Ablation yields and thresholds for 193 nm UV laser ablation of ultrathin HfO2 are presented. The single shot threshold fluence increases approximately linearly with HfO2 thickness form 28 nm to 120 nm. Due to the logarithmic dependence of ablation depth on fluence this result with increasing layer thickness in an exponential increase of fluence necessary for clean ablation of the whole layer. The observed ablation depth for fixed HfO2 thickness can be reproduced phenomenologically by taking ablation from the HfO2 film as well as the quartz substrate into account. As a first approach to a quantitative understanding we calculate numerically the heat evolution in the layered system and identificate ablation with the onset of melting of the absorbing layer. Whereas the ablation curve for a 74 nm thick film can be reproduced that way, this is not the case for the case for the overall thickness dependence of the ablation threshold. This points to possible finite size effects for the phonon-phonon scattering rate in the thin dielectric layers.
[1]
Jan Siegel,et al.
UV-laser ablation of ductile and brittle metal films
,
1997
.
[2]
B. Wolff-Rottke,et al.
Excimer laser ablation patterning of dielectric layers
,
1995
.
[3]
J. Siegel,et al.
The influence of thermal diffusion on laser ablation of metal films
,
1994
.
[4]
Aaas News,et al.
Book Reviews
,
1893,
Buffalo Medical and Surgical Journal.
[5]
Size effects and determination of absolute temperature increases in laser heating of dielectrics
,
1995
.
[6]
J. Ihlemann,et al.
Graded transmission dielectric optical masks by laser ablation
,
1998
.
[7]
Lee,et al.
Thermal conductivity of sputtered oxide films.
,
1995,
Physical review. B, Condensed matter.
[8]
C. Henager,et al.
Thermal conductivities of thin, sputtered optical films.
,
1993,
Applied optics.
[9]
C. Zheng,et al.
; 0 ;
,
1951
.