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Such hydrogenated (2×1) π-reconstructed surface was found to be a stable structure according to ab initio calculation (Refs. 17 and 20). Additional supporting evidence is from the comparison with H/C (100)-(2×1). The calculated bond length (1.61 Å) of a C-C dimer chain on the first layer of the reconstructed H/C (111)-(2×1) surface is similar to that of a dimer C-C bond (1.62 Å) for the monohydride phase on H/C (100)-(2×1). Since the monohydride H/C (100)-(2×1) surface has been shown to be a stable structure both theoretically and experimentally, the existence of a stable H/C (111)-(2×1) surface is thus not unlikely. Moreover, the C-H bonds in two adjacent carbon atoms on H/C (111)-(2×1) are expected to be in the pseudostaggered conformation and suffer less van der Waals repulsion
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Such hydrogenated (2×1) π-reconstructed surface was found to be a stable structure according to ab initio calculation (Refs. 17 and 20). Additional supporting evidence is from the comparison with H/C (100)-(2×1). The calculated bond length (1.61 Å) of a C-C dimer chain on the first layer of the reconstructed H/C (111)-(2×1) surface is similar to that of a dimer C-C bond (1.62 Å) for the monohydride phase on H/C (100)-(2×1). Since the monohydride H/C (100)-(2×1) surface has been shown to be a stable structure both theoretically and experimentally, the existence of a stable H/C (111)-(2×1) surface is thus not unlikely. Moreover, the C-H bonds in two adjacent carbon atoms on H/C (111)-(2×1) are expected to be in the pseudostaggered conformation and suffer less van der Waals repulsion.
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To the first order of approximation, the strain energy was estimated to be ∼1.5 eV/unit cell, based on the potential curve shown in Fig. 14 in Ref. 6, where the energy difference between 2D/C (111)-(1×1) and clean C (111)-(2×1) states was ∼3 eV
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To the first order of approximation, the strain energy was estimated to be ∼1.5 eV/unit cell, based on the potential curve shown in Fig. 14 in Ref. 6, where the energy difference between 2D/C (111)-(1×1) and clean C (111)-(2×1) states was ∼3 eV.
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