We have the subgroup $PSL(2,\mathbb{C}) \simeq SO^+(1,3)$. So yes we can take the subgroup given by the classes of the following elements
$$
P_b = \begin{pmatrix}
1&b\\
0&1
\end{pmatrix}
$$
with $b$ real.
Under the specified isomorphism this becomes
$$
Q=\begin{pmatrix}
t+z&x-iy\\
x+iy&t-z
\end{pmatrix}
\rightarrow
P_b Q P_b^\dagger\\
= \begin{pmatrix}
t+2bx+b^2 t + (1-b^2) z & x+bt-bz-i y\\
x+bt-bz+i y & t-z \\
\end{pmatrix}\\
x \to x+bt-bz\\
y \to y\\
t \to bx+(1+\frac{b^2}{2})t - \frac{b^2}{2} z\\
z \to \frac{b^2}{2} t+(1-\frac{b^2}{2})z+b x
$$
This therefore acts on functions on $\mathbb{R}^{1,3}$ by acting on the underlying space. So that function space is a representation of this $P_b$ group. We can try to decompose it by characters.
Recall the usual Fourier transform. You have the translation action $x \to x+a$ and the characters of that are the functions $e^{ipx}$ which the function gets decomposed into. They are eigenvectors with eigenvalue $e^{ipa}$ under this transformation.
So take the formula for $P_b Q P_b^\dagger$ and find the analogs for $e^{i p x}$.
See the part of the wiki on parabolic transformations. In particular the sorts of functions that are invariant under this group are given. Those are the ones with eigenvalue $0$ so replace that procedure with other eigenvalues.
But you can see unlike a simple translation and Fourier transform, this is not as intuitive of a transformation. There the two sides were position translations and momentum easily interpreted. Here on one side is this explicit mix of rotations and boosts. Send $b \to \epsilon$, if you want the infinitesimal transformation to write the analog of $\frac{d}{dx} f = ip f$. The other side is the corresponding conserved charge for that 1-parameter group.
The $U(1)$ QED group is a separate group. That refers to an internal symmetry not a symmetry of spacetime. $\psi (t,x,y,z) \to e^{i \theta} \psi (t,x,y,z)$. $(t,x,y,z)$ don't change. That abelian group does not move points around, this abelian group does.
For an uncertainty principle, you just need two operators that don't commute acting on your Hilbert space. But the Hilbert space is something that should be assigned to a timelike slice. This is mixing up different slices.
