Here's one way to get the hypergeometric function for the "simpler" equation:

Consider the operator $x^3 (1 + t\partial_t)(\partial^3_{xxx} + \frac{6}x \partial^2_{xx} + \frac{6}{x^2} \partial_x)$, we can rewrite it as 
$$ (1 + T)(X+2)(X+1)X $$
where $T = t\partial_t$ and $X = x\partial_x$. These two operators have $t^\alpha$ and $x^\beta$ as eigenfunctions. 

Your simpler equation is 
$$ (1 + T)(X + 2)(X + 1) X A + x^3 t A = 0 $$
assuming there is a series expansion of the form 
$$ A = \sum c_{\alpha\beta} x^\alpha t^\beta $$
the equation reduces to the recurrence
$$ \alpha(\alpha + 1)(\alpha + 2) (1+\beta) c_{\alpha\beta} + c_{(\alpha-3)(\beta-1)} = 0$$
Your boundary conditions (at $x = 0$ and at $t = 0$) would require 
$$ c_{00} = 1, \quad  c_{\alpha 0 } = c_{0\beta} = 0 \text{ for } \alpha,\beta > 0 $$
This implies that the only non-vanishing terms are those for which $\alpha = 3 \beta$; writing $b_\beta = c_{3\beta,\beta}$ the recurrence is 
$$ 3\beta(3\beta + 1)(3\beta + 2)(\beta + 1) b_\beta = - b_{\beta - 1} $$
This procedure actually gets a somewhat simpler power series, 
$$ A(x,t) = A_{\mathrm{simp}}(x,t) = \sum_{k = 0}^\infty \frac{(-1)^k\cdot 2}{(3k+2)! (k+1)!} x^{3k}t^k $$ 
(which is of course equivalent to your hypergeometric series expansion)

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Note, however, your initial data provides no information on those $c_{\alpha\beta}$ with $\alpha = \{1,2\}$ and $\beta > 0$. Here we've made a **choice** to set such $c_{\alpha\beta} = 0$. For each such choice one gains another series solution. Essentially the issue is that your equation is third order in $x$ within your principal part, and so you do expect needing to prescribe the 0th, first, and second derivatives in the $x$ direction for boundary conditions. 

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For the original problem, the equation is

$$ (1 + T)(X+2)(X+1)X A + \frac{x^3t}{(1-x)^3} A = 0 $$

Let's set $\xi := \frac{x}{1-x}$ and try to expand $A$ in series form as 
$$ A = \sum c_{\alpha\beta} \xi^\alpha t^\beta$$
Conveniently we find that
$$ X(\xi) = \xi + \xi^2$$
which leads to the following recursion relation (where I use the [Pochhammer symbol notation](https://en.wikipedia.org/wiki/Falling_and_rising_factorials))
$$ (1+\beta)(2+\alpha)_3 c_{\alpha\beta} + 3(1+\beta)(1+\alpha)_3 c_{(\alpha-1)\beta} + 3(1+\beta) (\alpha)_3 c_{(\alpha-2)\beta} + (1+\beta)(\alpha-1)_3 c_{(\alpha - 3)\beta} + c_{(\alpha - 3)(\beta-1)} = 0 $$

The coefficients can be uniquely solved if one prescribes the boundary conditions $c_{00} = 0$, $c_{\alpha 0} = c_{0\beta} = 0$ for all $\alpha, \beta> 1$ (as you did) _augmented_ with the choice that $c_{1\beta} = c_{2\beta} = 0$ for all $\beta$. 

Unfortunately, the decay property of the coefficients is somewhat worse (at least, I cannot prove that it is better). In the "simplified problem" you have that as a function of $x^3 t$ the corresponding series has an infinite radius of convergence; this is reflected in you having found a way to write the solution as a hypergeometric function. 

For the recursion relation in the present problem, the best I can do is something like $|c_{\alpha\beta}| \leq \frac{M^{(\alpha - 3\beta - 1)_+}}{\beta! (3\beta)!}$ (maybe not quite right, just did it very quickly), where $M$ is a global constant. If true this will allow the series to converge for all $\xi \lesssim \frac{1}{M}$ (and all $t$). 

Assuming what I wrote above is correct, this will also justify your expectation that "as $\xi \to 0$ the solution converges to $A_{\mathrm{simp}}$ of the simplified problem."