Crossref journal-article
American Vacuum Society
Journal of Vacuum Science and Technology (20)
Abstract

Radio-frequency sputtering cannot be used for absolute measurements of sputtering yields because of the spread in energies of the bombarding ions. This paper describes how these yields can be studied by simultaneously sputtering with the insulators other materials with known dc sputtering yields. Silicon and germanium were selected as reference materials. The dielectric materials studied were fused quartz, Pyrex 7740 glass, Pyrex 7059 glass, soda lime glass, and aluminum oxide (Lucalox). The experiments were performed in an Argon atmosphere at 3 × 10−3 Torr and at rf electrode potentials between 1.3 and 3.9 kV peak-to-peak. The frequency in all experiments was 13.56 MHz. Sputtering yields were found to be highest for fused quartz (0.16 to 0.5 molecules/ion) and lowest for aluminum oxide (0.04 to 0.17 molecules/ion). The data for fused quartz were found to fall between published low-energy yields determined by Langmuir probe and very high-energy yields determined by ion beams.

Bibliography

Davidse, P. D., & Maissel, L. I. (1967). Equivalent dc Sputtering Yields of Insulators. Journal of Vacuum Science and Technology, 4(1), 33–36.

Authors 2
  1. P. D. Davidse (first)
  2. L. I. Maissel (additional)
References 0 Referenced 29

None

Dates
Type When
Created 23 years, 1 month ago (July 27, 2002, 5:34 a.m.)
Deposited 2 years, 2 months ago (June 28, 2023, 6:23 p.m.)
Indexed 4 days ago (Sept. 2, 2025, 6:35 a.m.)
Issued 58 years, 8 months ago (Jan. 1, 1967)
Published 58 years, 8 months ago (Jan. 1, 1967)
Published Print 58 years, 8 months ago (Jan. 1, 1967)
Funders 0

None

@article{Davidse_1967, title={Equivalent dc Sputtering Yields of Insulators}, volume={4}, ISSN={0022-5355}, url={http://dx.doi.org/10.1116/1.1492514}, DOI={10.1116/1.1492514}, number={1}, journal={Journal of Vacuum Science and Technology}, publisher={American Vacuum Society}, author={Davidse, P. D. and Maissel, L. I.}, year={1967}, month=jan, pages={33–36} }