I have the following situation:$$ f_1(x_1) + f_1(x_2) + f_1(x_3) + \cdots + f_1(x_n) = c_1\\ f_2(x_1) + f_2(x_2) + f_2(x_3) + \cdots + f_2(x_n) = c_2\\ \vdots\\ f_n(x_1) + f_n(x_2) + f_n(x_3) + \cdots + f_n(x_n) = c_n $$These formulae are evaluated at a particular vector $\vec{x}$, producing a vector $\vec{c}$ of constants. Now, given this vector $\vec{c}$, I want to reconstruct the original $\vec{x}$. What $f_i$s should I choose that will let me do this?
There are two constraints: $f_i$ is bounded on $(0,1)$ and $\left[f_i(x_j)=0\right] \rightarrow \left[x_j \in \{0,1\}\right]$ (and $f_i(x_j)$ is $0$ in at least one point).
There are, however, some simplifying assumptions. Each $x_i \in [0,1]$ and $\left[x_i=x_j\right] \rightarrow \left[\left[i=j\right] \vee \left[f_k(x_i)=f_k(x_j)=0\right]\right]$. Furthermore, the order of the components of $\vec{x}$ is irrelevant (that is, reconstructing any permutation of $\vec{x}$ is fine).
A closed-form solution is ideal, but a numerical solution scaling gracefully with $n$ is acceptable too. Partial solutions for $n \geq 4$ will be accepted if there is no general approach.
I have tried a number of things, but my best attempt so far is the rather basic:$$ f_i(x_j) := x_j^{i} $$So that we have:$$ f_1(x_j) := x_j^1\\ f_2(x_j) := x_j^2\\ \vdots\\ f_n(x_j) := x_j^n $$Viewed this way, each equation represents an $n$-dimensional superquadric. For $n=2$, a closed form exists (intersection of line with circle quadrant). For $n=3$, I used multidimensional Newton iteration. However, for $n=4$, the solver fails to converge (or at least has numerical issues).
The question again: What is a good choice of $f_i$ such that I can reconstruct $\vec{x}$ given $\vec{c}$?