Due to mirror symmetry breaking, two-dimensional Janus transition metal dichalcogenides (; ) present charming electronic properties. However, there have not been many related studies as of yet, and the intrinsic physical pictures are unclear. Here, we use first-principles calculations to explore the universality of electronic characteristics and photocatalyst applications of Janus , finding that the induced dipole moment, vibrational frequency, Rashba parameters, and direct-indirect band transition of monolayer are deeply associated with the atomic radius and electronegativity differences of chalcogen and elements. The internal electric field renders Janus the ideal photocatalysts. Moreover, the stacking-dependent on/off switch of the dipole moment further confirms that asymmetric Janus serves as a promising candidate for highly efficient photocatalysts within a broad range from infrared, visible, to ultraviolet light.
Type-II band alignment, a suitable direct gap (1.519 eV), superior optical-absorption (∼10 5 ) and a broad spectrum make the GeSe/SnS heterobilayer a promising material for photovoltaic applications.
Recently, constructing van der Waals (vdW) heterojunctions by stacking different two-dimensional (2D) materials has been considered to be effective strategy to obtain the desired properties. Here, through first-principles calculations, we find theoretically that the 2D -InSe/-GeSe(SnS) vdW heterojunctions are the direct-band-gap semiconductor with typical type-II band alignment, facilitating the effective separation of photogenerated electron and hole pairs. Moreover, they possess the high optical absorption strength (), broad spectrum width, and excellent carrier mobility (). Interestingly, under the influences of the interlayer coupling and external electric field, the characteristics of type-II band alignment is robust, while the band-gap values and band offset are tunable. These results indicate that 2D -InSe/-GeSe(SnS) heterojunctions possess excellent optoelectronic and transport properties, and thus can become good candidates for next-generation optoelectronic nanodevices.