Topological semimetals in ferromagnetic materials have attracted enormous attention due to the potential applications in spintronics. Using the first-principles density functional theory together with an effective lattice model, here we present a new family of topological semimetals with a fully spin-polarized nodal loop in alkaline-metal monochalcogenide MX (M = Li, Na, K, Rb, Cs; X = S, Se, Te) monolayers. The half-metallic ferromagnetism can be established in MX monolayers, in which one nodal loop formed by two crossing bands with the same spin components is found at the Fermi energy. This nodal loop half-metal survives even when considering the spin-orbit coupling owing to the symmetry protection provided by the M z mirror plane. The quantum anomalous Hall state and Weyl-like semimetal in this system can be also achieved by rotating the spin from the out-of-plane to the in-plane direction. The MX monolayers hosting rich topological phases thus offer an excellent materials platform for realizing the advanced spintronics concepts.2 Spintronics is a multidisciplinary field, which utilizes the electron's spin degree of freedom as an information carrier for data storage and processing. 1,2 Compared with conventional semiconductor devices, spintronic devices have higher integration density, faster processing speed, and lower power consumption. However, many issues such as the generation and transport of a pure spin current still present profound challenges in realizing three-dimensional spintronics devices, 3,4 hindering the range of possible competitive applications. In this respect, the two-dimensional (2D) materials are being currently promoted as a flagship for realizing advanced spintronics concepts, among which the emerging 2D topological quantum states exhibiting striking advantages for spintronics, have attracted tremendous attention in recent years.2D nodal loop semimetals (NLSs) 5,6 provide an exciting avenue for realizing topological quantum phase transitions between the gapped and gapless states. Physically, the 2D NLSs are topologically protected by the crystal symmetry, e.g., mirror or glide-mirror symmetry.These proposed protection mechanisms provide guiding principles for predicting real materials to realize various NLSs. Many exotic properties were reported to be associated with NLSs, including high-temperature surface superconductivity, 7 non-dispersive Landau energy level, 8 and specific long-range Coulomb interactions. 9 Recent advances in the domain of 2D ferromagnetic (FM) materials gave an additional boost to the young field of NLSs. Unlike the previously proposed NLSs in nonmagnetic materials, it was recently proposed that the NLSs can be achieved in 2D ferromagnets due to band crossings occuring between the states of opposite spins. 10,11 Nevertheless, for applications which rely on strong spin-polarization of generated currents, it is desired to realize the NLSs in fully spin-polarized 2D systems, such as half-metals.In this work, using the first-principles calculation together with an eff...