effect transistor (FET), and opto-electronic applications. Graphene displays excellent properties when coupled with 0D quantum dots, 1D carbon nanotubes (CNTs), or 3D bulk materials to form mixed-dimensional van der Waals heterojunctions (vdW HJs). However, the applications of graphene are limited by the absence of a bandgap. [1][2][3][4] In this regard, the 2D transition metal chalcogenides (TMDs) have gained much attention as excellent alternatives to the use of graphene in FETs, photodiodes, and solar cells, due to the presence of considerable band gaps, direct-to-indirect (monolayerto-bulk) transitions without the need for surface dangling bonds, valley-selective optical coupling, exciton binding energies, high I on /I off ratios (≈10 6 ), and both ambipolar and unipolar behavior. [5][6][7] Eminent p-n heterojunction (HJ) structures can be fabricated via the vertical stacking of various TMDs to combine the individual properties of each TMD, thus resulting in novel functionalities. [8][9][10] The resulting vertically stacked TMD HJs exhibit a lower lattice mismatch than the conventional heterojunctions, and offer strong light-matter interactions that ultimately result in a large photocurrent generation. Additionally, the atomically thin nature and steep interfacial charge-carrier gradient of the 2D HJs promote modulation of the carrier density and band alignments. [11][12][13][14] A diverse range of HJs can be fabricated depending on the work function and bandgaps of the TMDs, including Type-I straddlinggap, type-II staggered-gap, and type-III broken gap HJs. [15] In recent years, TMDs and HJs containing WS 2 , MoS 2 , WSe 2 , MoSe 2 , MoTe 2 , GeSe, and black phosphorus (BP) have shown promising characteristics. [16][17][18][19] For instance, GeSe/WS 2 has shown strong NIR detection and gate tunable rectification behavior, [20] while MoS 2 /BP, WSe 2 /MoS 2 , and MoSe 2 /MoS 2 display excellent rectification behavior with high photoresponsivity toward radiation ranging from the ultraviolet-visible (UV-Vis) to the near infrared (NIR). [21][22][23][24] However, while type-I alignment is favorable for optoelectronic applications involving radiative electron-hole (e-h) recombination, numerous applications demand the formation of large band offsets. [25] By contrast, Type-II HJs give rise to the separation of photoexcited electrons and holes, thus leading to tuned interlayer coupling, ultrafast charge transfer, and an increased chargecarrier lifetime via reduced interfacial e-h recombination. [26][27][28][29] Visible near infrared (VNIR) transition-metal dichalcogenides (TMDs) photodetectors have attracted attention due to their unique electronic and optoelectronic properties. Herein, the photodetection performance of a novel MoTe 2 / ReSe 2 van der Waals heterojunction (vdW HJ) diode is studied in the VNIR region. Density functional theory calculations reveal the formation of type-II band alignment, which is beneficial for the design of a MoTe 2 /ReSe 2 HJ diode with better optoelectronic properties. A superb rec...