There's an easy counterexample to your guess: Let $M^6 = \mathrm{SU}(3)/\mathbb{T}^2$, where $\mathbb{T}^2\subset\mathrm{SU}(3)$ is the maximal torus (for example, the diagonal subgroup). In that case, there is a 3-parameter family of non-isometric metrics on $M^6$ that are invariant under $\mathrm{SU}(3)$, so they are not unique up to a constant (or even non-constant) scalar factor.
I imagine that $M^6$ does not carry a metric whose isometry group has dimension greater than $8=\dim\mathrm{SU}(3)$, but I don't have a proof handy.
On the other hand, it is true that any Riemannian metric on $\mathbb{CP}^n$ whose isometry group has dimension at least $n(n{+}2)$ must be isometric to a constant scalar multiple of the Fubini-Study metric. Here is one argument:
Suppose that a connected, compact group $G$ acts effectively and smoothly on $\mathbb{CP}^n$. Then, by averaging, there exists a $G$-invariant metric $g$. Moreover, since $H^2_{dR}(\mathbb{CP}^n,\mathbb{R})\simeq\mathbb{R}$, it follows from the Hodge Theorem that there is a $g$-harmonic $2$-form $\omega$ that represents a generator of $H^2_{dR}(\mathbb{CP}^n,\mathbb{R})$, and it is unique up to constant multiples. Since $G$ is connected, it follows that it must leave $\omega$ fixed. Moreover, because of the structure of the cohomology ring of $\mathbb{CP}^n$, the top-degree form $\omega^n$ must represent a generator of $H^{2n}_{dR}(\mathbb{CP}^n,\mathbb{R})$. In particular, $\omega^n$ does not vanish identically.
Thus, there is a point $p\in\mathbb{CP}^n$ such that $\omega_p\in \Lambda^2(T^*_pM)$ is a 2-form of full rank. Now considerConsider the stabilizer $G_p\subset G$ of $p$. Since $G$ acts by isometries and $\mathbb{CP}^n$ is connected, it follows that $G_p$ injects into $\mathrm{O}(T_pM)$ and, moreoverby identifying $g\in G_p$ with $g'(p):T_pM\to T_pM$. Moreover, must leave $G_p$ leaves $\omega_p$ fixed. In particular Thus, $G_p$ must lie inside a subgroup of $\mathrm{O}(T_pM)$ that fixes a complex structure $J:T_pM\to T_pM$ and hence must have dimension at most $\dim \mathrm{U}(n) = n^2$. Thus Now, we have $$ \dim G = \dim G_p + \dim G{\cdot}p \le n^2 + 2n = n(n{+}2). $$$$ \dim G = \dim G_p + \dim G/G_p = \dim G_p + \dim G{\cdot}p \le n^2 + 2n = n(n{+}2). $$ If equality holds, then $\dim G_p = n^2$ and $G{\cdot}p = \mathbb{CP}^n$$\dim G{\cdot}p = 2n = \dim \mathbb{CP}^n$. Since Thus, the orbit $G{\cdot}p$ is both open and closed in $\mathbb{CP}^n$, so $G$ acts transitively on $\mathbb{CP}^n$, it. It follows that $\omega$ is everywhere of full rank and, after scaling $\omega$ so that it has comass 1, we have that $\omega(u,v) = g(Ju,v)$ for a unique almost-complex structure $J$ on $\mathbb{CP}^n$ that is preservd by $G_p$, which has the same dimension as the connected group $\mathrm{U}(g_p,J_p)\simeq \mathrm{U}(n)$. Moreover Thus, since$G_p = \mathrm{U}(g_p,J_p)$. Since $G_p$ contains $-I\in\mathrm{O}(T_pM)$$-I\in\mathrm{U}(g_p,J_p)$, it follows that there is an element of $G$ that fixes $p$ and reverses all $g$-geodesics through $p$. Since $G$ acts transitively on $\mathbb{CP}^n$, it follows that $(\mathbb{CP}^n,g)$ is a Riemannian symmetric space. Using the classification, it follows that $G\simeq \mathrm{SU}(n{+}1)$$G\simeq \mathrm{SU}(n{+}1)/Z$ (where $Z\simeq\mathbb{Z}_{n+1}$ is the center of $\mathrm{SU}(n{+}1)$) and that the metric $g$ is, up to isometry, a constant multiple of the standard Fubini-Study metric.