What does the notation $L/K$ for a field extension exactly specify? In group theory, such an object would be the group of cosets of a normal subgroup $K$ of a group $L$ and a similar usage exists for quotient rings.
In field theory however, I have the impression that the object $L/K$ is the field $L$ itself and that the notation only tells us that we want to talk about elements of the subfield $K$ as well. Is this correct or did I miss something?
A field extension $L/K$ is not a quotient in any sense. It just (confusingly) uses the same notation.
When we talk about a field extension $L/K$, we mean that $K\subset L$ as fields. Sometimes, you might find the terminology $L/K$ used to mean that there is a field homomorphism $$ K\hookrightarrow L $$
(exercise - why is this the same sort of thing?) But it is never a quotient.
We like to talk about $L$ being a field extension over $K$, so we use the normal notation for over - $/$ (as in $2/4 = 2 \textit{ over } 4$).
At least at a basic level, writing
tells us nothing more than writing
The distinction is that the extension $L/K$ has interesting structure in its own right (for example, $L$ is a $K$-vector space). You'll get used to this as you do more field theory.