AVS 62nd International Symposium & Exhibition | |
Plasma Science and Technology | Thursday Sessions |
Session PS-ThP |
Session: | Plasma Science and Technology Poster Session |
Presenter: | Sanbir Kaler, University of Houston |
Authors: | S. Kaler, University of Houston Q. Lou, University of Houston V.M. Donnelly, University of Houston J. Economou, University of Houston |
Correspondent: | Click to Email |
Atomic Layer Etching (ALEt) with monolayer accuracy is a critical requirement for advancing nanoscience and nanotechnology. Current plasma etching techniques do not have the level of control or damage-free nature that is needed for patterning delicate sub-10 nm structures with uniform etching rates and higher selectivities. Here we present beam studies of ALEt of SiO2. Substrates consisting of thin layers of SiO2 on Si are placed in an ultrahigh vacuum (UHV) chamber, cleaned with an oxygen plasma beam, and then exposed first to a beam of species effusing from a C4F8 plasma, followed by bombardment by an Ar+ beam. The C4F8 plasma beam deposits a fluorocarbon (FC) film and the Ar+ beam removes the film along with a small amount of SiO2. The process is then repeated. Multiple times between each step, the sample is moved under vacuum to another UHV chamber equipped with x-ray photoelectron spectroscopy (XPS). Changes in FC film thickness and composition are measured as a function of exposure time to the C4F8 plasma beam. Similarly, changes are measured in the FC film and SiO2 film thickness and composition as a function of Ar+ beam exposure time. The FC film first deposits rapidly, then nearly saturates at a thickness of 0.8 nm and then continues to grow at a much slower steady rate. Stopping at this saturation FC film thickness and exposing the sample to a ~120 eV Ar+ beam removes 0.08 nm of SiO2, concomitant with the loss of CF3 and CF2 moities (but not of C and F), and then continues to sputter SiO2 at a much slower rate. The 7:1 F:C ratio observed after 0.8 nm FC film deposition is much higher than the F:C ratio computed from a peak fit of the C(1s) high resolution spectrum (1.3:1), indicating that most of the F is bound in the SiO2 film. Further details and mechanisms for the ALEt process will be presented.