Yoon Seok Kim1,Donghun Lee1,Jea Jung Lee2,Yeon Ho Kim1,Jong Chan Kim3,Woong Huh1,Jaeho Lee1,Sungmin Park1,Hu Young Jeong3,Young Duck Kim2,Chul-Ho Lee1
Korea University1,Kyung Hee University2,Ulsan National Institute of Science and Technology3
Yoon Seok Kim1,Donghun Lee1,Jea Jung Lee2,Yeon Ho Kim1,Jong Chan Kim3,Woong Huh1,Jaeho Lee1,Sungmin Park1,Hu Young Jeong3,Young Duck Kim2,Chul-Ho Lee1
Korea University1,Kyung Hee University2,Ulsan National Institute of Science and Technology3
Doping in two-dimensional (2D) semiconductors while suppressing Coulomb scattering is essential to achieve high-performance electronic devices. Despite recent advances in the fabrication of artificial van der Waals heterostructures and their electronic device applications, modulation doping in 2D semiconductors has not been demonstrated so far. Typically, these atomically thin materials can be easily doped by simple molecular charge transfer methods. However, the ionized dopants generated on the surface are present in close proximity to the atomically thin channel and thereby can significantly hamper the charge transport by Coulomb interaction, leading to the charged impurity scattering. Here, we demonstrate a modulation doping in the WSe<sub>2</sub>/<i>h</i>-BN/MoS<sub>2</sub> heterostructure that can diminish the doping-induced scattering, in which electrons in the underlying MoS<sub>2</sub> channel doped by remote charge transfer are spatially separated from molecular dopants on the WSe<sub>2</sub> surface. Remarkably, as decreasing the temperature, <i>μ</i> of the modulation-doped (MD) device monotonically increases and begins to saturate below 100 K, whereas, for the direct-doped (DD) device, <i>μ</i> peaks around 200 K and gradually decreases as further decreasing the temperature. Such a decreasing behavior of <i>μ</i> at low temperature is not observed in the case of the undoped samples. In particular, the MD device exhibits over an order of magnitude enhancement in <i>μ</i> at 10 K from 63 to 1,100 cm<sup>2</sup>V<sup>-1</sup>s<sup>-1</sup> compared with the DD counterpart. These results could be explained by the reduction of the dopant-induced charge impurity scattering.