Let be a metric measure space satisfying both the geometrically doubling and the upper doubling conditions. Let $\rho\in (1,\infty)0<p\le1\le q\le\inftyp\neq q\gamma\in[1,\infty)\epsilon\in(0,\infty)$. In this article, the authors introduce the atomic Hardy space and the molecular Hardy space ${\widetilde H_{\rm{mb},,\rho}^{p,,q,,\gamma,,\epsilon}(\mu)}$ via the discrete coefficient , and prove that the Calder'on-Zygmund operator is bounded from ${\widetilde H_{\rm{mb},,\rho}^{p,,q,,\gamma,,\delta}(\mu)}{\widetilde H_{\rm{atb},,\rho}^{p,,q,,\gamma}(\mu)}L^p(\mu){\widetilde H_{\rm{atb},,\rho(\rho+1)}^{p,,q,,\gamma+1}(\mu)}{\widetilde H_{\rm{mb},,\rho}^{p,,q,,\gamma,,\frac12(\delta -\frac{\nu}{p}+\nu)}(\mu)}$ whose genealized fractional versions are also obtained. The authors also introduce the -weakly doubling condition, with , of the measure and construct a non-doubling measure satisfying this condition. If is -weakly doubling, the authors further introduce the Campanato space ${\mathcal E}^{\alpha,,q}{\rho,,\eta,,\gamma}(\mu){\mathcal E}^{\alpha,,q}{\rho,,\eta,,\gamma}(\mu)\rho\eta\gammaq$; the authors then introduce the atomic Hardy space and the molecular Hardy space , which coincide with each other; the authors finally prove that is the predual of . Moreover, relations of these Hardy spaces are also discussed.

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