Peace be upon you,
I had the following system of equations to be solved \begin{align*} \begin{cases} \psi(\alpha)-\psi(\alpha+\beta)=c_1\\ \psi(\beta)-\psi(\alpha+\beta)=c_2 \end{cases} \end{align*} where $c_1$ and $c_2$ are constants (I should solve the above, for miscellaneous constant couples). First of all, I wanted to solve it analytically so I tested some ideas and then asked for the solution in the question "A late-diverging "approximating solution" for a system of functional equations"; but after visiting no answer I proceeded to solve it numerically, using the popular approximation of the Digamma function \begin{align*} \psi(x)= \ln(x)-\frac{1}{2x}-\frac{1}{12x^2}+\frac{1}{120x^4}-\frac{1}{252x^6}+\frac{1}{240x^8}-\frac{5}{660x^{10}}+\frac{691}{32760x^{12}}-\frac{1}{12x^{14}}+O\left(\frac{1}{x^{16}}\right) \end{align*} as you can see from the approximation order, the error in 1 can even be 1! and for the values less that 1 the story is worse; while the answer of my system ($\alpha$ and $\beta$) maybe in this interval ($(0,1]$). I wonder if someone can present a better approximation of the Beta function which can cope my task for such values.
Any lighting up ideas?

An approximation close to $1$ (i.e. $x=1+\epsilon$ ) is given below (from WolframAlpha) :
For more accuracy, you can use the Taylor's expansion : $$\psi(1+\epsilon)=\Sigma_{n=0}^{\infty} \frac{\psi^{(n)}(1)}{n!}\epsilon^n$$ with numerical values of $\psi^{(n)}(1)$