2016
DOI: 10.1016/j.spmi.2016.03.031
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Effect of mono vacancy defect on the charge carrier mobility of carbon nanotubes: A case study on (10, 0) tube from first-principles

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Cited by 20 publications
(13 citation statements)
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“…The ratio of peaks G and D reflects the defect degree of the CNT materials . A high I G /I D ratio suggests few defects in CNTs, which ensures the good electrical performance of the FET devices, such as high carrier mobility . From the inset of Figure b, it should be noted that a narrow radial breathing mode (RBM) peak appears at 165 cm –1 , which further verifies the high purity of the CNT film that is consistent with the previous results observed in the UV–vis–NIR absorption spectrum .…”
Section: Results and Discussionsupporting
confidence: 87%
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“…The ratio of peaks G and D reflects the defect degree of the CNT materials . A high I G /I D ratio suggests few defects in CNTs, which ensures the good electrical performance of the FET devices, such as high carrier mobility . From the inset of Figure b, it should be noted that a narrow radial breathing mode (RBM) peak appears at 165 cm –1 , which further verifies the high purity of the CNT film that is consistent with the previous results observed in the UV–vis–NIR absorption spectrum .…”
Section: Results and Discussionsupporting
confidence: 87%
“…39 A high I G /I D ratio suggests few defects in CNTs, which ensures the good electrical performance of the FET devices, such as high carrier mobility. 40 From the inset of Figure 2b, it should be noted that a narrow radial breathing mode (RBM) peak appears at 165 cm −1 , which further verifies the high purity of the CNT film that is consistent with the previous results observed in the UV−vis−NIR absorption spectrum. 41 The narrow RBM peak at 165 cm −1 indicates a diameter distribution of CNTs of around 1.5 nm according to the formula ω = 248/d (nm), where ω and d are the RBM Raman shift and diameter of CNTs, respectively.…”
Section: Resultsmentioning
confidence: 99%
“…38 The higher I G / I D ratio indicates that the CNTs used in this work have fewer defects, 39,40 which ensures the good electrical properties of the FET, such as high carrier mobility. 41,42 In addition, it can be seen from Fig. 2b that a radial respiration mode (RBM) peak appears at 170 cm −1 .…”
Section: Resultsmentioning
confidence: 93%
“…In general, these NQSBR models use as input physicochemical properties of nanomaterials (nanodescriptors) to predict their biological activity, nanotoxicity, and/or binding affinity for specific targets. Despite the relative progress in the discovery of new nanodescriptors for modeling the toxicity caused by carbon nanotubes (i.e., mitochondrial nanotoxicity), the influence of topological vacancies has not been explored until now. Indeed, in most cases, a broad spectrum of topological vacancies are spontaneously generated in the side-walled SWCNT surface derived from chemical oxidation processes (e.g., by OH and COOH), like vacancies, Stone–Wales vacancies, and octagon–pentagon pair vacancies. Such vacancies significantly affect the geometric and electronic properties of SWCNTs and, at the same time, may increase their chemical reactivity and nanotoxicological potential . In fact, topological SWCNT vacancies are often seen and may change redox biochemical mechanisms at the subcellular level (mitochondria). , Previous theoretical studies have shown that the most stable vacancies correspond to monovacancy, divacancy, tetravacancy, and hexavacancy in terms of chemical reactivity .…”
Section: Introductionmentioning
confidence: 99%