Lemma 4.35.2. Let p : \mathcal{S} \to \mathcal{C} be a functor. The following are equivalent
p : \mathcal{S} \to \mathcal{C} is a category fibred in groupoids, and
all fibre categories are groupoids and \mathcal{S} is a fibred category over \mathcal{C}.
Moreover, in this case every morphism of \mathcal{S} is strongly cartesian. In addition, given f^\ast x \to x lying over f for all f: V \to U = p(x) the data (U \mapsto \mathcal{S}_ U, f \mapsto f^*, \alpha _{f, g}, \alpha _ U) constructed in Lemma 4.33.7 defines a pseudo functor from \mathcal{C}^{opp} in to the (2, 1)-category of groupoids.
Proof.
Assume p : \mathcal{S} \to \mathcal{C} is fibred in groupoids. To show all fibre categories \mathcal{S}_ U for U \in \mathop{\mathrm{Ob}}\nolimits (\mathcal{C}) are groupoids, we must exhibit for every f : y \to x in \mathcal{S}_ U an inverse morphism. The diagram on the left (in \mathcal{S}_ U) is mapped by p to the diagram on the right:
\xymatrix{ y \ar[r]^ f & x & U \ar[r]^{\text{id}_ U} & U \\ x \ar@{-->}[u] \ar[ru]_{\text{id}_ x} & & U \ar@{-->}[u]\ar[ru]_{\text{id}_ U} & \\ }
Since only \text{id}_ U makes the diagram on the right commute, there is a unique g : x \to y making the diagram on the left commute, so fg = \text{id}_ x. By a similar argument there is a unique h : y \to x so that gh = \text{id}_ y. Then fgh = f : y \to x. We have fg = \text{id}_ x, so h = f. Condition (2) of Definition 4.35.1 says exactly that every morphism of \mathcal{S} is strongly cartesian. Hence condition (1) of Definition 4.35.1 implies that \mathcal{S} is a fibred category over \mathcal{C}.
Conversely, assume all fibre categories are groupoids and \mathcal{S} is a fibred category over \mathcal{C}. We have to check conditions (1) and (2) of Definition 4.35.1. The first condition follows trivially. Let \phi : y \to x, \psi : z \to x and f : p(z) \to p(y) such that p(\phi ) \circ f = p(\psi ) be as in condition (2) of Definition 4.35.1. Write U = p(x), V = p(y), W = p(z), p(\phi ) = g : V \to U, p(\psi ) = h : W \to U. Choose a strongly cartesian g^*x \to x lying over g. Then we get a morphism i : y \to g^*x in \mathcal{S}_ V, which is therefore an isomorphism. We also get a morphism j : z \to g^*x corresponding to the pair (\psi , f) as g^*x \to x is strongly cartesian. Then one checks that \chi = i^{-1} \circ j is a solution.
We have seen in the proof of (1) \Rightarrow (2) that every morphism of \mathcal{S} is strongly cartesian. The final statement follows directly from Lemma 4.33.7.
\square
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