Using the so-called angle bisector theorem, one can write
(with usual notations $a,b,c$ for the side lengths $BC,CA,AB$ resp.):
$$\tag{1}\vec{AA_1}=\dfrac{b}{b+c}\vec{AC}+\dfrac{c}{b+c}\vec{AB}$$
In the same way, by cyclic permutation:
$$\vec{BB_1}=\dfrac{c}{c+a}\vec{BA}+\dfrac{a}{c+a}\vec{BC}$$
which can be written:
$$\tag{2}\vec{BB_1}=-\dfrac{c}{c+a}\vec{AB}+\dfrac{a}{c+a}\vec{AC}-\dfrac{a}{c+a}\vec{AB}$$
and finally:
$$\vec{CC_1}=\dfrac{a}{a+b}\vec{CB}+\dfrac{b}{a+b}\vec{CA}$$
which can be written:
$$\tag{3}\vec{CC_1}=\dfrac{a}{a+b}\vec{AB}-\dfrac{a}{a+b}\vec{AC}-\dfrac{b}{a+b}\vec{AC}$$
adding (1)+(2)+(3) gives
$$\tag{4}\vec{AA_1}+\vec{BB_1}+\vec{CC_1}=\alpha \vec{AB}+\beta \vec{AC}$$
with $\alpha=\frac{c}{b+c}-\frac{c}{c+a}-\frac{a}{c+a}+\frac{a}{a+b}=\frac{ac-b^2}{(a+b)(a+c)}$ and
$\beta=\frac{b}{b+c}+\frac{a}{a+c}-\frac{a}{a+b}-\frac{b}{a+b}=\frac{ab-c^2}{(b+c)(a+c)}.$
$\{\vec{AB},\vec{AC} \}$ being a basis of the plane, we will have a zero sum in relationship (4) if and only if the two numerators in the expressions of $\alpha$ and $\beta$ are zero, i.e.,
$ac=b^2$ and $ab=c^2$, whence $\dfrac{a}{b}=\dfrac{b}{c}=\dfrac{c}{a}$ from which, denoting the common value of these ratios by $k$ we obtain $a=kb, b=kc,c=ka$. Thus $k^3=1$ which is equivalent to $k=1$. Consequence: $a=b=c$.