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312–317, ISSN 0040-6090. ; Forder, S. -D. (2000). The interface between TiAlN hard coatings and steel substrates generated by high energetic Cr+ bombardment. Surface & Coatings Technology, Vol. 125, No. 1, pp. 6670, ISSN 0257-8972. ; Sakata, T. & Mori, H. (1997). Phase variation and properties of (Ti, Al)N films prepared by ion beam assisted deposition . Surface & Coatings Technology, Vol. 97, No. 1, pp. 254-258, ISSN 02578972. Shieh, J. H. (2001). Nanostructure and hardness of titanium aluminum nitride prepared by plasma enhanced chemical vapor deposition.

Nanostructure and hardness of titanium aluminum nitride prepared by plasma enhanced chemical vapor deposition. Thin Solid Films, Vol. 391, No. 1, pp. 101-108, ISSN 0040-6090. I. & Borodko. G. (1976). X-ray Photoelectronspectra of scandium, titanium, vanadium and chromium mononitrides, Zhurnal Neorganicheskoi khimii, Vol. 21, No. 10, pp. 2621-2624, ISSN 0036-0236. F. G. (2004). Structural and mechanical properties of titanium–aluminium–nitride films deposited by reactive close-field unbalanced magnetron sputtering, Surface & Coatings Technology, Vol.

It is clear that a Td, slow value too long reduces the number of the counts in the measured spectrum (analyzed events) and its optimum value is the best compromise between the required energy resolution and throughput. The time Ta is paralyzable dead time for the slow shaping operation. Both fast and slow procedures gave consistent values of the incoming photon counting rate. 1 Pulse shape discrimination A pulse shape discrimination (PSD) technique was implemented in our DPP system by analyzing the peaking time distribution of the pulses and their correlations with the energy spectra.

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