3.C0=0 C1=1

Continuing from the equation

Ci,j+1=kCk,jB^i,k(C)
Ci,j+1C1,jCi,j=k=1i1Ck,jB^i,k

Taking C1=1, it becomes

Ci,j+1Ci,j=k=1i1Ck,jB^i,k

We can list some Ci,j:

i Ci,j
1 1
2 C2j
3 C22j2+(C3C22)j

As we can see, they are polynomials. We can thus guess the model

Ci,j=k=0i1Ai,kjk

Trivial properties:

  • A1,0=1

  • k=0i1Ai,k=Ci

We also have

Ci,j+1=k=0i1Ai,k(j+1)k=k=0jkn=0i1(nk)Ai,n.

Injecting it, we now have

k=0jkn=0i1(nk)Ai,nk=0i1Ai,kjk=k=1i1n=0k1Ak,njnB^i,k
n=0i1(nk)Ai,nAi,k=n=0i1An,kB^i,n
n=k+1i1(nk)Ai,n=n=k+1i1An,kB^i,n

Let n such that k+1=iN

n=iNi1(niN1)Ai,n=n=iNi1An,iN1B^i,n
(iN)Ai,iN(i1)C2Ai1,j1N=n=0N2An+iN,iN1B^i,n+iN(n+iN+1iN1)Ai,n+iN+1

We can do a change of variable such that

Ai,iN=(i1)!(iN)!C2iVN(i)

Injecting it in, leads, after some computation, to

VN(i)VN(i1)=n=0N2B^i,n+iN(n+iN1)!(i1)!C2nNVn+1(n+iN)VNn1(i)(n+2)!
VN(n)=i=N+1nk=0N2B^i,k+iN(k+iN1)!(i1)!C2kNVk+1(k+iN)Vk+1(i)(Nk)!
V1(n)=1C2
V2(n)=C23(C3C22)(Hn1)

with Hn=i=1n1i, the harmonic numbers. V3(n) is already quite complicated and long to be shown here. Let QN(n)=VN(n)C2N+1,

QN(n)=i=N+1nk=0N2B^i,k+iN(k+iN1)!(i1)!C21Qk+1(k+iN)C2Nk1(Nk)!Qk+1(i)

Now let

QN(n)=i(i1)jiU(ji,n)i2Ciji

Injecting it gives

i1ji=NU(jr,n)C2i2Ciji=i=N+1nk=0N2((j1)aj=Nk(j1)bj=k+1(k+iN1)!(k+iN)!(i1)!r=1Nk+1ar!U(bi,k+iN)r2Cr,ar+br(j1)dj=k+1U(dr,i)(Nk)!C2Nkr2Crdr)

Identifying terms, we get

U(ji,n)=m=N+1nk=0N2(U({j2+1+kN;j3;j4;},m)(Nk)!+(i1)a1=Nk(i1)bi=k+1{ai+bi=ji,i>2a2+b2=j2+1((k+mN)!(k+mN1)!(m1)!(m+kNr2ar)!U(br,k+mN)r2ar!))

To simplify formulas, let shift j's by 1 such that j2 is now noted as j1. The fomula then becomes

U(ji,n)=m=N+1nk=0N2(U({j1+1+kN;j2;},m)(Nk)!+ibi=k+1ai+bi=ji,i:1<i<NaN=jNa1+b1=j1+1a10,ibi0,i>1((k+mN)!(k+mN1)!(m1)!(m+kNar)!U(br,k+mN)ar!))

Some properties: Let J(N)={ji=1 if i=N;ji=0 else}, we have

U(J(N),n)=1N2(1(N1)!(nN+1)!(n1)!)
U({N},n)=m=N+1nk=0N21(Nk)!((k+mN)!(k+mN1)!(m1)!(m+2k2N)!U({k+1},k+mN)U({k+1},m))
U({2N;N1},n)m=2N2n1U({3N;N2},m1)m

From this last functions, we will define

FN(n)=i=2N2n1FN1(i1)i

with initial condition

F1(n)=1
J U(J,n)
{0;1} F2(n)
{2} F2(n)
{-1;2} F3(n)
{3} F3(n)321n1+34
{1,1} 521n1542F3(n)
{4} 29727121n225121n1+32(1n112)F2(n2)F4(n)
{1,0,1} 162n1+1n2+F2(n2)(1n112)
{-1;1;1} 512+12(1n+1+1n+2)+F2(n2)(121n1)
{2;1} 3F4(n)+F2(n2)4(121n1)+721n2+121n18372
{0;2} 11122n1121n2+52(1n112)F2(n2)3F4(n)

We can guess the form as

U(jr,n)=l=0N1Kl({jr},n)FNl(nl)

Through some shady techniques, we can find

K0(j1,j2)=(1)j1+j2+1(j1+2j21j2)
K1(j1,j2)=0
K2(j1,j2)=(121n1)(1)j1+j2((j1+2j23j2)52(j1+2j22j2))

This is actually only true if ji=0i>2 as all of those case, create "parralel" solutions, which should respect similar recurence equations but with different initial conditions.

The form should be injected in the equation to find general solutions but the computations is very complicated and I was not able to get through with it at the moment.