Bob Dylan said:
Kudos for your efforts to learn and understand. In general, early stages in the curriculum for QM lay quite a claim on one's imagination (witness he numerous threads in PF). At the same time your imagination easily leads you astray from the beaten path of well-established science (even more threads in PF, however hard the moderators try to lock 'em

)
It is hard to attribute a physical meaning to the wave function ##\psi## itself ("
a complex-valued probability amplitude"

), other than that ##\ \psi^*\psi\ ## repesents a probability density (*).
(*) Already here I have to correct post #2, where I wrote that the amplitude ##\ \sqrt{\psi^*\psi }\ ## repesents a probability density. The amplitude is a probability
amplitude. ( Sounds logical, doesn't it. I looked it up in my Merzbacher, QM 1970 ; fortunately
wiki agrees )
Scale is determined by normalization: like ##\ \int \psi^*\psi = 1 ## (a resonable requirement for a probability density function) .
Since ##\ \psi^*\psi\ ## is a density, its dimension is 1/"whatever it is you are integrating over":##\ \int_{\rm \text whole \ space} \psi^*\psi \; d\tau = 1 ##
Dimensions come in with the operators. Physically relevant operators are Hermitian and (phew...) therefore have real-valued eigenvalues that are potentially observable. So expectation values of operators have the corresponding dimension.
You'll learn and after a while the lingo becomes almost natural. Usually that's where genuine theoreticians come into declare it's all nonsense and should be re-built from scratch
