Laser sputtering: Part I. On the existence of rapid laser sputtering at 193 nm

Abstract Irradiation, i.e.bombardment, with 193 nm laser pulses having an energy fluence of 2.5 J cm 2 and a duration of ~12 ns leads to rapid sputtering with Au, Al2O3, MgO, MgO. Al2O3, SiO2, glass and LaB6, relatively slow sputtering with MgF2 and diamond, and mainly thermal-stress cracking with W. Scanning electron microscopy (SEM) suggests that the mechanism for the sputtering of Au in either vacuum or air is one based on the hydrodynamics of molten Au, while an SEM-derived surface temperature estimate confirms that thermal sputtering (which might have been expected) is not possible. SEM with W shows that the near total lack of material removal is due to the thermal-stress cracking not leading to completed exfoliation, together with the surface temperature being too low for either hydrodynamical or thermal processes. Corresponding SEM with Al2O3 shows, in the case of specimens bombarded in vacuum, topography of such a type that all mechanisms except electronic ones can be ruled out. The topography of Al2O3 or other oxides bombarded in air through a mask is somewhat different, showing craters as for vacuum bombardments but ones which have a cone-like pattern on the bottom.

[1]  J. C. Jaeger,et al.  Conduction of Heat in Solids , 1952 .

[2]  J. F. Figueira,et al.  Observations of the morphology of laser‐induced damage in copper mirrors , 1982 .

[3]  R. Kelly Thermal effects in sputtering , 1979 .

[4]  T. Tombrello Solar system sputtering , 1982 .

[5]  Joshua E. Rothenberg,et al.  Laser sputtering: Part III. The mechanism of the sputtering of metals low energy densities , 1985 .

[6]  R. Kelly The mechanisms of sputtering part I. , 1984 .

[7]  P. B. Price,et al.  Ion Explosion Spike Mechanism for Formation of Charged-Particle Tracks in Solids , 1965 .

[8]  C. Martin,et al.  Optical Properties of Some Transition Metals , 1968 .

[9]  O. Auciello,et al.  On the origin of pyramids and cones on ion-bombarded copper surfaces , 1980 .

[10]  Joshua E. Rothenberg,et al.  Laser sputtering. Part II. The mechanism of the sputtering of Al2O3 , 1984 .

[11]  N. Itoh,et al.  Mechanism of neutral particle emission from electron-hole plasma near solid surface , 1982 .

[12]  R. Ollerhead,et al.  Erosion of frozen-gas films by MeV ions , 1980 .

[13]  Y. S. Touloukian Thermal Expansion: Metallic Elements and Alloys , 1975 .

[14]  J. L. Hansen,et al.  The erosion of frozen argon by swift helium ions , 1981 .

[15]  Y. S. Touloukian Thermal Expansion: Nonmetallic Solids , 1977 .

[16]  G. J. Galvin,et al.  Time-resolved conductance and reflectance measurements of silicon during pulsed-laser annealing , 1983 .

[17]  T. Nakayama Laser-induced sputtering of ZnO, TiO2, CdSe and GaP near threshold laser fluence , 1983 .

[18]  A. N. Syverud,et al.  JANAF Thermochemical Tables, 1982 Supplement , 1982 .

[19]  Tony Huen,et al.  Optical Constants of Silver and Gold in the Visible and Vacuum Ultraviolet , 1971 .

[20]  W. Hunter,et al.  The optical properties of evaporated gold in the vacuum ultraviolet from 300 Å to 2 000 Å , 1964 .

[21]  M. Walmsley,et al.  Waves: A Mathematical Approach to the Common Types of Wave Motion , 1979 .

[22]  B. Appleton,et al.  Ion-beam mixing of metal-semiconductor eutectic systems , 1981 .

[23]  Jeff F. Young,et al.  Laser‐induced periodic surface damage and radiation remnants , 1982 .

[24]  R. S. Robinson,et al.  Ion‐beam‐induced topography and surface diffusion , 1982 .

[25]  R. Srinivasan,et al.  Kinetics of the ablative photodecomposition of organic polymers in the far ultraviolet (193 nm) , 1983 .

[26]  S. T. Picraux,et al.  Slip deformation and melt threshold in laser‐pulse‐irradiated Al , 1981 .

[27]  R. A. McDonald,et al.  JANAF thermochemical tables, 1978 supplement , 1978 .