2005
DOI: 10.1143/jjap.44.5443
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Observation of Large-Scale Features on Graphite by Scanning Tunnelling Microscopy

Abstract: Superlattice structures and rippling fringes were imaged on two separate pieces of graphite (HOPG) by scanning tunnelling microscopy (STM). We observed the corrugation conservation phenomenon on one of the superlattice structures where an overlayer does not attenuate the corrugation amplitude of the superlattice. Such a phenomenon may illustrate an implication that nanoscale defects a few layers underneath the surface may propagate through many layers without decay and form the superlattice structure on the to… Show more

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Cited by 10 publications
(14 citation statements)
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“…Another large-scale feature on graphite, related to superlattices and which has been reported recently [43], is that of one-dimensional fringes with periodicities of 20 and 30 nm and corrugations of 0.1 and 0.15 nm which have been observed on a superlattice (figures 2 and 3). The fringes were observed under differing tunnelling conditions as shown in figures 2(c) and (e).…”
Section: Large-scale Features Observed On Graphite Under Stmsupporting
confidence: 52%
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“…Another large-scale feature on graphite, related to superlattices and which has been reported recently [43], is that of one-dimensional fringes with periodicities of 20 and 30 nm and corrugations of 0.1 and 0.15 nm which have been observed on a superlattice (figures 2 and 3). The fringes were observed under differing tunnelling conditions as shown in figures 2(c) and (e).…”
Section: Large-scale Features Observed On Graphite Under Stmsupporting
confidence: 52%
“…Tunnelling conditions overlayers factor [37] V tip = 20 mV, I t = 0.8 nA 1 2.6 [37] V tip = 180 mV, I t = 0.9 nA 1 2.3 [37] V tip = 15 mV, I t = 0.8 nA 1 2.6 [37] V tip = 180 mV, I t = 0.9 nA 1 1.6 a [72] (not provided) 1 2 b [72] (not provided) 2 4 b [43] V s = 206 mV, I t = 0.5 nA 1 2.3 [21] V tip = 178 mV, I t = 2.4 nA 2 5 [48] V s = 100 mV, I t = 1.0 nA 1 2.4 [47] V tip = 150 mV 1 1.59 [70] V s = 1200 mV 1 2.15 a This is the AF for the bead-like boundary of the superlattice covered by one overlayer. b The authors of [72] observed the superlattices covered by one and two graphite sheets, and from these data, they proposed equation (15), however, without mentioning explicitly the AFs that they observed experimentally for one and two overlayers.…”
Section: Number Of Attenuation Of Datamentioning
confidence: 99%
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“…c), the particle diameter increased slightly to 7.4 nm, but the height doubled to 0.4 nm. The question then arises on the nature of the observed nanoparticles organized in a regular hexagonal pattern on HOPG, Pt, or C. It was found in the literature that there is an anomaly of the STM related to superlattices on graphite, which are formed because of intrinsic defects of the substrate generated during crystal growth or cleavage. In principle, these particles could be associated to a graphite structure generated from the preparation of the surface before each experiment.…”
Section: Resultsmentioning
confidence: 99%
“…Various publications have reported an attenuation factor (AF) associated with overlayer coverage of a moiré pattern in HOPG. 8,9,24 A fit of this data yields AF n = e 0.81n , where n is the number of overlayers. 10 In view of this, a second/third layer moiré pattern would be visible (AF 1 = 2.25) if present but the visibility of patterns from deeper layers decays exponentially.…”
Section: Multilayer Moirémentioning
confidence: 99%