We show that germanene nanoroads embedded in a completely hydrogenated germanene (germanane) exhibits a Quantum Spin Hall Effect (QSHE). These nanoroads can be obtained experimentally by local hydrogen dissociation from germanane. Using first principle calculations we predict that germanene nanoroads with zigzag interfaces show dissipationless conducting channels with in-plane and out-of-plane spin textures.The search for topological quantum phases of matter led condensed matter scientists to inspect, under a different point of view, materials known as Topological Insulators (TI). Those materials exhibit different properties and physical phenomena, like the quantum spin Hall effect (QSHE) [1], axion electrodynamics [2] and Majorana fermions [3]. The QSHE in two dimensional (2D) materials was proposed by Kane and Mele for graphene [1], followed by an independent proposal by Bernevig, Hughes and Zhang for the CdTe/HgTe/CdTe quantum well [4]. The latter has been confirmed experimentally [5], but for graphene due to the small spin-orbit bandgap, the observation of the QSHE would apply only at unaffordable experimental conditions [6,7].New candidate materials has been proposed to overcome the issue presented by graphene for the observation of the QSHE. Among some of these materials are the silicene [8][9][10][11][12][13], germanene [14], 2D hexagonal Si x Ge 1−x [15], and stanene [16]. They present similar properties to graphene, having some additional features, such as: (i) buckled honeycomb lattice; (ii) relatively large spin-orbit coupling (SOC), with bandgap of the order of meV and topological invariant Z 2 = 1 [14,15]. Such characteristics makes these 2D TI good candidates for the observation of the QSHE.From the experimental point of view, the pursuit of 2D materials that could display the QSHE was intensified by the synthesization of silicene. Silicene is mostly grown on metal surfaces, [8][9][10][11][12][17][18][19][20] that introduces some difficulties to isolate this single layer material and construct devices that will allow the measurement of the QSHE. Also the SOC bandgap in silicene is small, around 1.9 meV, so that the temperature to observe the QSHE will also be very low.A recent work of Bianco et al.[21] reported synthesis of germanane, a completely hydrogenated germanene structure. This opens up a new route to the experimental observation of the QSHE at higher temperatures. The formation and stability of this material, as well as the study of the QSHE may play an important role in nanoelectronics [21].In this work we propose a feasible setup for the observation of QSHE that is based on germanane [21]. The system is a germanene nanoroad embedded in germanane. We find that the germanene nanoroads with zigzag interfaces presents dissipationless conducting channels with in-plane and out-of-plane spin texture. We also show that with a small perturbation at the edge is possible to lift the degeneracy between interfaces, allowing a single-interface conduction. The electronic structure simulations were perf...