Is the SL(2,R) action on the upper half-plane transitive?

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SUMMARY

The action of the group \( G = \text{SL}_2(\mathbb{R}) \) on the upper half-plane \( \mathcal{H} = \{ z \in \mathbb{C} : \text{Im}(z) > 0 \} \) is defined by \( g \cdot z = \frac{az + b}{cz + d} \) for \( g = \begin{pmatrix} a & b \\ c & d \end{pmatrix} \in G \). The orbit of \( i \) under this action, denoted \( \text{Orb}_G(i) \), consists of all points in \( \mathcal{H} \) that can be reached from \( i \) via the action of \( G \). The stabilizer \( \text{stab}_G(i) \) is the set of elements in \( G \) that fix \( i \). The action is indeed transitive, meaning every point in \( \mathcal{H} \) can be reached from \( i \) by some element of \( G \).

PREREQUISITES
  • Understanding of group theory, specifically the properties of \( \text{SL}_2(\mathbb{R}) \).
  • Familiarity with complex analysis, particularly the upper half-plane model.
  • Knowledge of group actions and orbits in mathematical contexts.
  • Basic linear algebra concepts related to matrix operations.
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  • Study the properties of \( \text{SL}_2(\mathbb{R}) \) and its representations.
  • Learn about the concept of transitivity in group actions.
  • Explore the relationship between orbits and stabilizers in group theory.
  • Investigate applications of the upper half-plane in number theory and modular forms.
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Mathematicians, particularly those specializing in group theory, complex analysis, and algebraic structures, will benefit from this discussion.

Chris L T521
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Here's this week's problem.

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Problem: Let $G=\text{SL}_2(\mathbb{R})$ and let $\mathcal{H}=\{z\in\mathbb{C}:\text{Im}(z)>0\}$. Let $g=\begin{pmatrix}a & b\\ c & d\end{pmatrix}\in G$ and define an action $\cdot :G\times\mathcal{H}\rightarrow\mathcal{H}$ where $g\cdot z=\dfrac{az+b}{cz+d}$. Compute $\text{Orb}_G(i)$ and $\text{stab}_G(i)$. Is this action transitive?

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No one answered this question correctly. You can find my solution below.

Let us first compute $\text{stab}_G(i)=\{g\in G:g\cdot i=i\}$. Let $g=\begin{pmatrix}a & b\\ c & d\end{pmatrix}\in\text{SL}_2(\mathbb{R})$. Then $\begin{pmatrix}a & b\\ c & d\end{pmatrix}\cdot i=i\implies \dfrac{ai+b}{ci+d}=i\implies ai+b=di-c\implies a=d\text{ and }b=-c$.
It now follows that $g$ is of the form $g=\begin{pmatrix} a & -c \\ c & a\end{pmatrix}$. Futhermore, since $g\in \text{SL}_2(\mathbb{R})$, we must have $\det g=1\implies a^2+c^2=1$. Thus, our matrix $g$ must represent a rotation on the unit circle. Hence, $g\in SO(2)$, and thus $\text{stab}_G(i)\cong SO(2)$.

To compute $\text{Orb}_G(i)$, we first observe that any element of our orbit must lie in the upper half plane $\mathcal{H}$; i.e. $g\cdot i=\dfrac{ai+b}{ci+d}\in\mathcal{H}$. Now, note that for $y>0$ and for any $x\in\mathbb{R}$, we have that $g=\begin{pmatrix}y^{1/2} & xy^{-1/2}\\ 0 & y^{-1/2}\end{pmatrix}\in \text{SL}_2(\mathbb{R})$. It now follows that $g\cdot i = \dfrac{y^{1/2}i+xy^{-1/2}}{y^{-1/2}}=y^{1/2}(y^{1/2}i+xy^{-1/2})=x+iy\in\mathcal{H}$. From this, it now follows that $g\cdot i$ generates the entire upper half plane; thus, $\text{Orb}_G(i)=\mathcal{H}$. Furthermore, $\text{Orb}_G(\mathcal{H})=\mathcal{H}$, and thus it follows that the action is transitive.
 
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