AVS 56th International Symposium & Exhibition | |
Plasma Science and Technology | Thursday Sessions |
Session PS1-ThM |
Session: | Applications of Plasma-Surface Interactions |
Presenter: | K. Nakamura, Kyoto University, Japan |
Authors: | K. Nakamura, Kyoto University, Japan Y. Ueda, Kyoto University, Japan H. Kiyokami, Kyoto University, Japan H. Tsuda, Kyoto University, Japan K. Eriguchi, Kyoto University, Japan K. Ono, Kyoto University, Japan |
Correspondent: | Click to Email |
Selective etching of high dielectric constant (high-k) films over the underlying Si (and/or SiO2) is indispensable in the fabrication of high-k gate stacks. In practice, the selectivity is usually not so high, owing to highly volatile halogen compounds of Si, and also to strong metal-oxygen bonds of high-k dielectrics and less volatile metal-halogen compounds. Profile control is also indispensable during etching of high-k: anisotropic profiles are required for high-k, and also profiles of gate electrodes on high-k are required to remain unchanged. This paper presents the control of selectivity and profile for high-k HfO2 etching under low ion-energy conditions in BCl3-containing plasmas, with emphasis being placed on a better understanding of the etching mechanisms concerned. Experiments were performed in both electron cyclotron resonance (ECR) and inductively coupled (ICP) plasmas, by varying pressure, additive concentration of O2, Cl2, and Ar, rf bias power, and also substrate temperature. Samples for etching were blanket HfO2 and TaN films, and separate Si and SiO2 substrates were also employed for reference. Samples of TaN/HfO2 stack as well as separate HfO2 and TaN masked with line-and-space patterns were also employed to examine the etched profile. We examined substrate surfaces by x-ray photoelectron spectroscopy, and investigated reactant and product species in the plasma during etching by optical emission spectroscopy and quadrupole mass spectrometry. A transition from deposition to etching regimes was found to be caused on all substrate surfaces, by varying pressure, by using additives such as O2 and Cl2, and by increasing rf bias power. In practice, surface inhibitor deposition was less significant for HfO2 than for Si, SiO2, and TaN; and the threshold bias power or ion energy for HfO2 etching was in the range 10-20 eV, while the threshold was more than 20 eV for the other. A difference in pressure, additive concentration, and bias power for the transition between HfO2 and Si (and/or SiO2) gave rise to high or infinite selectivity of high-k over Si (and/or SiO2), together with vertical high-k profiles. The difference for the transition between HfO2 and TaN also gave no significant distortion of TaN profiles during HfO2 etching, owing to passivation layers deposited on TaN sidewalls. Plasma and surface diagnostics indicated that inhibitor species for deposition are primarily boron-chloride polymers produced in the plasma, whose concentration largely depends on pressure, additive concentration, and plasma reactor (ECR and ICP), which in turn leads to a marked difference in etching characteristics.