  We represent the first investigation of pole-skipping on both the gravity and
field theory sides. In contrast to the higher dimensional models, there is no
momentum degree of freedom in $(1+1)-$dimensional bulk theory. Thus, we then
consider a scalar field mass as our degree of freedom for the pole-skipping
phenomenon instead of momentum. The pole-skipping frequencies of the scalar
field in 2D gravity are the same as higher dimensional cases: $\omega=-i2\pi
Tn$ for positive integers $n$. At each of these frequencies, there is a
corresponding pole-skipping mass, so the pole-skipping points exist in
$(\omega,m)$ space. We also compute the pole-skipping points of the SYK model
in $(\omega, h)$ space where $h$ is the dimension of the bilinear primary
operator. We find that there is a one-to-one correspondence of the
pole-skipping points between the JT gravity and the SYK model. To obtain the
pole-skipping points, we need to consider the parameter $\epsilon$ related to
the chemical potential on the horizon of charged JT gravity and the
particle-hole asymmetric parameter $\mathcal{E}$ of the complex SYK model as
shift parameters. This highlights the $\epsilon-\mathcal{E}$ correspondence in
relation to pole-skipping phenomenon.
