We present a perturbative approach to a broad class of disordered systems in
one spatial dimension. Considering a long chain of identically disordered
scatterers, we expand in the reflection strength of any individual scatterer.
This expansion accesses the full range of phase disorder from weak to strong.
We apply this expansion to several examples, including the Anderson model, a
general class of periodic-on-average-random potentials, and a two-component
discrete-time quantum walk, showing analytically in the latter case that the
localization length can depend non-monotonically on the strength of phase
disorder (whereas expanding in weak disorder yields monotonic decrease).
Returning to the general case, we extend the perturbative derivation of
single-parameter scaling to another order and obtain to all orders a particular
non-separable form for the joint probability distribution of the
log-transmission and reflection phase. Furthermore, we show that for weak local
reflection strength, a version of the scaling theory of localization holds: the
joint distribution is determined by just three parameters.Comment: 23+15 pages, 10 figures. Longer version of arXiv:2210.0799