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For $p>p_0=\frac{2\lambda}{2\lambda+1}$ with $\lambda>0$, the Hardy space$H_{\lambda}^p(\mathbb R_+^2)$ associated with the Dunkl transform$\mathcal{F}_\lambda$ and the Dunkl operator $D$ on the real line $\mathbb R$,where $D_xf(x)=f'(x)+\frac{\lambda}{x}[f(x)-f(-x)]$, is the set of functions$F=u+iv$ on the upper half plane $\mathbb R^2_+=\left\{(x, y): x\in\mathbb R,y>0\right\}$, satisfying $\lambda$-Cauchy-Riemann equations: $ D_xu-\partial_yv=0$, $\partial_y u +D_xv=0$, and $\sup\limits_{y>0}\int_{\mathbbR}|F(x+iy)|^p|x|^{2\lambda}dx<\infty$. In this paper, we will give a furthercharacterization of $H_{\lambda}^p(\mathbb R_+^2)$ in \cite{ZhongKai Li 3}. Weprove the inequality $\|F\|_{H_{\lambda}^p(\mathbb R_+^2)}\leqc\|u_{\nabla}^*\|_{L^p_{\lambda}}$, which gives a Real Characterization of theclass $H_{\lambda}^p(\mathbb R_+^2)$ for $\frac{2\lambda}{2\lambda+1}<p\leq1$as a main result.

The Real Characterization of $H_{\lambda}^p(\mathbb R_+^2)$ for $\frac{2\lambda}{2\lambda+1}