With low-peak-power sources, materials are removed by photon-induced desorption of material components from the irradiated sample surface. Each XUV/x-ray photon carries enough energy to break any chemical bond. This energy is also usually higher than the cohesive energy of any crystal. Therefore, the photons absorbed in a near-surface region may create small fragments of a sample material, which are emitted into the vacuum. It is necessary to underline, that in the case of low-peak-intensity irradiation, material is removed from the surface and a very thin near-surface layer only. Quite a different situation is expected if a high-peak-power source delivers a single high-energy pulse to the sample. The sample is then exposed to a high local dose of radiation (given by the energy content of the pulse and the absorption length of the radiation in the irradiated material) in a short period of time (given by the pulse length), i.e. at a very high dose rate. This means that a large number of events that cause radiation-induced structural decomposition (i.e. polymer chain scissions, etc.), occur almost simultaneously in a relatively thick layer of irradiated material. Since a portion of the radiation energy absorbed in the material will be thermalized, the sudden heating of the layer, which is also heavily chemically altered by the radiation, must be taken into account. The overheated, fragmented region of the sample represents a new phase, which tends to blow off into the vacuum. These particular processes, as well as specific features of short-wavelength ablation, with respect to ablation induced by conventional UV-Vis-IR sources, represent the subject of our research. Ablation characteristics, i.e. thresholds, etch (ablation) rates, and ablated structure quality, often differ dramatically with conventional UV-Vis-IR lasers, depending on whether the radiation energy is delivered to the material surface in either short (typically nanosecond) or ultra-short (typically femtosecond) pulses. Does such a difference also exist for lasers operating in the XUV (λ < 100 nm) spectral region? This question can now be answered due to the availability of XUV lasers with pulse durations ranging from tens of femtoseconds to several nanoseconds. These sources, whichonly recently became available, are promising tools for appli cations in the field of nano-patterning of solids, as they will enable the printing of features with dimensions comparable to the wavelength. A key advantage of XUV lasers for nano-structure fabrication is the unique combination of exceptionally short wavelength, spatial coherence, and high peak power. The ablation threshold for processing materials makes it necessary for XUV sources to deliver enough fluence and thus sufficiently high power to the irradiated surface area. Although non-coherent sources developed for XUV lithography can also pattern material surfaces at sub-10-nm resolutions, they cannot directly produce three-dimensional structures using only a few shots in a single processing step. Recently it has been demonstrated that intense XUV radiation can directly produce sub-100-nm structures quite easily. Grating-like structures (i.e. LIPSS – laser-induced periodic surface structures) with a spatial period about 70 nm have already been produced in amorphous carbon (a-C; [8]) and poly(methyl methacrylate) – PMMA [6] surfaces irradiated with FEL radiation at 98 nm and 86 nm, respectively. Recent publications [1] L. Juha, J. Krása, A. Präg, A. Cejnarová, D. Chvostová, K. Rohlena, K. Jungwirth, J. Kravárik, P. Kubeš, Yu. L. Bakshaev, A. S. Chernenko, V. D. Korolev, V. I. Tumanov, M. I. Ivanov, A. Bernardinello, J. Ullschmied, F. P. Boody: Ablation of poly(methyl methacrylate) by a single pulse of soft X-rays emitted from Z-pinch and laser-produced plasmas, Surf. Rev. Lett. 9, 347–352 (2002). [2] L. Juha, J. Krása, A. Cejnarová, D. Chvostová, V. Vorlíček, J. Krzywinski, R. Sobierajski, A. Andrejczuk, M. Jurek, D. Klinger, H. Fiedorowicz, A. Bartnik, M. Pfeifer, P. Kubát, L. Pína, J. Kravárik, P. Kubeš, Yu. L. Bakshaev, A. S. Chernenko, V. D. Korolev, M. I. Ivanov, M. Scholz, L. Ryc, J. Feldhaus, J. Ullschmied, F. P. Boody: Ablation of various materials with intense XUV radiation, Nucl. Instrum. Meth. Phys. Res. A507, 577–581 (2003). [3] H. Fiedorowicz, A. Bartnik, L. Juha, K. Jungwirth, B. Kralikova, J. Krasa, P. Kubat, M. Pfeifer, L. Pina, P. Prchal, K. Rohlena, J. Skala, J. Ullschmied, M. Horvath, J. Wawer: High-brightness laser plasma soft X-ray source using a double-stream gas puff target irradiated with the Prague Asterix Laser System (PALS), J. Alloys Comp. 362, 67–70 (2004) [4] H. Fiedorowics, A. Bartnik, M. Bittner, L. Juha, J. Krasa, P. Kubat, J. Mikolajczyk, R. Rakowski, Micromachining of organic polymers by direct photo-etching using a laser plasma X-ray source, Microelectronic Eng. 73–74, 336–339 (2004). [5] L. Juha, J. Krzywinski, A. Andrejczuk, M. Bittner, F. P. Boody, D. Chvostova, J. Feldhaus, M. E. Grisham, J. Krasa, V. Letal, C. S. Menoni, J. B. Pelka, Z. Otcenasek, J. J. Rocca, R. Sobierajski, G. O. Vaschenko, Comparing etch rates of poly(methyl methacrylate) ablated by nanosecond and femtosecond pulses of XUV-laser radiation, HASYLAB Annual Report 2003 – Part I., 241–242 (2003) [6] L. Juha, J. Krzywinski, A. Andrejczuk, M. Bittner, J. Feldhaus, J. B. Pelka, R. Sobierajski, B. Steeg, A. Wawro, Laser-induced periodic surface structures (LIPSS) produced by short-wavelength, fast beam of TTF1 FEL, HASYLAB Annual Report 2003 – Part I., 763–764 (2003) [7] M. Bittner, L. Juha, D. Chvostova, V. Letal, J. Krasa, Z. Otcenasek, M. Kozlova, J. Polan, A. R. Praeg, B. Rus, M. Stupka, J. Krzywinski, A. Andrejczuk, J. B. Pelka, R. Sobierajski, J. Feldhaus, F. P. Boody, M. E. Grisham, G. O. Vaschenko, C. S. Menoni, J. J. Rocca, Comparing ablation induced by fs, ps and ns XUV-laser pulses, Proceedings of the High-Power Laser Ablation 2004, April 25–30, 2004 Taos USA, Proc. SPIE 5448, 827–836 (2004). [8] B. Steeg, L. Juha, J. Feldhaus, S. Jacobi, R. Sobierajski, C. Michaelsen, A. Andrejczuk, J. Krzywinski: Total reflection amorphous carbon mirrors for VUV Free Electron Laser, Appl. Phys. Lett. 84, 657–659 (2004). [9] L. Juha, M. Bittner, D. Chvostová, V. Létal, J. Krása, Z. Otčenášek, M. Kozlová, J. Polan, A. R. Präg, B. Rus, M. Stupka, J. Krzywinski, A. Andrejczuk, J. B. Pelka, R. Sobierajski, L. Ryc, J. Feldhaus, F. P. Boody, H. Fiedorowicz, A. Bartnik, J. Mikolajczyk, R. Rakowski, L. Pína, M. E. Grisham, G. O. Vaschenko, C. S. Menoni, J. J. Rocca: Short-wavelength ablation of solids: pulse duration and wavelength effects, Proc. SPIE 5534, 95–107 (2004). [10] L. Juha, M. Bittner, D. Chvostova, J. Krasa, Z. Otcenasek, A. R. Präg, J. Ullschmied, Z. Pientka, J. Krzywinski, J. B. Pelka, A. Wawro, M. E. Grisham, G. Vaschenko, C. S. Menoni, and J. J. Rocca: Ablation of organic polymers by 46.9-nm laser radiation, Appl. Phys. Lett. 86, 034109 (2005). Networking [A] inland
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