The six matrices$$\begin{pmatrix}0 & 0 \\ 0 & 0\end{pmatrix}, \begin{pmatrix}1 & 0 \\ 0 & 0\end{pmatrix}, \begin{pmatrix}-1 & 0 \\ 0 & 0\end{pmatrix}, \begin{pmatrix}1 & 0 \\ 0 & 1\end{pmatrix}, \begin{pmatrix}-1 & 0 \\ 0 & -1\end{pmatrix}, \begin{pmatrix}1 & 0 \\ 0 & -1\end{pmatrix}$$are representatives for the orbits.
The determinant of the matrix $A = \begin{pmatrix}x & y \\ y & z\end{pmatrix}$ is $xz - y^2$, and because the determinant is homogeneous, the locus $xz = y^2$ is an ellptical double cone $C$ in $\mathbb{R}^3$. To visualize the cone, one may diagonalize by the substitution $\sqrt{2}x = u + v$, $\sqrt{2}z = u - v$. The equation becomes $u^2 = v^2 + 2y^2$.
The cone splits into three orbits, the first three on the list, and it also splits into three connected parts, $\{0\}$, the "positive" cone $C^+$ with $u > 0$, and the "negative" cone $C^-$ with $u < 0$. The complement of $C$ in $\mathbb{R}^3$ splits into the remaining three orbits, and it splits into three connected parts, the interiors $D^+$ and $D^-$ of $C^+$ and $C^-$, and the exterior $\Delta$ of the cone.
It is natural to guess that the orbits of the six representatives are the sets $0$, $C^+$, $C^-$, $D^+$, $D^-$, $\Delta$, in that order, and it is obvious that the orbit of $0$ is $0$. To show this, one first checks that the representatives are in the respective sets. Then the quickest thing to do is to note that one can put a symmetric matrix $A$ into the standard form, in which $P^\text{T}AP$ is one of the six matrices listed, using a matrix $P$ that has positive determinant. The group of matrices with positive determinant is path connected. Therefore an orbit will also be path connected. The connected orbit of $e_{11}$ is contained in $C$, and since the complement of $0$ splits into two connected parts, that orbit must be contained entirely in $C^+$. Similarly, the orbit of $-e_{11}$ must be contained entirely in $C^-$. Together the orbits of $0$, $e_{11}$, and $-e_{11}$ make up $C$. So the orbit of $e_{11}$ must be all of $C^+$, etc$\dots$
In the interests of completeness, the orbits are explicitly:
- $1$, $1$ gives $(a^2 + c^2, ab + cd, b^2 + d^2)$ with $ad - bc \neq 0$ $($negative of $-1$, $-1)$. Then $xz - y^2 = (ad - bc)^2 > 0$, with $x$, $z > 0$.
- $1$, $-1$ gives $(a^2 - c^2, ab - cd, b^2 - d^2)$ with $ad - bc \neq 0$. Then $xz - y^2 = -(ad - bc)^2 < 0$, with no restrictions on $x$, $z$.
- $-1$, $-1$ gives $(-a^2 - c^2, -ab-c, -b^2-d^2)$ with $ad - bc \neq 0$ $($opposite of $1$, $1)$. Then $xz - y^2 = (ad-bc)^2 > 0$, with $x$, $z < 0$.
- $1$, $0$ gives $(a^2, ab, b^2)$ with $ad - bc \neq 0$ $($opposite of $-1$, $0)$. Then $xz = y^2$, with $x$, $z \ge 0$ but not both zero.
- $-1$, $0$ gives $(-a^2, -ab, -b^2)$ with $ad - bc \neq 0$ $($opposite of $1$, $0)$. Then $xz = y^2$, with $x$, $z \le 0$ but not both zero.
- $0$, $0$ gives $(0, 0, 0)$.
These are simply determinant identities.