This editorial serves as an introduction to a series of 10 papers collected under the special issue "Quantum Embedding Electronic Structure Methods." The idea to assemble a special issue came during a symposium at the Spring 2019 meeting of the American Chemical Society where we (Adam and Michele) organized a Physical Chemistry symposium bearing the same name as the special issue. The symposium ran for the entire week and featured many flavors of embedding: from density embedding to embedding within lattice models, as well as continuum models and many-body expansions. While it may seem that these approaches are far removed from each other, the symposium highlighted common goals, such as the reduction of the computational effort through "divide-and-conquer" strategies, and stressed the importance of establishing a common language across all embedding methods. It is clear that human interaction is key for scientific progress, and traveling to conferences is an important aspect of scientific research. Unfortunately, we write this introduction during a pandemic of historic proportions, when working on theoretical and computational chemistry may seem like an unacceptable luxury or an unjustified distraction. It is striking to remember how we interacted prior to the outbreak. Figure 1 provides a glimpse into the social nature of the symposium participants and the massive crowds at the conference. The editorial is organized into three sections: Origins, where we briefly discuss the origins of embedding methods for newcomers to the field; Present, where we highlight some of the current efforts with an emphasis on the contributions submitted to this Special Issue of IJQC; and Future, where we enumerate a few of the open challenges in the field and speculate on some of its possible future directions. 2 | ORIGINS Modern embedding methods can be broadly classified into three groups: density embedding, density-matrix and Green's function (GF) embedding, and classical (quantum mechanics / molecular mechanics (QM/MM) and continuum dielectrics) embedding. We briefly discuss the origins of these three approaches separately. orbitals. The KSCED follows by requiring that E[n] be minimized directly with regard to variations of the n α (r). A different set of equations is