Possible hard wall boundary condition for particle?
This package is pretty nice for the demonstration of time of particle evolution in the model potential. Would it be possible to remove the periodic boundary condition? I mean, use the "hard wall" boundary condition during the calculation?
There's no out-of-the-box way to do this right now, but you can always define your own potential using e.g. the potentialoperator function. Essentially, you could create a symmetric version of the potential used in this example https://docs.qojulia.org/examples/particle-into-barrier/ and make the potential high enough so it acts as a wall.
Thanks for the advice. I'll try it later.
If you have had success implementing it, do not hesitate to submit it as a pull request -- libraries like this really improve when users contribute back and we would be happy to help along the way.