I review the status of the model of dark matter as the neutralino of supersymmetry in the light of constraints on supersymmetry given by the 7-to 8-TeV data from the Large Hadron Collider (LHC).Large Hadron Collider | supersymmetry | dark matter M odels for the dark matter particle span a huge range of masses, from 1 millionth of an electronvolt and lower to masses larger than that of the sun. The particles in these models vary in interaction strength from that of gravitational particle interactions to the gravitational force of a macroscopic black hole. And yet, most of the literature on the particle nature of dark matter is concentrated in one small region of this parameter space.The particles that have received most of the attention belong to the generic class called weakly interacting massive particles (WIMPs). These are neutral, stable particles whose number density was determined by the constraint that they were in thermal equilibrium at some time in the early universe. Even within this class, a particular hypothesis has received special attention, that the dark matter particle is the "neutralino," the lightest supersymmetric partner of the photon, the Z boson, and the Higgs bosons.There are good reasons to favor this neutralino hypothesis for dark matter. However, they are entirely theoretical. The neutralino fits easily into our current picture of particle physics. Supersymmetry is the unique extension of the Poincaré spacetime symmetry. New physical interactions are required at the teraelectronvolt mass scale to allow us to compute the symmetrybreaking potential of the Higgs boson. The extension of spacetime symmetry to supersymmetry naturally achieves this. When the Higgs potential is computed, the symmetry-breaking shape of the potential is related to the large value of the top quark Yukawa coupling. The addition of new particles related to the familiar elementary particles by supersymmetry changes the predictions for the very short distance values of the strong, weak, and electromagnetic couplings. The changes are such that these couplings become approximately equal at about 10 16 GeV, supporting the idea of a grand unification of couplings at this mass scale. These features of supersymmetry are all discussed in more detail in pedagogical reviews such as refs. 1-4.The final piece of the puzzle would be the explanation of dark matter. In fact, under rather weak hypotheses, supersymmetry requires a new discrete symmetry that makes its lightest new particle absolutely stable. There are several possibilities that make the lightest supersymmetric particle neutral. It may, for example, be a sneutrino or a gravitino. Here, I concentrate on the case in which the lightest supersymmetric particle is a neutralino, notatedχ 0 . If theχ 0 is stable, this particle satisfies all of the basic hypotheses of the WIMP model.To finish the picture, we need the mass scale of supersymmetric particles. From particle physics arguments, this should be of the order of the mass scale of the Higgs boson, 100-200 GeV. The WIMP hy...