An extended comment, answering the question asked by fedja in one of the comments. (Edited: In order to simplify the example I chose to work in dimension two, but this example requires dimension at least three.)
My bet was incorrect: I am very surprised to find that the answer is negative! In order to construct a counterexample (in dimension 3, for simplicity), consider two independent random walks: $A_n$ the simple random walk in $\mathbb{Z}$, and $B_n$ a random walk with symmetric $\alpha$-stable distribution in $\mathbb{R}^2$ for some $\alpha \in (1, 2)$. Fix $\epsilon > 0$. We have $$|B_n| \geqslant n^{1/\alpha - \epsilon}$$ for all $n$ large enough (see Corollary 2 in Takeuchi, doi:10.2969/jmsj/01620109). Furthermore, by LIL, $$A_n \ge -n^{1/2 + \epsilon}$$ for all $n$ large enough. Choosing $\epsilon > 0$ small enough, we find that for an arbitrary constant $p > 0$, $$p A_n + |B_n| \geqslant 0$$ for all $n$ large enough. In other words, with probability one the random walk $(A_n, B_n)$ visits the cone $\{(a, b) \in \mathbb{R} \times \mathbb{R}^2 : p a + |b| < 0\}$ finitely many times.
It remains to choose $p$ and rotate $(A_n, B_n)$ appropriately, so that the above cone fits into the negative octant. To be specific, we set $$X_n = A_n \vec{v}_1 + B_{n,1} \vec{v}_2 + B_{n,2} \vec{v}_3, $$ where $\vec{v}_1 = \tfrac{1}{\sqrt{3}} (1, 1, 1)$ and otherwise $\vec{v}_1, \vec{v}_2, \vec{v}_3$ are arbitrary orthonormal vectors in $\mathbb{R}^3$. Then, by an easy calculation, $$ \max\{X_{n,1}, X_{n,2}, X_{n,3}\} \geqslant \tfrac{1}{\sqrt{3}} A_n + \tfrac{1}{\sqrt{6}} |B_n| \ge 0 $$
for all $n$ large enough (by choosing $p = \sqrt{2}$ above). This means that there is $k < 0$ such that with positive probability we have $X_{n,j} \geqslant k$ for every $j = 1, 2, 3$ and every $n = 0, 1, \ldots$