The concept of ordered half antiperovskites (HAP) derives A
2
M
3
X
2
structures formally from metal‐rich intermetallic antiperovskites AM
3
X such as MgNi
3
C. It was developed within the last decade in Regensburg accompanied by fascinating discoveries of other groups. It extends the idea known for oxide structures related to perovskite such as cuprate superconductors: therein, the 3D M‐O network is cut to 2D sheets, that is YBaCu
2
O
7‐d
. By systematic formation of unoccupied sites 3D interlinked MO
6
octahedra in perovskites are cut to 2D substructures with CuO
4
and CuO
5
units. To the best of our knowledge, a similar scheme was not described for antiperovskites AM
3
X, where X and M sites of perovskites are exchanged. MgNi
3
C is taken subsequently as reference example. First reported by Hütter and Stadelmaier it became famous as noncuprate nonoxide superconductor. We show that MX
6
and XM
6
units in perovskites AMX
3
and APs AM
3
X can be cut to MX
3
and XM
3
units to form 2D structures. The situation compares to gray As and black P that are derived from a primitive α‐Po structure by cutting three of the six bonds. In both cases, interlinked 3D networks are cut to 2D structures. However, the ternary compounds introduce additional degrees of freedom by varying the electron count by composition that turns out important to design properties such as for example magnetism and thermoelectrics of superconductivity. Consequently, the HAP concept consists of a crystal structure part for compounds A
2
M
3
X
2
= AM
3/2
L
3/2
X with AP superstructures and an electronic structure part. In this review, we point out relations to antiperovskite AM
3
X crystal and electronic structures, the history of A
2
M
3
X
2
compounds, the HAP concept, important discoveries of HAP materials and novel investigations on synthesis, spintronics, thermoelectrics, superconductors, and topological properties. Advantages of the given conceptual view are pointed out for computer modeling, design, and prediction of structures and functions.