2019
DOI: 10.1039/c9na00223e
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Doping nanoparticles using pulsed laser ablation in a liquid containing the doping agent

Abstract: While doping is crucial for numerous technological applications, its control remains difficult especially when the material is reduced down to the nanometric scale. We suggest a new way to dope nanoparticles using laser ablation in liquids.

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Cited by 24 publications
(19 citation statements)
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“…The emission spectrum of the Laser Induced Plasma (LIP) under water is characterized mainly by continuum radiation with possibly some resonance peaks of the element constituting the target [ 40 ]. The absence of the typical atomic spectral lines of the LIP expanding in a gaseous environment is due to the high density reached by the ablated matter under liquid confinement as discussed in [ 40 , 41 , 42 ]. In this case, the emission spectrum has a Planck-like shape that has been ascribed to the radiative recombination and that in turn is proportional to the blackbody law, although the spectrum is not related to any blackbody system.…”
Section: Lal Synthesis Methods: Principle Process Parameters and mentioning
confidence: 99%
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“…The emission spectrum of the Laser Induced Plasma (LIP) under water is characterized mainly by continuum radiation with possibly some resonance peaks of the element constituting the target [ 40 ]. The absence of the typical atomic spectral lines of the LIP expanding in a gaseous environment is due to the high density reached by the ablated matter under liquid confinement as discussed in [ 40 , 41 , 42 ]. In this case, the emission spectrum has a Planck-like shape that has been ascribed to the radiative recombination and that in turn is proportional to the blackbody law, although the spectrum is not related to any blackbody system.…”
Section: Lal Synthesis Methods: Principle Process Parameters and mentioning
confidence: 99%
“…The photoionization cross section at high density conditions, shows a smooth dependence on wavelength [ 42 ], so that its contribution can be considered constant in the range of photon energy investigated in the visible range, i.e., 1–3 eV. In the frame of this assumption and since, at fixed time N e and T are constant, Equation (5) becomes: where G is a constant with respect to wavelength at each time of plasma lifetime since it represents a function depending on detection efficiency, on the electron number density and on plasma temperature, but not on the wavelength.…”
Section: Lal Synthesis Methods: Principle Process Parameters and mentioning
confidence: 99%
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“…To increase the nanoparticle yield from oxide targets in LAL, unwanted byproducts in the form of microparticles should be minimized, which is achieved by using mechanically stable targets. In this way, challenging materials like ternary oxide nanoparticles [29,30] or doped nanoparticles [31,32] can be produced.…”
Section: Introductionmentioning
confidence: 99%