“…The specific properties of graphene channel (GCs) [1][2][3] and black-P (b-P), black-As (b-As) , or black-AsP (b-AsP) layers [4][5][6][7][8] open up prospects for devices based on the GCs (see, for example, the review [9]) and on the GC/b-AsP heterostructures [6], including the electron devices using the real-space transfer over the b-AsP layers [10,11] and different optoelectronic devices [12][13][14][15]. Due to relatively low energy barriers for the electrons and holes at the GC/b-AsP interface, the thermionic emission through such an interface can be effective, particularly, enabling the creation of the GC/b-AsP-bolometric terahertz (THz) detectors.…”