Abstract:We have investigated ion desorption from single-walled carbon nanotubes (SWNTs) that is induced by soft X-ray illumination in the C 1s core-excitation energy range in order to have insight to the mechanism of defect formation caused by the similar excitation. The mass of desorbed ions was analyzed by a time of flight (TOF) spectrometer and the photon energy 2 dependence of the ion yield or the desorption efficiency spectra were measured as a function of the monochromatic photon energy used for illumination. Ex… Show more
“…Recently, Mera et al directly measured ion desorption from SWCNTs under soft X-ray illumination (Mera et al, 2010). They also excluded emission of carbon atoms from the SWCNTs.…”
Section: Reversible Damage and Recoverymentioning
confidence: 99%
“…The low-energy irradiation damage has been observed in a surface-science-grade ultra-high vacuum (UHV) of 1×10 -8 Pa by VUV light illumination (Suzuki & Kobayashi, 2006a. Suzuki & Kobayashi, 2007a. Mera et al, 2010, electron beam irradiation , and electron (hole) injection from a STM tip (Berthe et al, 2007.…”
Section: Occurrence Of the Damage In An Ultra-high Vacuummentioning
“…Recently, Mera et al directly measured ion desorption from SWCNTs under soft X-ray illumination (Mera et al, 2010). They also excluded emission of carbon atoms from the SWCNTs.…”
Section: Reversible Damage and Recoverymentioning
confidence: 99%
“…The low-energy irradiation damage has been observed in a surface-science-grade ultra-high vacuum (UHV) of 1×10 -8 Pa by VUV light illumination (Suzuki & Kobayashi, 2006a. Suzuki & Kobayashi, 2007a. Mera et al, 2010, electron beam irradiation , and electron (hole) injection from a STM tip (Berthe et al, 2007.…”
Section: Occurrence Of the Damage In An Ultra-high Vacuummentioning
“…As mentioned in section 2, Coulomb explosion cold take place because the localized multiple holes generated also in the normal Auger final states have a relatively long lifetime [15]. In fact, the desorption efficiency spectrum in SWNTs obtained by dividing total counts of desorbed ions with the counts of normal Auger electrons of 259 eV in energy exhibits a non-resonant feature at energies higher than 290 eV [26]. Nevertheless, there could be another scenario that low-energy electrons generated as secondary products of core excitations are responsible for the non-resonant damage.…”
Section: Non-resonant Damage Induced By Soft X-ray Illuminationmentioning
confidence: 94%
“…To examine these hypotheses, we conducted TOF measurements of photo-desorbed species at KEK-PF [25,26]. The ta-C sample we used was basically the same as that used for illumination experiments at SPring-8.…”
Section: The Mechanism Of the Resonant Effectmentioning
Intense soft X-ray illumination near the carbon core edge induces significant structural damage in tetrahedral amorphous carbon films and less significant but detectable defect formation in single-walled carbon nanotubes (SWNTs). The efficiency spectra of the photo-induced damage commonly show a resonant peak between the π * and σ * peaks of X-ray absorption spectra in addition to a non-resonant background. The resonant damage cannot be explained by the coreexciton mechanism but can be attributed to a recoil damage accompanying the photo-desorption of heavy chemisorbates that is resonantly decomposed by the spectator Auger mechanism. The cause of the non-resonant damage in SWNTs may be attributed to anomalous radiation damage by low-energy electrons generated by secondary effects of soft X-ray illumination, which is supported by the recent finding by authors that hot electron injection from probe tips of scanning tunneling microscopes generates defects in the SWNT samples.
Pulsed desorption of organic conducting polymer by XUV-photons, formed by a thin capillary collimator, has been investigated. Short-wavelength radiation has been resulted from a metal target irradiated by a sharply focused Ti:Sa laser beam (0.8 μm, 40 fs, 3 mJ∕pulse) and has been filtered by Mylar-gold substrate. Single shot and 1-kHz pulses regimes of driving femtosecond laser have been compared using a time-of-flight mass spectrometer. A stepwise function of photoion signal vs laser pulse energy has been observed.
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