I'm reading Tensor Methods in Statistics by McCullagh 1987, (P209 for this question) and I can't understand one step he uses.
He begins with the usual log-likelihood \begin{equation*} l(\theta; Y) = \sum_i l(\theta;Y_i). \end{equation*} And then writes "It is convenient in the calculations that follow to make the dependence on n explicit by writing \begin{equation*} \frac{\partial\mathcal{L}(\beta)}{\partial\beta^r}= U_r = n^\frac{1}{2} Z_r, \end{equation*} \begin{equation*} \frac{\partial^2\mathcal{L}(\beta)}{\partial\beta^r \partial\beta^s} = U_{rs} = n\kappa_{rs} + n^\frac{1}{2} Z_{rs}, \end{equation*} \begin{equation*} \frac{\partial^3\mathcal{L}(\beta)}{\partial\beta^r \partial\beta^s\partial^t} = U_{rst} = n\kappa_{rst} + n^\frac{1}{2} Z_{rst}, \end{equation*} and so on for the higher-order derivatives."
My question is where does this relationship come from? $\kappa$ are the cumulants, but he doesn't explicitly say what $Z$ is, but I believe they might be observations. Please can someone verify/explain how he's written the partial derivatives in this way?