain that the original constraints prevent this. The discussion remains unresolved regarding the feasibility of such a topology change.

Contextual Notes

Limitations include the dependence on the fixed parameter ## a ## and the unresolved nature of the continuity of functions across different charts. The discussion highlights the complexity of defining topological properties in relation to subgroup structures.

yamata1
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TL;DR
I'm trying to grasp Lie algebra with a non-example. Why isn't it a Lie group? The matrices seem invertible but is it a smooth manifold ?
"The group given by ## H = \left\{ \left( \begin{array} { c c } { e ^ { 2 \pi i \theta } } & { 0 } \\ { 0 } & { e ^ { 2 \pi i a \theta } } \end{array} \right) | \theta \in \mathbb { R } \right\} \subset \mathbb { T } ^ { 2 } = \left\{ \left( \begin{array} { c c } { e ^ { 2 \pi i \theta } } & { 0 } \\ { 0 } & { e ^ { 2 \pi i \phi } } \end{array} \right) | \theta , \phi \in \mathbb { R } \right\} ## with ## a \in \mathbb { P } = \mathbb { R } \backslash \mathbb { Q }
## a fixed irrational number,is a subgroup of the torus ## \mathbb { T}^2## that is not a Lie group when given the subspace topology.

The group
H
can, however, be given a different topology, in which the distance between two points
{\displaystyle h_{1},h_{2}\in H}
is defined as the length of the shortest path in the group
H
joining
h_{1}
to
h_{2}
. In this topology,
H
is identified homeomorphically with the real line by identifying each element with the number
\theta
in the definition of
H
. With this topology,
H
is just the group of real numbers under addition and is therefore a Lie group."

Why isn't it " a Lie group when given the subspace topology" ?
 
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Consider an open set in either topology. One is connected, the other one is not.
 
fresh_42 said:
Consider an open set in either topology. One is connected, the other one is not.
How do we change the topology of the subgroup from the original group? Could you show a simple proof of why it becomes connected ?
 
Look at the second component. This is a discrete set, namely ##[0,2\pi]-(\mathbb{Q}\cap [0,2\pi])##. All these points are open sets in the subspace topology, or combined with the first component, the union of open circular stripes. However, there is no way to guarantee that functions on two overlapping charts behave equally, Between two charts is always another chart such that the chart maps do not need to be continuous on their intersection.
 
fresh_42 said:
Look at the second component. This is a discrete set, namely [0,2π]−(Q∩[0,2π]). All these points are open sets in the subspace topology, or combined with the first component, the union of open circular stripes. However, there is no way to guarantee that functions on two overlapping charts behave equally, Between two charts is always another chart such that the chart maps do not need to be continuous on their intersection.
I'm a bit lost, is ##[0,2\pi]-(\mathbb{Q}\cap [0,2\pi])## equal to H or ##\mathbb{P}## ?I've never worked with topological groups,how does a disconnected topological group or set become connected?
 
A basis of the subspace topology on ##H## is given by
$$
\mathcal{T}_H=\left\{\left.\begin{pmatrix}e^{2\pi i \theta}&0\\0&e^{2\pi i a }\end{pmatrix}\, \right| \, \theta \in (\alpha,\beta) \subseteq \mathbb{R}\, , \,a\in \mathbb{P}\right\}
$$
Unions of these sets are the subspace topology on ##H##. Let us use two overlapping such sets
\begin{align*}
U_1&:= \left\{\left.\begin{pmatrix}e^{2\pi i \theta}&0\\0&e^{2 \pi i a}\end{pmatrix}\, \right| \, 0< \theta < 1\, , \,0<a<2/3\, , \, a\notin \mathbb{Q}\right\}\\
U_2&:= \left\{\left.\begin{pmatrix}e^{2\pi i \theta}&0\\0&e^{2\pi i a}\end{pmatrix}\, \right| \, 0< \theta < 1\, , \,1/3<a<1\, , \,a\notin \mathbb{Q} \right\}
\end{align*}
The second coordinate is expected to make problems. We now need the definition of a Lie group to see why this isn't one.

Which properties do you have that define a Lie group?
 
fresh_42 said:
Which properties do you have that define a Lie group

1-a finite-dimensional real smooth manifold
2- the group operations of multiplication and inversion are smooth maps.
 
Let's consider the manifold property. Can you define a chart at ##(\theta , a )=\left(\dfrac{1}{2},\dfrac{1}{\sqrt{2}}\right)\in U_2\,## such that multiplication with ##\begin{bmatrix}e^{2\pi i / n}&0\\0&e^{\sqrt{2}\pi i /n}\end{bmatrix}## becomes smooth?
 
I can't find a proper homeomorphism in ##U_2##.
 
  • #10
Yes, it is not locally Euclidean because of the gaps at the rationals. No matter how tiny the neighborhood is chosen, there are still gaps.
 
  • #11
How do we change the topology to make H a Lie group ?
 
  • #12
I don't think this is possible, except dropping the constraint ##a\notin \mathbb{Q}##. With ##a=\theta \in \mathbb{R}## we get a one parameter subgroup.
 
  • #13
"The group
H
can, however, be given a different topology, in which the distance between two points
{\displaystyle h_{1},h_{2}\in H}
is defined as the length of the shortest path in the group
H
joining
h_{1}
to
h_{2}
"
What does this give us in formal math ?
 
  • #14
@fresh_42 I think you're misreading the definition. The constant ##a## is fixed. The space ##H## "should be" one-dimensional. You wouldn't vary both ##\theta## and ##a## in a coordinate chart.

The subset ##H\subset T^2## is not a manifold because small open neighborhoods of every point are disconnected. I think you should try to draw a picture of this. Geometrically, ##H## is a continuous path in ##T^2## that gets arbitrarily close to every point in ##T^2##, infinitely often.

The map ##\theta\mapsto\begin{pmatrix}e^{2\pi i \theta} & 0\\0 & e^{2\pi i a\theta}\end{pmatrix}## gives a bijection from ##\mathbb{R}## to ##H.## You can give ##H## the topology that makes this map a homeomorphism- this is the metric topology you describe in your last post.
 
  • #15
Infrared said:
The map ##\theta\mapsto\begin{pmatrix}e^{2\pi i \theta} & 0\\0 & e^{2\pi i a\theta}\end{pmatrix}## gives a bijection from ##\mathbb{R}## to ##H.## You can give ##H## the topology that makes this map a homeomorphism- this is the metric topology you describe in your last post.
How can we write the topology change for H as a topological group ?
 
  • #16
I'm not sure what you mean by "topology change".

Call the elements of ##H## by ##A_\theta=\begin{pmatrix}e^{2\pi i \theta} & 0\\0 & e^{2\pi i a\theta}\end{pmatrix}.## The metric you describe in your post 13 is ##d(A_\theta,A_\phi)=|\theta-\phi|.## This is a valid metric on ##H## because the map ##\theta\mapsto A_\theta## is a bijection (from ##\mathbb{R}## to ##H##), so it defines a topology on ##H.## It is different from the subspace topology from the torus.
 
Last edited:
  • #17
Infrared said:
I'm not sure what you mean by "topology change".

Call the elements of ##H## by ##A_\theta=\begin{pmatrix}e^{2\pi i \theta} & 0\\0 & e^{2\pi i a\theta}\end{pmatrix}.## The metric you describe in your post 13 is ##d(A_\theta,A_\phi)=|\theta-\phi|.## This is a valid metric on ##H## because the map ##\theta\mapsto A_\theta## is a bijection (from ##\mathbb{R}## to ##H##), so it defines a topology on ##H.## It is different from the subspace topology from the torus.
So giving a different metric gives us the right topology to make H a Lie group.
Thank you.
 
  • #18
One result I remember is that given ##G## a Lie Group; here ## \mathbb T^2##, a subset is a Lie Group if it's both a subgroup and topologically closed in ##G##.
 

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