Abstract

Two methods were used for the deposition of thin films and layers: pulsed laser deposition (PLD) and laser-induced film transfer (LIFT). The first one was based on using KrF laser radiation. Thin films and layers were deposited by KrF laser ablation of CrSi<sub>2</sub> and &beta;-FeSi<sub>2</sub> targets with the aim to obtain silicide layers with narrow band gap for sensor applications. The CrSi<sub>2</sub>-based films display both semiconductor and metal properties, depending on the deposition parameters. Thus, the film d &cong; 40 nm thick, deposited on Si at 740 K, presents a band gap E<sub>g</sub> &cong; 0.18 eV, a thermo e.m.f. coefficient &alpha; &cong; 1.0-1.4 mV/K for 300&le;T&le;340 K and a coefficient of tensosensitivity (R-R<sub>0</sub>)/R<sub>0&epsilon;</sub>) &cong; 5. The film with the same thickness, but deposited on SiO<sub>2</sub> at 740 K, presents a metal behavior in the range 125&le;T&le;296 K and a semiconductor one for 77&le;T&le;125 K. Its &alpha; coefficient changes in the range 5.0 - 7.5 &mu;V/K for 300&le;T&le;340 K. The 750 nm thick film deposited on SiO<sub>2</sub> at 740 K displays only semiconductor behavior in the range 296-77 K with E<sub>g</sub> &cong; 0.013 eV and &alpha; &cong; 10-15 &mu;V/K for 293&le;T&le;340 K. The coefficient of tensosensitivity for these films is changing in the range 2-5. The &beta;-FeSi<sub>2</sub>-based films deposited on SiO<sub>2</sub> at 295&le;T&le;740 K show only semiconductor behavior. The thicker the film, the higher E<sub>g</sub>: d &cong; 150 nm, E<sub>g</sub> &cong; 0.032 eV; d &cong; 70 nm, E<sub>g</sub> &cong; 0.027 eV; d &cong; 60 nm, E<sub>g</sub> &cong; 0.023 eV. The thermo e.m.f coefficient &alpha; &cong; 10 &mu;V/K for the 150 nm thick film and &alpha; 8 &mu;V/K for the 60 nm thick film at 293&le;T&le;340 K. The coefficient of tensosensitivity for these films varies in the range 2.3-4.7. The second one was based on LIFT of CrSi<sub>2</sub> and &beta;-FeSi<sub>2</sub> targets, using a Q-switched Nd: YAG laser. The &alpha; coefficient for the deposited layer from &beta;-FeSi<sub>2</sub> is about 2.2 &mu;V/K with E<sub>g</sub> &cong; 0.05 eV. While decreasing the average power density of the Q-switched Nd: YAG laser, the band gap decreases down to 0.005 eV. For this film we found &alpha; &cong; 2.0 &mu;V/K. The &alpha; coefficient for the deposited layer from CrSi<sub>2</sub> is about 36 &mu;V/K with E<sub>g</sub> &cong; 0.09 eV. Coefficient of thermo e.m.f. for layers obtained by LIFT method was measured at 300&le;T&le;350 K. The coefficient of tensosensitivity for layers obtained by LIFT varied in the range 1.5-4.2. The higher the semiconductor phase content in the deposited films and layers obtained by PLD and LIFT methods, the higher are the values of &alpha; and (R-R<sub>0</sub>)/R<sub>0&epsilon;.</sub>

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