I am reading Nigel Hitchin's [notes](https://arxiv.org/pdf/math/9907034.pdf) to understand about gerbes.


It starts the article by saying the following :



> 
> Before giving a definition, it’s worthwhile to recognize when we, as
> mathematicians, might be in a situation where the language of gerbes
> could be relevant. We are basically in gerbe territory (for smooth
> manifolds) if a ny one of the following is being considered:
> 
> 
> * a cohomology class in $H^3(X,\mathbb{Z})$
> * a Cech cocycle $[g\_{\alpha\beta\gamma}]\in H^2(X,C^\infty(S^1))$
> 
> 
> In the last case, this means a 2-cocycle for the sheaf of germs of
> $C^\infty$ functions with values in the circle.
> 
> 
> 


Here, sheaf $C^\infty(S^1)$ on $X$ defined as $C^\infty(S^1)(U)=\{\text{smooth }f:U\rightarrow S^1 \}$ for open $U\subseteq X$.



> 
> To understand gerbes, we need to consider the other creatures in a hierarchy to which gerbes belong, and here the lowest form of life consists of circle valued functions $f:X\rightarrow S^1$. Consider the following features of such a function:
> 
> 
> * a cohomology class in $H^1(X,\mathbb{Z})$
> * a Cech cocycle $[g\_\alpha]\in H^0(X,C^\infty(S^1))$
> 
> 
> The next step in hierarchy consists of unitary line bundle $L$, or its
> principal $S^1$ bundle of unitary frames. Here we have
> 
> 
> * a cohomology class in $H^2(X,\mathbb{Z})$.
> * a Cech cocycle $[g\_{\alpha\beta}]\in H^1(X,C^{\infty}(S^1))$
> 
> 
> 


I dont know what a unitary line bundle is. I only know what is a line bundle. I am guessing unitary line bundle is the one whose transition functions takes values in $S^1$ and not just in $\mathbb{C}^\*$.


Given a line bundle $\pi:L\rightarrow X$, we have trivialization cover $\{U\_\alpha\}=\mathcal{U}$ with trivializations $pi^{-1}(U\_\alpha)\times U\_\alpha\times \mathbb{C}$ and corresponding transition funcions $g\_{\alpha\beta}:U\_\alpha\cap U\_\beta\rightarrow S^1$. So, we have $(g\_{\alpha\beta})\in \mathcal{C}^1(\mathcal{U},C^{\infty}(S^1))$. We also have $g\_{\alpha\beta}g\_{\beta\gamma}=g\_{\alpha\gamma}$ on $U\_\alpha\cap U\_\beta\cap U\_\gamma$.
This says that $\underline{g}=(g\_{\alpha\beta})\in \mathcal{C}^1(\mathcal{U},C^{\infty}(S^1))$ is actaully a $1$ cocycle in the sense of Cech cocycles. This gives an element in first Cech cohomology $H^1(X,C^{\infty}(S^1))$.


It says further that



> 
> Now take an open covering of $X$ and a map $g\_{\alpha\beta\gamma}:U\_\alpha\cap U\_\beta\cap U\_\gamma\rightarrow S^1$ on each threefold intersection with $g\_{\alpha\beta\gamma}=g\_{\beta\alpha\gamma}^{-1}=g\_{\alpha\gamma\beta}^{-1}=g\_{\gamma\beta\alpha}^{-1}$ and satisfying the cocycle condition $$g\_{\beta\gamma\delta}g\_{\alpha\gamma\delta}^{-1}g\_{\alpha\beta\delta}g\_{\alpha\beta\gamma}^{-1}=1 \text{ on } U\_\alpha\cap U\_\beta\cap U\_\gamma\cap U\_\delta.$$
> We shall say that this data defines a gerbe. By this we mean that it suffices to define a gerbe in the same way that a collection of transition functions defines a line bundle or a collection of coordinate charts defines a manifold.
> 
> 
> 


I understand that we are trying to go a step above to second Cech cohomology group to define a gerbe. So, we need to give an element of $\mathcal{C}^2(\mathcal{U},C^{\infty}(S^1))$ that is a $2$ cocycle. This only means that we are asked to give $\overline{g}=(g\_{\alpha\beta\gamma})$ with
$g\_{\alpha\beta\gamma}\in C^{\infty}(S^1)(U\_\alpha\cap U\_\beta\cap U\_\gamma)$ such that $$g\_{\beta\gamma\delta}g\_{\alpha\gamma\delta}^{-1}g\_{\alpha\beta\delta}g\_{\alpha\beta\gamma}^{-1}=1 \text{ on } U\_\alpha\cap U\_\beta\cap U\_\gamma\cap U\_\delta$$ which is just the multiplicative version of coycle condition.


Can some one help me to realize why to impose the condition $$g\_{\alpha\beta\gamma}=g\_{\beta\alpha\gamma}^{-1}=g\_{\alpha\gamma\beta}^{-1}=g\_{\gamma\beta\alpha}^{-1}$$ on threefold intersection. I understand that if we allow $\underline{g}$ to be a $2$ couboundary then this condition holds true but I am sure we are not allowing $\overline{g}$ to be a $2$ coboundary, otherwise cohomology class of $\overline{g}$ would just be $0$.


So, what is happening here when they impose condition $g\_{\alpha\beta\gamma}=g\_{\beta\alpha\gamma}^{-1}=g\_{\alpha\gamma\beta}^{-1}=g\_{\gamma\beta\alpha}^{-1}$?


Is this some generalization of a condition in case of $1$ coycles seen above? If so, can some one suggest me the way to see this?



Confusion in definition of Gerbes in Hitchin's notes
Isn't the condition you mention just saying that the $g\_{\alpha\beta\gamma}$ depends only on the corresponding intersection and not on the order in which the three sets are listed in writing down that intersection, mod transposition of any two. It is thus a normalisation condition, like saying $g\_{\alpha \beta}=g\_{\beta\alpha}^{-1}$ or $g\_{\alpha\alpha}=1$. Are you thinking it is more than that? If you know about Cech complexes and simplicial objects this is like a `compatibility with degeneracy' condition together with a symmetry condition. (I personally like the clarity that comes, for me, with using simplicial objects, although some people find the notation can get in the way.)


It may help to compare Hitchin's treatment with that of Larry Breen in
<https://arxiv.org/abs/math/0611317>


or 


<https://link.springer.com/chapter/10.1007/978-1-4419-1524-5_5>


Looking at several treatments will I am sure help resolve the difficulty. 


As an aside it is interesting / fun to look at case in which the order of intersection does influence the assignment, i.e. in which $g\_{\alpha\beta}$ need not be $g\_{\beta\alpha}^{-1}$, as that to a limited extent reflects a more 'quantum theoretic' viewpoint in that an `observation' corresponding to $U\_{\alpha}$ followed by one corresponding to $U\_\beta$ need not be the same as when the observations are done in the opposite order.


