As I began to teach myself in differential geometry, I finally used to use the Nabla-Operator.
I know and understand its usage as in
$$ \nabla f := \left( \begin{matrix} \frac{∂f}{∂x_1} & \frac{∂f}{∂x_2} & \cdots & \frac{∂f}{∂x_n} \end{matrix} \right)^\intercal $$
but in many books I read a pure definition of $\nabla$: $$ \nabla := \left( \begin{matrix} \frac{∂}{∂x_1} & \frac{∂}{∂x_2} & \cdots & \frac{∂}{∂x_n} \end{matrix} \right) ^ \intercal $$
which seems to be just a visualisation of the content, because it's mathematically false $-$ an equation needs to have two evaluatable terms on both sides, but an operator is not a value.
For example, the derivation operator can conformly be defined as $$ \frac{∂}{∂x_i}: ℝ → ℝ, \quad f ↦ \frac{∂f}{∂x_i} := \lim_{x_i→0}{\frac{f(x_1,\cdots,x_i+h,\cdots,x_n)-f(_1,\cdots,x_i,\cdots,x_n)}{h}} $$
But the Nabla-Operator is applied in multiple ways; therefore, one cannot define it as a function.
Do I suppose rightly that there does not exists an explicit definition, or does there exist some kind of ‘trick’?