Trying to get a first understanding of QM. The Schrödinger equation in standard form for $\Psi$
$$ i \hbar\frac{\partial }{\partial t} \Psi(x,t) =\left[-\frac{\hbar^2}{2m}\frac{\partial^2 }{\partial t^2} +V(x,t)\right]$$
Can we look at it this way, since we can have both signs for $ i= \pm \sqrt{-1} $ and agree to accommodate/use Planck's constant also as an imaginary constant $i \hbar\to \hbar $ can the following Schrödinger equation form still interpret or represent negative potential energy $V$ (unconventionally) for same wave function $\Psi?$
$$ \hbar \frac{\partial }{\partial t} \Psi(x,t) =\left[\frac{\hbar ^2}{2m}\frac{\partial^2 }{\partial t^2}+V(x,t)\right].$$
An advantage could be that an imaginary quotient need explicitly occur in the PDE. I am not sure of the constants making sense.