I am wondering how to show looking obvious $\mathbb{Q}(2^{\frac{1}{3}}) \ne \mathbb{Q}(3^{\frac{1}{3}}) $?
This question has appeared to compute the order of $\text{Gal}(\mathbb{Q}(2^{\frac{1}{3}},3^{\frac{1}{3}},\xi_3)/\mathbb{Q})$ where $\xi_3$ is a primitive root of unity.
I already know to show this by brutal force by assumimg $2^{\frac{1}{3}}=a+b\cdot2^{\frac{1}{3}}+c\cdot 2^{\frac{2}{3}}$ for some $a,b,c\in \mathbb{Q}$ and take 3rd power on both side and compare their coefficients. But its too boring.
Is there any neat method?
We can argue using the field trace. Consider $ K = \mathbb{Q}(2^{1/3}) $ and $ L = \mathbb{Q}(2^{1/3}, \zeta_3) $ where $ \zeta_3 $ is a primitive third root of unity. $ L $ is the normal closure of $ K $. Now, assume that we had $ 3^{1/3} \in K $, then we would have
$$ 3^{1/3} = c_0 + c_1 2^{1/3} + c_2 2^{2/3} $$
for some $ c_k \in \mathbb{Q} $. Let $ T = \textrm{Tr}_{L/\mathbb{Q}} $ denote the field trace, defined by
$$ T(x) = \sum_{\sigma \in \textrm{Gal}(L/\mathbb{Q})} \sigma(x) $$
The properties $ T(cx) = c T(x) $ for rational $ c $ and $ T(x) = 0 $ iff $ x = 0 $ for rational $ x $ are evident. Now, note that applying $ T $ to both sides of the relation yields $ c_0 = 0 $. Multiply both sides by $ 2^{1/3} $ to get
$$ 6^{1/3} = c_1 2^{2/3} + 2c_2 $$
and apply the field trace to both sides again to get $ c_2 = 0 $. These results imply that we must have $ (3/2)^{1/3} \in \mathbb{Q} $; impossible. Thus, $ 3^{1/3} \notin K $ after all.