Since supersymmetry is not realized in our world, any supersymmetric model must include supersymmetry breaking. Similar to how the Higgs mechanism breaks the $SU(2) \times U(1)$ symmetry of the standard model to a $U(1)$ subgroup, so too must there be a variant of the Higgs mechanism that breaks supersymmetry to explain why our vacuum is not manifestly supersymmetric.
Any symmetry breaking mechanism comes with a scale. Above the energy scale of symmetry breaking, the symmetry is approximately restored; below the energy scale of symmetry breaking, the symmetry is broken. This scale will typically be associated with the masses of the supersymmetric partners. Traditional solutions of the hierarchy problem will place the scale of supersymmetry breaking somewhere around where the LHC can probe the new superpartners. However, there is no a priori reason for the SUSY breaking scale to be within reach of the LHC; theoretically it could take any value beyond current experiments (at least up to the Planck scale where one presumably has to incorporate quantum gravity as well). There are models such as split supersymmetry where the SUSY breaking scale could be of order 100 TeV while still being relevant for the hierarchy problem.
So, to summarize:
- For SUSY in general, the SUSY breaking scale could take on any value up to the Planck scale, so we will essentially never be able to rule out SUSY as a possibility with lab experiments.
- For SUSY relevant to the hierarchy problem, there are published models where the SUSY scale could be as high as the 100 TeV range. However, at least as far as I know, there is no guarantee that if experiments ruled out SUSY breaking up to about 100 TeV, that theorists would not discover interesting models with a SUSY breaking scale in (say) the 1000 TeV range (and so on). The further we get above the mass of the Higgs, the harder it is to argue that the model solves the hierarchy problem, but there is no sharp line where it becomes impossible to make that connection.
- There are other SUSY parameters that I did not talk about which are necessary to understand how constraints arise on specific instantiations of SUSY. However, the presence of a SUSY breaking scale is a universal feature of phenomenological SUSY models.