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We use two families of parameters $\{(\epsilon_{x_j},\epsilon_{t_j})\,|\,\epsilon_{x_j,t_j}=\pm1,\, j=1,2,...,n\}$ to firstintroduce a unified novel two-family-parameter system (simply called ${\mathcalQ}^{(n)}_{\epsilon_{x_{\vec{n}}},\epsilon_{t_{\vec{n}}}}$ system), connectingintegrable local, nonlocal, novel mixed-local-nonlocal, and other nonlocalvector nonlinear Schr\"odinger (VNLS) equations. The ${\mathcalQ}^{(n)}_{\epsilon_{x_{\vec{n}}}, \epsilon_{t_{\vec{n}}}}$ system with$(\epsilon_{x_j}, \epsilon_{t_j})=(\pm 1, 1),\, j=1,2,...,n$ is shown topossess Lax pairs and infinite number of conservation laws. Moreover, we alsoanalyze the ${\mathcal PT}$ symmetry of the Hamiltonians with self-inducedpotentials. The multi-linear forms and some symmetry reductions are alsostudied. In fact, the used two families of parameters can also be extended tothe general case $\{(\epsilon_{x_j}, \epsilon_{t_j}) | \epsilon_{x_j} =e^{i\theta_{x_j}}, \epsilon_{t_j} = e^{i\theta_{t_j}},\, \theta_{x_j},\theta_{t_j}\in [0, 2\pi),\, j=1,2,...,n\}$ to generate more types of nonlinearequations. The two-family-parameter idea used in this paper can also be appliedto other local nonlinear evolution equations such that novel integrable andnon-integrable nonlocal and mixed-local-nonlocal systems can also be found.

A novel hierarchy of two-family-parameter equations: Local, nonlocal, and mixed-local-nonlocal vector nonlinear Schrodinger equations