Short-wavelength ablation of solids: pulse duration and wavelength effects

For conventional wavelength (UV-Vis-IR) lasers delivering radiation energy to the surface of materials, ablation thresholds, ablation (etch) rates, and the quality of ablated structures often differ dramatically between short (typically nanosecond) and ultrashort (typically femtosecond) pulses. Various short-wavelength (l < 100 nm) lasers emitting pulses with durations ranging from ~ 10 fs to ~ 1 ns have recently been put into a routine operation. This makes it possible to investigate how the ablation characteristics depend on the pulse duration in the XUV spectral region. 1.2-ns pulses of 46.9-nm radiation delivered from a capillary-discharge Ne-like Ar laser (Colorado State University, Fort Collins), focused by a spherical Sc/Si multilayer-coated mirror were used for an ablation of organic polymers and silicon. Various materials were irradiated with ellipsoidal-mirror-focused XUV radiation (λ = 86 nm, τ = 30-100 fs) generated by the free-electron laser (FEL) operated at the TESLA Test Facility (TTF1 FEL) in Hamburg. The beam of the Ne-like Zn XUV laser (λ = 21.2 nm, τ < 100 ps) driven by the Prague Asterix Laser System (PALS) was also successfully focused by a spherical Si/Mo multilayer-coated mirror to ablate various materials. Based on the results of the experiments, the etch rates for three different pulse durations are compared using the XUV-ABLATOR code to compensate for the wavelength difference. Comparing the values of etch rates calculated for short pulses with those measured for ultrashort pulses, we can study the influence of pulse duration on XUV ablation efficiency. Ablation efficiencies measured with short pulses at various wavelengths (i.e. 86/46.9/21.2 nm from the above-mentioned lasers and ~ 1 nm from the double stream gas-puff Xe plasma source driven by PALS) show that the wavelength influences the etch rate mainly through the different attenuation lengths.

[1]  G. G. Stokes "J." , 1890, The New Yale Book of Quotations.

[2]  Tomas Mocek,et al.  Multimillijoule, highly coherent x-ray laser at 21 nm operating in deep saturation through double-pass amplification , 2002 .

[3]  Richard A. London,et al.  X-ray optics research for free electron lasers: study of material damage under extreme fluxes , 2003 .

[4]  David A. G. Deacon,et al.  Optical coating damage and performance requirements in free electron lasers , 1986 .

[5]  R. Sobierajski,et al.  Sructural changes at solid surfaces irradiated with femtosecond, intense XUV pulses generated by TTF-FEL , 2003 .

[6]  N. V. Filippov,et al.  Megajoule scale plasma focus as efficient X-ray source , 1996 .

[7]  C S Menoni,et al.  Damage to extreme-ultraviolet Sc/Si multilayer mirrors exposed to intense 46.9-nm laser pulses. , 2004, Optics letters.

[8]  John B. Shoven,et al.  I , Edinburgh Medical and Surgical Journal.

[9]  Libor Juha,et al.  Ablation of Organic Polymers and Elemental Solids Induced by Intense XUV Radiation , 2002 .

[10]  B. L. Henke,et al.  X-Ray Interactions: Photoabsorption, Scattering, Transmission, and Reflection at E = 50-30,000 eV, Z = 1-92 , 1993 .

[11]  M. Stuke,et al.  Femtosecond uv excimer laser ablation , 1987 .

[12]  J. J. Roccaa,et al.  Extremely compact soft X-ray lasers based on capillary discharges , 2003 .

[13]  Per F. Peterson,et al.  X-ray response of National Ignition Facility first surface materials , 1994 .

[14]  H. Hiraoka,et al.  Radiation chemistry of poly(methacrylates) , 1977 .

[15]  Per F. Peterson,et al.  EXPERIMENTAL METHODS FOR MEASURING X-RAY ABLATION RESPONSE OF SURFACES , 1997 .

[16]  Hiroyuki Daido,et al.  Review of soft x-ray laser researches and developments , 2002 .

[17]  Bodil Braren,et al.  Ablation and etching of polymethylmethacrylate by very short (160 fs) ultraviolet (308 nm) laser pulses , 1987 .

[18]  Elke Plönjes,et al.  Taking free-electron lasers into the X-ray regime , 2003 .

[19]  Jorge J. Rocca,et al.  Table-top soft x-ray lasers , 1999, CLEO 2016.

[20]  Andrew Thomas Anderson X-ray ablation measurements and modeling for ICF applications , 1996 .

[21]  Libor Juha,et al.  Micromachining of organic polymers by direct photo-etching using a laser plasma X-ray source , 2004 .

[22]  P ? ? ? ? ? ? ? % ? ? ? ? , 1991 .

[23]  Thomas Weiland,et al.  A new powerful source for coherent VUV radiation: Demonstration of exponential growth and saturation at the TTF free-electron laser , 2002 .

[24]  Libor Juha,et al.  High-brightness laser plasma soft X-ray source using a double-stream gas puff target irradiated with the Prague Asterix Laser System (PALS) , 2004 .

[25]  Andreas K. Freund,et al.  Multilayer optics for intense synchrotron x-ray beams: Recent results on their performance , 1992 .

[26]  R. Sobierajski,et al.  Ablation of various materials with intense XUV radiation , 2003 .

[27]  J. M. Soures,et al.  Submicron x‐ray lithography using laser‐produced plasma as a source , 1983 .

[28]  Libor Juha,et al.  Total reflection amorphous carbon mirrors for vacuum ultraviolet free electron lasers , 2004 .

[29]  Takeshi Kanashima,et al.  Evaporation and Expansion of Poly-tetra-fluoro-ethylene Induced by Irradiation of Soft X-Rays from a Figure-8 Undulator , 2001 .

[30]  Y. Zhang,et al.  Synchrotron radiation direct photo etching of polymers , 2004 .

[31]  Hubertus Wabnitz Interaction of intense VUV radiation from a Free-Electron Laser with rare gas atoms and clusters , 2003 .

[32]  J. Rocca,et al.  Focusing of a tabletop soft-x-ray laser beam and laser ablation. , 1999, Optics letters.

[33]  James F. Young,et al.  Imaging characteristics of poly(methyl methacrylate) at vacuum ultraviolet wavelengths , 1997 .

[34]  Per F. Peterson,et al.  Modeling and Experiments of X-Ray Ablation of National Ignition Facility First Wall Materials , 1996 .