2014
DOI: 10.1103/physrevb.89.195422
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Nanostructuring and oxidation of diamond by two-photon ultraviolet surface excitation: An XPS and NEXAFS study

Abstract: We report C(1s) and O(1s) surface sensitive x-ray photoelectron spectroscopy (XPS) and C and O K-edge partial-electron yield near-edge x-ray absorption fine structure (NEXAFS) measurements for (100) and (110) oxidized diamond surfaces, etched by a laser two-photon ultraviolet (UV) desorption process. Etched regions of the (100) surface show increased oxygen coverage with a higher fraction of singly bonded termination species than unetched regions. Similar changes are observed for the (110) but with smaller mag… Show more

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Cited by 27 publications
(26 citation statements)
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References 37 publications
(59 reference statements)
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“…The C 1s peak at 285 eV arises primarily from sp 3 (in bulk), and the asymmetric shape indicates the presence of other bonds such as C-O, C=O (> 285 eV), and sp 2 (< 285 eV). 18,42 The O 1s peak at 532 eV has a broad linewidth, presumably composed of C-O-C, C-C-H, and C=O (< 532 eV). 18,42 Despite the limited spectral resolution, we can conclude that the chemical composition of the surface is essentially the same between the t = 0 and t = 0 areas.…”
Section: Surface Conditionmentioning
confidence: 99%
“…The C 1s peak at 285 eV arises primarily from sp 3 (in bulk), and the asymmetric shape indicates the presence of other bonds such as C-O, C=O (> 285 eV), and sp 2 (< 285 eV). 18,42 The O 1s peak at 532 eV has a broad linewidth, presumably composed of C-O-C, C-C-H, and C=O (< 532 eV). 18,42 Despite the limited spectral resolution, we can conclude that the chemical composition of the surface is essentially the same between the t = 0 and t = 0 areas.…”
Section: Surface Conditionmentioning
confidence: 99%
“…Recently, a novel 2-photon laser induced desorption (LID) phenomenon has been reported for diamond surfaces exposed to nanosecond ultraviolet (UV) pulses with incident fluence well below the threshold for laser ablation [1][2][3][4][5]. This "cool-etching" phenomenon appears to have a number of advantages over traditional ablative laser-machining (for which the minimum etch rates are around 10 nm/pulse); most notably, the LID process has no intensity threshold [3] and allows for carbon removal rates as low as 3×10 −9 nm/pulse for low incident fluence [6].…”
mentioning
confidence: 99%
“…To date, a number of key features of LID have been characterized; in particular, the nonlinear nature of the underlying electronic excitation is evidenced by the dependence of the desorption rate on the intensity of the incident pulse [3,7]. The surface two-photon absorption cross-section -evaluated based on the LID etch ratesis close to 25-times higher than that of bulk diamond [4,8]; moreover, the threshold-free nature and observed dependence on the polarization of incident photons [4,5] points to a surface-specific multi-photon-excited desorption mechanism. Given that etching of the O-terminated diamond surface is quenched in vacuum [2], it seems likely that carbon removal involves laser induced carbon monoxide (CO) desorption.…”
mentioning
confidence: 99%
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