Let Aωp\documentclass[12pt]{minimal}
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\begin{document}$$A^p_\omega $$\end{document} denote the Bergman space in the unit disc D\documentclass[12pt]{minimal}
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\begin{document}$$\mathbb {D}$$\end{document} of the complex plane induced by a radial weight ω\documentclass[12pt]{minimal}
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\begin{document}$$\omega $$\end{document} with the doubling property ∫r1ω(s)ds≤C∫1+r21ω(s)ds\documentclass[12pt]{minimal}
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\begin{document}$$\int _{r}^1\omega (s)\,ds\le C\int _{\frac{1+r}{2}}^1\omega (s)\,ds$$\end{document}. The tent space Tsq(ν,ω)\documentclass[12pt]{minimal}
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\begin{document}$$T^q_s(\nu ,\omega )$$\end{document} consists of functions such that ‖f‖Tsq(ν,ω)q=∫D∫Γ(ζ)|f(z)|sdν(z)qsω(ζ)dA(ζ)<∞,0<q,s<∞.\documentclass[12pt]{minimal}
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\begin{document}$$\begin{aligned} \begin{aligned} \Vert f\Vert _{T^q_s(\nu ,\omega )}^q =\int _\mathbb {D}\left( \int _{\varGamma (\zeta )}|f(z)|^s\,d\nu (z)\right) ^\frac{q}{s}\omega (\zeta )\,dA(\zeta ) <\infty ,\quad 0<q, \; s<\infty . \end{aligned} \end{aligned}$$\end{document}Here Γ(ζ)\documentclass[12pt]{minimal}
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\begin{document}$$\varGamma (\zeta )$$\end{document} is a non-tangential approach region with vertex ζ\documentclass[12pt]{minimal}
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\begin{document}$$\zeta $$\end{document} in the punctured unit disc D\{0}\documentclass[12pt]{minimal}
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\begin{document}$$\mathbb {D}{\setminus }\{0\}$$\end{document}. We characterize the positive Borel measures ν\documentclass[12pt]{minimal}
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\begin{document}$$\nu $$\end{document} such that Aωp\documentclass[12pt]{minimal}
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\begin{document}$$A^p_\omega $$\end{document} is embedded into the tent space Tsq(ν,ω)\documentclass[12pt]{minimal}
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\begin{document}$$T^q_s(\nu ,\omega )$$\end{document}, where 1+sp-sq>0\documentclass[12pt]{minimal}
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\begin{document}$$1+\frac{s}{p}-\frac{s}{q}>0$$\end{document}, by considering a generalized area operator. The results are provided in terms of Carleson measures for Aωp\documentclass[12pt]{minimal}
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\begin{document}$$A^p_\omega $$\end{document}.