Since the pair of equations for deforming a pair of foliations is a pair of PDSs involving the beltrami coefficients, I checked to see whether they were simpler to work with if the beltrami coefficients were in turn represented as a ratio involving ∂ˉz and ∂z but that didn’t help.
I had worked out a series solution to them years ago, looking for simple solutions. The simple solutions all looked like they turned out to be trivial as I recall (i.e. no different than a deformation of each coordinate separately).
However, I went ahead and wrote out the series solution again just because the PDEs involved obviously have a series solution, and PDE’s can be hard to solve.
If b1 and b2 are the beltrami coefficients of the horizontal and vertical holomorphic leaves, the PDE pair is
∂b1∂ˉz2=b2∂b1∂z2
and
∂b2∂ˉz1=b1∂b2∂z1
You can select any two convergent series ∑aijkzi1zj2ˉzk1 and ∑cijkzi1zj2ˉzk2 then there is a nice series relationship that gives you actual solutions b1 and b2 as an infinite series. The series solution is nicer if you actually represent b1 and b2 as
b1=∑Aijˉzi1ˉzj2
and
b2=∑Cijˉzi1ˉzj2
Of course, where resulting series converges is a different matter altogether. But it appears this gives lots of solutions to the system of PDEs. For example, if the constants aijk and cijk get small very rapidly, this method would give you convergent solutions to the PDE.
∂b1∂ˉz2=b2∂b1∂z2
and
∂b2∂ˉz1=b1∂b2∂z1
You can select any two convergent series ∑aijkzi1zj2ˉzk1 and ∑cijkzi1zj2ˉzk2 then there is a nice series relationship that gives you actual solutions b1 and b2 as an infinite series. The series solution is nicer if you actually represent b1 and b2 as
b1=∑Aijˉzi1ˉzj2
and
b2=∑Cijˉzi1ˉzj2
where Aij and Cij are holomorphic functions.
You then get the relationships:
(j+1)Ai,j+1=∑k≤i,ℓ≤j∂Akℓ∂z2Ci−k,j−ℓ
(i+1)Ci+1,j=∑k≤i,ℓ≤j∂Ckℓ∂z1Ai−k,j−ℓ
This recursive relationship requires that you specify each Ai0 and each C0j as a holomorphic function.
Now, of course, there are many solutions, because one can simply take two transverse holomorphic motions and turn them into a deformation by treating them as a coordinate system. That is, take two different pairs of transverse foliations. For each foliation in each pair choose a leaf. Choose a way to match the selected two leaves that came from one pair with the selected two leaves that came from the other pair. Now extend by treating the transverse foliations as giving coordinates.
The PDE is written for the case where one of these pairs is simply the regular horizontal and vertical leaves, and we are specifying beltrami coefficients to deform the structure of those leaves.
So there are lots of solutions. But it is interesting to have solutions specified by beltrami coefficients. It means you can deform an existing structure and still have a holomorphic space.