Suppose we have $n$ Goldstone bosons which is obtained from the fact that the ground state $\eta$ is invariant under a subgroup $H$ of $G$. Each of these Goldstone bosons will be described by an independent field $\phi_{i}$ which is a smooth real function on Minkowski space $M^{4}$. These fields are collected in an $n$ -component vector $\Psi=\left(\phi_{1}, \ldots, \phi_{n}\right)$, defining the real vector space
$$
V \equiv\left\{\Psi: M^{4} \rightarrow \mathbb{R}^{n} \mid \phi_{i}: M^{4} \rightarrow \mathbb{R} \text { smooth }\right\}
$$
Now we define the map $F:G\times V \longrightarrow V$ by
\begin{gathered} F(e, \Psi)=\Psi \quad \forall \quad \Psi \in V, \quad e \text { identity of } G \\ F\left(g_{1}, F\left(g_{2}, \Psi\right)\right)=F\left(g_{1} g_{2}, \Psi\right) \quad \forall \quad g_{1}, g_{2} \in G, \quad \forall \quad \Psi \in V \end{gathered}
For the subgroup $H$ of $G$ the set $g H=\{g h \mid h \in H\}$ defines the left coset of $g$ and we define $G / H=\{g H \mid g \in G\}$ to be the set of all left cosets.
Now let $F':G / H \times V \longrightarrow V$ and $0\in V$. We have that $0$ is mapped onto the same vector in $\mathbb{R}^{n}$ under all elements of a given coset $g H$ since $$ F'(g h, 0)=F(g, F(h, 0))=F(g, 0) \quad \forall \quad g \in G \quad \text { and } \quad h \in H $$ The map is injective since for two elements $g$ and $g^{\prime}$ of $G$ where $g^{\prime} \notin g H$. Let us assume $F'(g, 0)=F'\left(g^{\prime}, 0\right)$ : $$ 0=F'(e, 0)=F(e, 0)=F\left(g^{-1} g, 0\right)=F\left(g^{-1}, F(g, 0)\right)=F\left(g^{-1}, F\left(g^{\prime}, 0\right)\right)=F\left(g^{-1} g^{\prime}, 0\right) $$ However, this implies $g^{-1} g^{\prime} \in H$ or $g^{\prime} \in g H$ in contradiction to the assumption $g^{\prime} \notin g H$ and therefore $F'(g, 0)=F'\left(g^{\prime}, 0\right)$ cannot be true. Let $n_G$ be the dimension of the lie group G and $n_h$ the dimension of the lie subgroup $H$. Goldstone theorem says that $n=n_G-n_h$. But it is a fact that for lie groups we have the dimension of $G / H$ is $n_{G / H}=n_G-n_h$
From the considerations above in this notes A Chiral Perturbation Theory Primer they claim that there exists an isomorphic mapping between the quotient $G / H$ and the Goldstone-boson fields.
But I am not seeing the isomorphism since $G / H$ has $n$ elements and the $V$ has infinite elements.
Am I missing something here?