Studies of plasma surface interactions during short time plasma etching of 193 and 248nm photoresist materials

  • Xuefeng Hua
    University of Maryland Department of Physics, , College Park, Maryland 20742 and Institute for Research in Electronics and Applied Physics, , College Park, Maryland 20742
  • S. Engelmann
    University of Maryland Department of Materials Science and Engineering, , College Park, Maryland 20742 and Institute for Research in Electronics and Applied Physics, , College Park, Maryland 20742
  • G. S. Oehrlein
    University of Maryland Department of Materials Science and Engineering, , College Park, Maryland 20742 and Institute for Research in Electronics and Applied Physics, , College Park, Maryland 20742
  • P. Jiang
    Texas Instruments, Inc. , Dallas, Texas 75243
  • P. Lazzeri
    Center for Scientific and Technological Research (ITC-irst) , 38050 Povo, Trento, Italy
  • E. Iacob
    Center for Scientific and Technological Research (ITC-irst) , 38050 Povo, Trento, Italy
  • M. Anderle
    Center for Scientific and Technological Research (ITC-irst) , 38050 Povo, Trento, Italy

抄録

<jats:p>As the device dimensions scale to 100nm, the use of photoresist materials is suitable for lithographic patterning at 193nm. The molecular structure of 193nm photoresist materials is significantly different from that of 248nm photoresist materials [H. Ito, IBM J. Res. Deu. 45, 683 (2001), T. Kajita et al., Proc. SPIE 4345, 712 (2001)], which leads to a number of undesirable consequences, including pronounced surface and line edge roughness during plasma etching [H. Ito, IBM J. Res. Deu. 41, 69 (1997), [E. Reichmanis et al., J. Vac. Sci. Technol. B 15, 2528 (1997), [L. Ling et al., ibid. 22, 2594 (2004)]. In this article, we present an investigation of the mechanisms for the surface/line edge roughening of photoresist materials during plasma etching using C4F8∕90%Ar discharges. We emphasized in our study short exposure times (the first few seconds) of the photoresist materials and structures to the plasma, a time regime that has not been well studied. Rapid modifications were observed for both 193 and 248nm photoresists during short time exposure. During the first seconds of plasma exposure, photoresist material densification and hydrogen depletion are important processes. It is also found that rough surfaces develop within a few seconds of exposure to the C4F8∕90%Ar discharges. Plasma exposure leads to the formation of rough edges on the top of trench sidewalls in photoresist trench and line structures. During prolonged exposure to the plasma, the roughness is transferred to produce striations on the sidewalls. After an initial stage, the roughening rate remains constant for 193nm photoresist, whereas for 248nm photoresist the roughening rate is negligible. This difference is possibly related to the preferential removal of carbonyl groups for the 193nm photoresist material, which has been revealed by x-ray photoelectron spectroscopy and seconday ion mass spectroscopy.</jats:p>

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