2D transition-metal dichalcogenides (TMDCs) have attracted increasing attention recently, not only because their different phases show diverse properties, [ 1,2 ] but also because their various nanostructures could provide versatile building blocks for nanodevices [3][4][5][6][7] or electrochemical electrodes. [ 8,9 ] The successful implementation of fi eld effect transistors [ 10,11 ] and phototransistors [ 12,13 ] based on semiconducting single-layer 2H TMDCs has demonstrated their high potential in nextgeneration nanoelectronics and optoelectronics applications. To realize fully 2D-integrated circuit, it is highly desirable to build up electrode components compatible with channel materials, but with conducting properties. There are several possible schemes to achieve this goal adopting different TMDC nanostructures which show metallic behaviors. First, electron radiation or chemical exfoliation by lithium intercalation can transform 2H TMDCs into metallic 1T phase which interfaces with 2H phase seamlessly. [ 14,15 ] Second, a focused electron beam can be applied to fabricate 1D metallic MX (M = Mo or W, X = S or Se) nanowires, which connect 2D TMDCs at designated points [ 16 ] (note the wire size-affected stoichiometry similar to metal disilicides case [ 17 ] . Third, metallic edges [ 18,19 ] can also be obtained in a way similar to fabricating nanowires or by cutting 2D TMDC into nanoribbons. However, each of these methods has intrinsic diffi culties in practice: the 1T phase is only metastable, and steering a focused electron beam or nanocutting adds more complexity during processing, while also introduces various defects into material.Grain boundaries (GBs), ubiquitous in large-scale polycrystalline samples, [ 20,21 ] are commonly believed to worsen the electronic transport of channel material, as shown in previous studies on Si.[ 22 ] For graphene, however, recent work on extended defects along the zigzag direction has demonstrated these defects can also behave as 1D metallic wires, which could potentially act as building blocks for future allcarbon electronics.[ [ 24 ] it would facilitate the development of electronics through nanoscale control of charge transport distribution. Here, we show that indeed such 1D metallic nanostructures can regularly occur in TMDC, in particular as large-angle (60°) GBs, which are fully embedded in the semiconducting 2H matrix. These 60° GB can naturally form when islands grow misoriented in a particularly inverted way, [ 21,25 ] due to specifi cs of stacking to substrate as exemplifi ed by graphene.[ 26 ] A dense network of them can even become thermodynamically favorable in experiment under chalcogenide-defi cient conditions.[ 27 ] Through systematic analysis, we reveal various possible GB structures, arising from unique metal-ligand bonding and the heteroelemental composition of TMDCs. All thermodynamically favorable GBs display metallic behaviors, which are robust against Peierls distortion. While possible structural irregularity can have detrimental infl uence on the ...