Metamaterial-based electromagnetically induced transparency (EIT) analogs have been developed to mimic the unique spectral properties of EIT phenomena, where a sharp transmission peak is generated in the broad reflection or absorption spectrum. For this reason, researchers have recently focused on appropriate designs for EIT-like metamaterials and utilized these analogs for diverse applications, including slow light devices, [1][2][3][4] optical buffers, [5,6] and biochemical sensors. [7,8] Therefore, if EIT phenomena can be actively controlled using metamaterials, it will be a fascinating topic and an effective way to utilize these exotic properties for practical applications. Thus far, there have been many efforts to realize active EIT analog systems using various external stimulations. For example, optical tuning of active EIT metamaterials has been reported using photoconductive materials within bright and dark metaatoms in the terahertz (THz) range. [9][10][11][12] Microelectromechanical system (MEMS)-based mechanical tuning of EIT metamaterials has also been demonstrated by actuating the fabricated metaatoms mechanically [13,14] or rotating the polarization of 3D EIT metamaterials. [15] However, the optical tuning method requires pump laser-based sophisticated experimental setups, while the MEMS-based tuning method requires complex fabrication processes. Hence, electrically controllable EIT metamaterials have attracted attention as an alternative method to realize active EIT systems for practical applications. [16][17][18] Recently, graphene-based active metamaterials have been extensively studied to realize electrically controllable metamaterials not only for active optical switches and filters, [19][20][21][22][23][24][25] but also for active EIT systems in the terahertz region. In particular, graphene-based EIT metamaterials have been reported with theoretical approaches, making use of solely patterned graphene [26][27][28] and metal-embedded hybrid structures. [29][30][31] However, because these approaches have assumed that the graphene films have extremely high electrical mobilities (>3000 cm 2 V −1 s −1 ) or shorter relaxation times (≈1 ps) that cannot be achievable for realistic thin graphene films; to our best knowledge, there has been no experimental verification to confirm the practical use of graphene metamaterials for EIT applications.Electromagnetically induced transparency (EIT) analogs using metamaterials have diverse applications, including nonlinear optics, telecommunications, and biochemical sensors. These EIT analogs can be actively controlled by embedding semiconducting materials into metamaterial structures, but most active EIT metamaterials require complex optical setups and complicated fabrication processes. Graphene-based EIT metamaterials are some of the most promising active EIT systems because of their simple controllability by electrical bias, but related researches have so far been limited to theoretical or numerical studies. Here, experimentally verified graphene EIT metamateri...