M any two-dimensional (2D) materials exist in bulk form as stacks of bonded layers with weak van der Waals interlayer attraction. Thanks to their particular structure, they can be exfoliated into atomically thin monolayers that hold promise for next-generation flexible electronics and optoelectronics. 1,2 Graphene has received much attention in the past decade, 3 due in large part to exceptional electronic properties such as its ultrahigh carrier mobility. However, the absence of a band gap has limited the progress of graphene-based technologies. For example, graphene field-effect transistors (FETs) cannot be turned off effectively, and even though small band gaps have been successfully opened in graphene, 4À7 the development of devices operating at room temperature with a low stand-by power dissipation remains a challenge. 8 On the other hand, transition-metal dichalcogenides (TMDCs) are a class of directband gap semiconductors that are emerging as strong candidates in next-generation nanoelectronic devices. 8À12 In the monolayer form, their lack of dangling bonds, structural stability, and mobility values comparable to Si make them optimal as channel materials in FETs. 1 In particular, FETs based on single layer MoS 2 , which has a direct band gap of 1.8 eV 1,13 and mobility in the range 1À50 cm 2 V À1 s À1 at room temperature, 14À17 show low power dissipation, 8 efficient control over switching 9 and reduction of shortchannel effects. 18,19 However, in order to develop logic circuits based on TMDCs, it is necessary to fabricate both n-and p-type FETs. TMDC FETs based on a Schottky device architecture can transport either electrons (n-FET) or holes (p-FET) in the conducting channel, depending on whether the Schottky barrier height (SBH) is smaller relative to the conduction or the valence band, respectively. 20 While monolayer n-FETs have been widely reported, fabrication of p-FETs has been challenging. 20 This is due to the relative difficulty in designing MoS 2 /metal contacts * Address correspondence to tiziana.musso@aalto.fi. Our analysis shows that this is possible due to the high work function of GO and the relatively weak Fermi-level pinning at the MoS 2 /GO interfaces compared to traditional MoS 2 /metal systems (common metals are Ag, Al, Au, Ir, Pd, Pt). The combination of easy-to-fabricate and inexpensive GO with MoS 2 could be promising for the development of hybrid all-2D p-type electronic and optoelectronic devices on flexible substrates.