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Photo enhanced CVD

In this section we will describe two forms of LCVD using laser beams. The deposition rate enhancement can be by  [Pg.160]

Deutsch and Rathman193 showed that using an ArF laser beam parallel to the substrate, tungsten depositions can be obtained in a H2/WF6 gas mixture at 8 Torr. The substrate temperature was varied between 200 and 440°C. At 440°C, the bulk resistivity was about 17 /rOcm. However, below 350°C, high resistivity (100-300 /iflcm) /3-W is obtained. By a heat treatment at 650°C in H2 the /3-W phase can be converted into the a-W phase. The activation energy found for the photo reaction was 40.7 kJ/mole. [Pg.160]

Tsuzuku et al.195 also used an ArF laser with the beam parallel to the substrate (10 mm above). While varying the substrate temperature between 350 and 450°C, tungsten depositions were obtained in a H2/WF6 mixture. In their case no /3-W was reported. The reaction orders obtained were one for hydrogen and 1/2 for WF6 according to the rate expression  [Pg.160]

The activation energy for the photo enhanced reaction is 35 kJ/mole which is similar to the value obtained by Deutsch and Rathman. The authors note that this is close to the activation energy of atomic hydrogen diffusion on a tungsten surface (40 kJ/mole). Tsuzuku ct al. come to the following proposal for the reaction route  [Pg.161]

Only depositions of tungsten on Si substrates were obtained. No tungsten was found on thermal oxide. A complication found was that the tungsten lines were partially silicided in the center. [Pg.163]


See other pages where Photo enhanced CVD is mentioned: [Pg.195]    [Pg.160]    [Pg.222]   


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