2021
DOI: 10.1016/j.carbon.2020.10.086
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A macro-scale ruck and tuck mechanism for deformation in ion-irradiated polycrystalline graphite

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Cited by 35 publications
(10 citation statements)
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“…The evolution of the ion-induced HOPG topography with increasing ion energy expands the view of anomalous deep modification, which in [8][9] has been associated with the intense diffusion of the interstitial carbon atoms along the inclined to the basal plane graphene planes of the ion-induced twins, leading to the formation of an altered layer with implanted ions at depths h Ar >> R p . The transition of the ion-induced HOPG topography from cones at E < E th to a submicron columnar-needle topography at an anomalously deep surface modification with h Ar >> R p suggests significant mass transfer in the HOPG surface layer at E > E th , which may occur by twinning, bending, kinking, and folding plastic deformations and their mixed types typical for two-dimensional layered materials [8][9][10][11]. The corresponding deformation patterns can be seen in the top view of the SEM images (bottom row in figure 1).…”
Section: Resultsmentioning
confidence: 99%
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“…The evolution of the ion-induced HOPG topography with increasing ion energy expands the view of anomalous deep modification, which in [8][9] has been associated with the intense diffusion of the interstitial carbon atoms along the inclined to the basal plane graphene planes of the ion-induced twins, leading to the formation of an altered layer with implanted ions at depths h Ar >> R p . The transition of the ion-induced HOPG topography from cones at E < E th to a submicron columnar-needle topography at an anomalously deep surface modification with h Ar >> R p suggests significant mass transfer in the HOPG surface layer at E > E th , which may occur by twinning, bending, kinking, and folding plastic deformations and their mixed types typical for two-dimensional layered materials [8][9][10][11]. The corresponding deformation patterns can be seen in the top view of the SEM images (bottom row in figure 1).…”
Section: Resultsmentioning
confidence: 99%
“…If a crystal is thick, the nonbasal twinning occurs along with bends. Under ion irradiation, the mechanical stresses are caused by gradient (x) of the radiation damage profiles in the number of dpa [5][6][7][8][9][10][11]. The profiles (x) corresponding to the present experiment are shown in figure 3.…”
Section: Resultsmentioning
confidence: 99%
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“…Regularly observed were 6-membered rings, 7-membered rings, edge sites, pores, 5-membered rings, methylene sites, methyl sites, 3-membered rings, sp 3 diamond bonds, and sp 2 bridging bonds. While not key to electrochemical or gas storage properties bridging bonds have been observed in HC films [49] and irradiated graphite [50][51][52] and are believed to contribute for HC's inability to graphitize. Beyond these motifs, 5-and 7-membered rings have been experimentally observed by TEM and can contribute to topological deformation of graphene sheets and their entanglement, another contributor preventing graphitization.…”
Section: Molecular Dynamics and Reverse Monte Carlomentioning
confidence: 99%
“…Twinning in graphite, first reported in [31] and observed by optical microscopy [32], is theorised as a rotation of approximately 20° about < 1101 > [33]. Twinning under load in natural graphite flakes has been demonstrated with electron microscopy [34] and the analysis of ion-beam irradiation of pyrolytic graphite has demonstrated the formation of a novel reoriented crystal vein structure due to basal dislocations [35]. It has also been reported, for neutron-irradiated synthetic graphite, that twins recover once the load is removed [36] so twinning may be an elastic deformation mechanism.…”
Section: Introductionmentioning
confidence: 99%