The electromagnetic response of a two-dimensional metal embedded in a periodic array of a dielectric host can give rise to a plasmonic Dirac point that emulates epsilon-near-zero (ENZ) behavior. This theoretical result is extremely sensitive to structural features like periodicity of the dielectric medium and thickness imperfections. We propose that such a device can actually be realized by using graphene as the two-dimensional metal and materials like the layered semiconducting transition-metal dichalcogenides or hexagonal boron nitride as the dielectric host. We propose a systematic approach, in terms of design characteristics, for constructing metamaterials with linear, elliptical, and hyperbolic dispersion relations which produce ENZ behavior, normal or negative diffraction. DOI: 10.1103/PhysRevB.94.201404 The confinement of metallic ("free") electrons in twodimensional interfaces can produce powerful effects used to drive electromagnetic (EM) devices like nanoantennas with extremely short wavelength resonance [1,2], metalenses and optical holography [3][4][5], active plasmonic systems [6][7][8], and sub-wavelength Bloch oscillations [9,10]. The key feature for such applications is the creation of waves propagating along a metal-dielectric interface with wavelength shorter than that of the incident radiation, while the waves decay exponentially in the perpendicular direction. This surface effect involves electronic motion (plasmons) coupled with electromagnetic waves (polariton) and is referred to as surface plasmon polariton (SPP). By combining the properties of different materials, it is even possible to produce behavior not found under normal circumstances like negative refraction [11][12][13][14][15][16], epsilon-near-zero (ENZ) [17][18][19], discrete solitons [20,21], and quantum control of light [22,23].The bottleneck in creating SPP devices with any desirable characteristic has been the limitations of typical three-dimensional solids in producing perfect interfaces for the confinement of electrons and the features of dielectric host. This may no longer be a critical issue. The advent of truly two-dimensional (2D) materials like graphene (a metal), transition-metal dichalcogenides (TMDC's, semiconductors), and hexagonal boron nitride (hBN, an insulator) make it possible to produce structures with atomic-level control of features in the direction perpendicular to the stacked layers [24][25][26][27]. This is ushering a new era in manipulating the properties of plasmons and designing devices with extraordinary behavior. In particular, 2D structures support plasmons (collective excitations) which fundamentally differ from SPPs, since the charge carriers are restricted in two dimensions [28,29]. Nevertheless, 2D plasmons and SPPs share similarities in field profiles and in dispersion behavior and could be used * mariosmat@seas.harvard.edu; http://scholar.harvard.edu/marios _matthaiakis/home † konstantinos.valagiannopoulos@nu.edu.kz; https://sst.nu.edu.kz /konstantinos-valagiannopoulos/ interchangeably fo...