248 nm excimer laser ablation of carefully prepared CuCl samples is reported, and shown to occur by a predominantly thermal mechanism. Using a quartz‐crystal microbalance (QCM) to monitor ablation, a precise and detailed plot of single‐pulse mass removal versus incident fluence was obtained for fluences up to 150 mJ/cm2. A two‐parameter Arrhenius exponential function was found to fit the experimental ablation data. Calculations of laser‐induced surface heating were carried out by use of a finite‐difference heating code, formulated in terms of enthalpy. Ablation was observed to commence at a fluence of 25 mJ/cm2, where the calculated surface temperature is approximately 910 K—some 200 K above the melting point. Dynamic ablation was included in the finite‐difference calculation by allowing the position of the CuCl surface ξ to vary in time. The best data fit is provided by the zeroth‐order kinetic equation: dξ(t)/dt=(16 Å/ns)exp[(−38 kJ/mole)/RTξ], where Tξ is the surface temperature. A thermodynamic calculation shows the average heat of CuCl vaporization in the temperature range from 900 to 2000 K to be near the fit value of 38 kJ/mole. From plots of the ablation depth versus time, the CuCl surface was estimated to recede during the ablation at rates up to 10 cm/s.
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15 July 1994
Research Article|
July 15 1994
Thermal activation in KrF laser ablation of CuCl
S. Küper;
S. Küper
IBM Almaden Research Center, 650 Harry Road, San Jose, California 95120
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K. Brannon;
K. Brannon
IBM Almaden Research Center, 650 Harry Road, San Jose, California 95120
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J. Brannon
J. Brannon
IBM Almaden Research Center, 650 Harry Road, San Jose, California 95120
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J. Appl. Phys. 76, 1203–1209 (1994)
Article history
Received:
December 02 1993
Accepted:
March 30 1994
Citation
S. Küper, K. Brannon, J. Brannon; Thermal activation in KrF laser ablation of CuCl. J. Appl. Phys. 15 July 1994; 76 (2): 1203–1209. https://doi.org/10.1063/1.357848
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