  Let $k\in\mathbb{N}$, $\Omega$ be homogeneous of degree zero, integrable on
$S^{d-1}$ and have vanishing moment of order $k$, $a$ be a function on
$\mathbb{R}^d$ such that $\nabla a\in L^{\infty}(\mathbb{R}^d)$, and
$T_{\Omega,\,a;k}$ be the $d$-dimensional Calder\'on commutator defined by
$$T_{\Omega,\,a;k}f(x)={\rm
p.\,v.}\int_{\mathbb{R}^d}\frac{\Omega(x-y)}{|x-y|^{d+k}}\big(a(x)-a(y)\big)^kf(y){d}y.$$
In this paper, the authors prove that if $$\sup_{\zeta\in
S^{d-1}}\int_{S^{d-1}}|\Omega(\theta)|\log ^{\beta}
\big(\frac{1}{|\theta\cdot\zeta|}\big)d\theta<\infty,$$ with
$\beta\in(1,\,\infty]$, then for $\frac{2\beta}{2\beta-1}<p<2\beta$,
$T_{\Omega,\,a;\,k}$ is bounded on $L^p(\mathbb{R}^d)$.
