I'm having some trouble manipulating these expressions to reach the following conclusion:
Let $d_1 = \gcd(a,b), d_2 = \gcd(b,c), d_3 =\gcd(c,a), D = \gcd(a,b,c), L=\lcm(a,b,c)$. Prove that:
$$L = \frac{abcD}{d_1d_2d_3}$$
Using some previous exercises in the book, I can rewrite $d_1, d_2, d_3, D$ and $L$ as:
$$d_1 = t_1^{\alpha_1}...t_v^{\alpha_v}$$ $$d_2 = t_1^{\beta_1}...t_v^{\beta_v}$$ $$d_3 = t_1^{\gamma_1}...t_v^{\gamma_v}$$ $$D = t_1^{\zeta_1}...t_v^{\zeta_v}$$ $$L = t_1^{\mu_1}...t_v^{\mu_v}$$
where each $t_i$ is a factor of at least one of $a,b,c$, and $\alpha_i$, $\beta_i$, $\gamma_i$, and $\zeta_i$ are the smallest powers for their corresponding $\gcd$ (e.g. $\alpha_1$ is the smaller of the two powers of factor $t_i$ that $a$ and $b$ have). Conversely, $\mu_i$ is the greatest exponent between $a,b,c$. It is here that I'm getting stuck. I've substituted these expressions into the equation for $L$, but something about the manipulation is throwing me off. I'm trying to logically work out what, say, $t_i^{\frac{\alpha_i+\beta_i+\gamma_i}{\mu_i}}$ is, but going from that to demonstrating the equality is not computing. Any suggestions would be sincerely appreciated.