“…This transformation enhances the adsorption of protons to the catalyst, thus promises am ore stable adsorption state of the intermediate in the HER. [18] Thee nergy profiles in Figure 3b shows that the theoretical Gibbs free energy to drive HER of 2(a(Co-Pt)@N8V4) is 0.08 V, which is lower than those of a(Co-Pt)@N8V4 and Pt/C.T he significant free-energy decreased from a(Co-Pt)@N8V4 to 2(a(Co-Pt)@N8V4) is probably ascribed to the strong adsorption of H* with the advantage of concentrated negative charges.T ov alidate the interaction of atomic metals trapped on the adjacent graphitic layers, control samples of A-CoPt-NG and A-CoPt-MNG with atomic Co and Pt trapped on single layer graphene and multilayer graphene were prepared, respectively.T hey were fabricated from the atomic Co trapped graphene with nitrogen dopants (Co-NG and Co-MNG) via the same electrochemical activations.M etal particles are absent in A-CoPt-NG (Supporting Information, Figure S10), but apparent signals of Co and Pt are observed from the energy-dispersive X-ray spectroscopy (EDS) elemental mapping images,i ndicating that Co and Pt are trapped on the graphene atomically. TheR aman spectra (Supporting Information, Figure S11) show that the 2D band of A-CoPt-NG around 2650 cm À1 is as ymmetric Lorentzian peak, indicating the single layered structure.However,the 2D band of A-CoPt-MNG splits and is shifted to high frequency,i mplying the multilayered structure.T he Pt contents of A-CoPt-MNG and A-CoPt-NG are 0.05 wt %a nd 0.03 wt %, respectively.W hen the Ag was photo-deposited (Supporting Information, Figure S12), there are more Ag particles on the surface of A-CoPt-MNG…”