Amorphous (a-C) Carbon thin films were deposited, using pulsed laser deposition (PLD) with a Nd:YAG laser ( 1064 nm, 7 ns), from a pyrolytic graphite target, on < 1 0 0 > silicon and refractory metal (Mo) substrates to a film thickness of 55, 400 and 500 nm. Samples were grown at RT and then annealed by a laser annealing technique, to reduce residual stress and induce a locally confined "graphitization'' process. The films were exposed to irradiation, in vacuum, by a Nd: YAG pulsed laser, operating at different wavelengths ( VIS, N-UV) and increasing values of energy from 6-100 mJ/pulse. The thinner films were completely destroyed by N-UV laser treatment also at lower energies, owing to the almost direct propagation of heat to the Si substrate with melting and ruinous blistering effects. For thicker films the Raman micro-analysis evidenced the influence of laser treatments on the sp(3)/sp(2) content evolution, and established the formation of aromatic nano-structures of average dimension 4.1 divided by 4.7 nm ( derived from the I-D/I-G peak ratio), at fluence values round 50 mJ/cm(2) for N-UV and 165 mJ/cm(2) for VIS laser irradiation. Higher fluences were not suitable for a-Carbon "graphitization'', since a strong ablation process was the prominent effect of irradiation. Grazing incidence XRD (GI-XRD) used to evaluate the dimension and texturing of nano-particles confirmed the findings of Raman analysis. The effects of irradiation on surface morphology were studied by SEM analysis.

Laser annealing of amorphous carbon films

Cappelli E;Orlando S;Valentini V;Servidori M
2009

Abstract

Amorphous (a-C) Carbon thin films were deposited, using pulsed laser deposition (PLD) with a Nd:YAG laser ( 1064 nm, 7 ns), from a pyrolytic graphite target, on < 1 0 0 > silicon and refractory metal (Mo) substrates to a film thickness of 55, 400 and 500 nm. Samples were grown at RT and then annealed by a laser annealing technique, to reduce residual stress and induce a locally confined "graphitization'' process. The films were exposed to irradiation, in vacuum, by a Nd: YAG pulsed laser, operating at different wavelengths ( VIS, N-UV) and increasing values of energy from 6-100 mJ/pulse. The thinner films were completely destroyed by N-UV laser treatment also at lower energies, owing to the almost direct propagation of heat to the Si substrate with melting and ruinous blistering effects. For thicker films the Raman micro-analysis evidenced the influence of laser treatments on the sp(3)/sp(2) content evolution, and established the formation of aromatic nano-structures of average dimension 4.1 divided by 4.7 nm ( derived from the I-D/I-G peak ratio), at fluence values round 50 mJ/cm(2) for N-UV and 165 mJ/cm(2) for VIS laser irradiation. Higher fluences were not suitable for a-Carbon "graphitization'', since a strong ablation process was the prominent effect of irradiation. Grazing incidence XRD (GI-XRD) used to evaluate the dimension and texturing of nano-particles confirmed the findings of Raman analysis. The effects of irradiation on surface morphology were studied by SEM analysis.
2009
Istituto per la Microelettronica e Microsistemi - IMM
Istituto di Struttura della Materia - ISM - Sede Roma Tor Vergata
Istituto dei Sistemi Complessi - ISC
Pulsed laser irradiation
Graphitizing process
a-Carbon films
Carbon nano-structures
GI-XRD analysis
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/151032
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