    ## Corrigendum: On the Abel differential equations of third kind

 1 Departamento de Matemática, ICMC-Universidade de São Paulo, Avenida Trabalhador São-carlense, 400-13566-590, São Carlos, SP, Brazil 2 Departamento de Matemática, Instituto Superior Técnico, Universidade Técnica de Lisboa, Av. Rovisco Pais, 1049–001, Lisboa, Portugal

* Corresponding author: Regilene Oliveira

Received  February 2021 Revised  April 2021 Published  June 2021

In this paper, using the Poincaré compactification technique we classify the topological phase portraits of a special kind of quadratic differential system, the Abel quadratic equations of third kind. In  where such investigation was presented for the first time some phase portraits were not correct and some were missing. Here we provide the complete list of non equivalent phase portraits that the Abel quadratic equations of third kind can exhibit and the bifurcation diagram of a $3$-parametric subfamily of it.

Citation: Regilene Oliveira, Cláudia Valls. Corrigendum: On the Abel differential equations of third kind. Discrete & Continuous Dynamical Systems - B, doi: 10.3934/dcdsb.2021157
##### References:
  R. Oliveira and C. Valls, On the Abel differential equations of third kind, Discrete Contin. Dyn. Syst. Ser. B, 25 (2020), 1821-1834.  doi: 10.3934/dcdsb.2020004.  Google Scholar

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##### References:
  R. Oliveira and C. Valls, On the Abel differential equations of third kind, Discrete Contin. Dyn. Syst. Ser. B, 25 (2020), 1821-1834.  doi: 10.3934/dcdsb.2020004.  Google Scholar Bifurcation diagram of system $(ⅰ)$ for $k_1 = 1$ and $k_1 = 0$. The phase portrait $P_2$ is topologically equivalent to $L_{8}$. In this diagram, the phase portraits in the surfaces $S_i$, for $i = 4, 5, 6, 9, 10, 18$ and in the curves $L_j$, for $j = 2, 4, 5, 6$ admit a separatrix connection and although such surfaces and curves do not need to be algebraic the surfaces $S_9$ and $S_{10}$ are contained in one component of the algebraic surface given by $-64 k_0^3 - k_1^6 + 16 k_0^2 k_1^2 k_2 - 3 k_0 k_1^4 k_2^2 + 16 k_0^3 k_2^3 - 3 k_0^2 k_1^2 k_2^4 - k_0^3 k_2^6 = 0$ Global phase portraits in the Poincaré disk of systems $(ⅱ)$. The phase portraits $V_{13}$ and $V_{15}$ of system $(ⅱ)$ are topologically equivalent to the phase portraits $S_3$ and $S_2$ of system $(ⅰ)$, respectively. Here we remark that in the phase portraits $S_3$ and $S_2$ of system $(ⅰ)$, such system has two complex points and a saddle–node as finite singular points but in system $(ⅱ)$ the phase portraits $V_{13}$ and $V_{15}$ have a saddle–node as the unique finite singular point. The phase portrait $S_{21}$ has a separatrix connection between the finite saddle-node and the infinite saddle
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