Two-dimensional quantum antiferromagnets host rich physics including long-range ordering, high-Tc superconductivity, quantum spin liquid behavior, topological ordering, variety of other exotic phases, and quantum criticalities. Frustrating perturbations in antiferromagnets may give rise to strong quantum fluctuations, challenging the theoretical understanding of the many-body ground state. Here we develop a method to describe the quantum antiferromagnets using fermionic degrees of freedom. The method is based on a formally exact mapping between spin-exchange models and theories describing fermionic matter with the emergent U (1) Chern-Simons gauge field. For the planar Néel state, this mapping self-consistently generates the Chern-Simons superconductor mean-field ground state of introduced fermions. We systematically compare the Chern-Simons superconductor state with the planar Néel state at the level of collective modes and order parameters. We reveal qualitative and quantitative correspondences between these states. Such a description of the Néel order, constructed from the fractionalized fermion excitations and emergent gauge fields, can be applied to the quantum spin-liquids. More importantly, it allows us to keep track of the unconventional phase transitions from ordered states to the spin-liquids. We show that such confinement-deconfinement transitions are signaled and characterized by the Chern-Simons superconductor instabilities, driven by strong frustration. These results provide a systematic parton mean-field approach that accounts for the magnetically ordered state, the spin-liquids, and the unconventional phase transitions in a unified physical picture. The findings suggest observing and classifying descendant states, including quantum spin-liquids and unconventional superconductors.