1995
DOI: 10.1002/pssa.2211510106
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Positron Annihilation in Carbon Fibers

Abstract: Preliminary results on positron annihilation in carbon fibers produced from polyacrylonitrile precursor are presented. An analysis of the Doppler broadening of annihilation line and positron lifetime is made. To characterize the fibers, X‐ray diffraction, electrical resistivity measurements, and elemental analysis are performed. Only one component is found in positron lifetime spectra ranging form 373 ± 1 to 441 ± 1 ps. It is observed that the positron lifetime increases with the temperature of heat treatment … Show more

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Cited by 11 publications
(7 citation statements)
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“…It is commonly accepted that such a value results from positrons annihilating in the open volume defect clusters like pores. Annihilation in such case occurs at the internal surface of the pores and the values obtained in our case are closely in agreement with those reported by others as well in graphite [11,12]. Many authors in general have attributed lifetimes ranging from 140 to 225 ps to free positron annihilation with π-electrons in the whole volume of the graphite.…”
Section: Resultssupporting
confidence: 93%
See 1 more Smart Citation
“…It is commonly accepted that such a value results from positrons annihilating in the open volume defect clusters like pores. Annihilation in such case occurs at the internal surface of the pores and the values obtained in our case are closely in agreement with those reported by others as well in graphite [11,12]. Many authors in general have attributed lifetimes ranging from 140 to 225 ps to free positron annihilation with π-electrons in the whole volume of the graphite.…”
Section: Resultssupporting
confidence: 93%
“…The results show that the raw, non purified CNC_05 sample is a very poor material as a potential hydrogen storage material. However, the results for the CNC_20 are comparable to previous experimental works on different carbon nanostructures such as single and multiwalled nanotubes, nanofibers and activated carbon [12][13][14][15][16], but are still far from required by US Department of Energy value of 6.5 wt% percent in storage material at ambient temperature and pressure.…”
Section: Discussionsupporting
confidence: 79%
“…The positron lifetime components (t 1 = 137.4 ps and t 2 = 338.3 ps) in MWCNTs are typical of those reported in graphite. 43 The shorter component (137.4 ps) is ascribed to the positron annihilation from the delocalized Bloch states in graphene sheets and the longer component (338.3 ps) is ascribed to the trapped state within the interstitials or inside the tubes. 41 The positron lifetime observed in CNTs ranging from 140 to 225 ps has been attributed to free positron annihilation with p electrons in the whole volume.…”
Section: Resultsmentioning
confidence: 99%
“…The short component (t 1 ) is usually attributed to the annihilation of the positron in bulk; the second (t 2 ), longer component, is attributed to the annihilation in a place with low electron density, for example, in different types of defects and small cavities or the annihilation of surface-trapped positrons [78]. It is known that Ps is not formed in pure carbon in different forms [79][80][81] or it creates in exceptional cases only [82], so it is impossible to analyze any mesopores in the material using standard PALS porosimetry based on the measured ortho-Ps lifetime and an appropriate models [83,84]. However, a short component associated with defect states is useful for characterizing micro-pores and defects that are not detectable by standard methods, such as BET (Brunauer, Emmett and Teller).…”
Section: Discussionmentioning
confidence: 99%