The solution of
$$ x \,\text{sech}(x)=k$$ cannot be explicit and then either numerical methods or approximations.
In your problem, what is interesting is the fact that the range of $x$ is quite limited. Assuming $k \geq 0$, $x$ varies between $0$ and $x_*$ corresponding to the maximum value of the lhs. $x_*$ is the solution of
$$x \tanh(x)=1 \implies e^{-2x}=\frac{x-1}{x+1}$$ and then $x_*$ is explicit in terms of the generalized Lambert function. So, the maximum value of $k$ is
$$k_{\text{max}}=\frac{\sqrt{x_*^2-1} }{x_*}\coth ^{-1}(x_*)$$
We can expand $ x \,\text{sech}(x)$ as an infite series
$$ x \,\text{sech}(x)= \sum_{n=0}^\infty \frac{E_{2 n}}{(2 n)!} x^{2n+1}$$ we can use series reversion to any order. This will give
$$x_{(p)}= \sum_{n=0}^p a_n \, k^{2n+1}+O\left(x^{2p+2}\right)$$
The first coefficients make the sequence
$$\left\{1,\frac{1}{2},\frac{13}{24},\frac{541}{720},\frac{9509}{8064},\frac{7231801}{
3628800},\frac{1695106117}{479001600},\frac{567547087381}{87178291200},\frac{3676
0132319047}{2988969984000},\cdots\right\}$$
To judge the quality, using the limited truncated series given above, give $x$ a value; from it compute $k$ and from $k$ recompute $x$. Here are the results
$$\left(
\begin{array}{cc}
x_{\text{given}} &x_{\text{recomputed}}\\
0.00 & 0.00000000 \\
0.05 & 0.05000000 \\
0.10 & 0.10000000 \\
0.15 & 0.15000000 \\
0.20 & 0.20000000 \\
0.25 & 0.25000000 \\
0.30 & 0.30000000 \\
0.35 & 0.34999998 \\
0.40 & 0.39999980 \\
0.45 & 0.44999859 \\
0.50 & 0.49999245 \\
0.55 & 0.54996756 \\
0.60 & 0.59988397 \\
0.65 & 0.64964481 \\
0.70 & 0.69904911 \\
0.75 & 0.74773420 \\
0.80 & 0.79512362 \\
0.85 & 0.84040336 \\
0.90 & 0.88254661 \\
0.95 & 0.92039514 \\
1.00 & 0.95278735 \\
1.05 & 0.97870666 \\
1.10 & 0.99741676 \\
1.15 & 1.00855418 \\
1.20 & 1.01216141
\end{array}
\right)$$
For sure, above $x=0.75$, the agreement is not fantastic but, again, we could add as many terms as we want. More coefficients on request.
For your example where $k=\frac{125}{267}$, this would give $x=0.537391$ while the solution given by Newton method is $x=0.537414$ (relative error of $0.0043$%). Thsi does not seem too bad.
Edit
As shown above, the approximation is not very good for large alues of $x$. What we can do is to perform a single iteration of Halley method which would give as a better estimate
$$x_1=x_0+\frac{4 (x_0-k \cosh (x_0)) (x_0 \sinh (x_0)-\cosh (x_0))}{k x_0 (\cosh (2 x_0)-3)-4 \sinh (x_0) (k
\cosh (x_0)+x_0)+2 \left(x_0^2+2\right) \cosh (x_0)}$$ $x_0$ being given by the series.
For example, for $x_{\text{given}}=1$, this will give $x_1=0.999460$ which is much better.
Update
For large values of $x$, we can make a series expansion around $x=1$, inverse it and obtain
$$x=1+t+\frac{e^4+6 e^2-3 } {4(1+e^2)}t^2+\frac{3 e^8+32e^6+74e^4-32e^2+19}{24 \left(1+e^2\right)^2}t^3 +O(t^4)$$ where
$$t=\frac{1}{2} \left(1+e^2\right) \cosh (1) (k-\text{sech}(1))$$