High brightness inductively coupled plasma source for high current focused ion beam applications
| dc.contributor.author | Smith, N. S. | |
| dc.contributor.author | Skoczylas, W. P. | |
| dc.contributor.author | Kellogg, S. M. | |
| dc.contributor.author | Kinion, D. E. | |
| dc.contributor.author | Tesch, P. P. | |
| dc.contributor.author | Sutherland, O. | |
| dc.contributor.author | Aanesland, Ane | |
| dc.contributor.author | Boswell, R. W. | |
| dc.date.accessioned | 2015-11-06T03:31:42Z | |
| dc.date.available | 2015-11-06T03:31:42Z | |
| dc.date.issued | 2006-11-30 | |
| dc.date.updated | 2015-12-08T02:46:51Z | |
| dc.description.abstract | A high brightnessplasmaion source has been developed to address focused ion beam(FIB) applications not satisfied by the liquid metal ion source (LMIS) based FIB. The plasmaFIB described here is capable of satisfying applications requiring high mill rates (>100μm³/s) with non-gallium ions and has demonstrated imaging capabilities with sub- 100-nm resolution. The virtual source size, angular intensity, mass spectra, and energy spread of the source have been determined with argon and xenon. This magnetically enhanced, inductively coupled plasmasource has exhibited a reduced brightness(βr) of 5.4×10³Am⁻²sr⁻¹V⁻¹, with a full width half maximum axial energy spread (ΔE) of 10eV when operated with argon. With xenon, βr=9.1×10³Am⁻²sr⁻¹V⁻¹ and ΔE=7eV. With these source parameters, an optical column with sufficient demagnification is capable of forming a sub-25-nm spot size at 30keV and 1pA. The angular intensity of this source is nominally three orders of magnitude greater than a LMIS making the source more amenable to creating high current focused beams, in the regime where spherical aberration dominates the LMIS-FIB. The source has been operated on a two lens ion column and has demonstrated a current density that exceeds that of the LMIS-FIB for current greater than 50nA. Source lifetime and current stability are excellent with inert and reactive gases. Additionally, it should be possible to improve both the brightness and energy spread of this source, such that the (βr/ΔE₂) figure-of-merit could be within an order of magnitude of a LMIS. | |
| dc.identifier.issn | 1071-1023 | en_AU |
| dc.identifier.uri | http://hdl.handle.net/1885/16393 | |
| dc.publisher | American Institute of Physics (AIP) | |
| dc.rights | http://www.sherpa.ac.uk/romeo/issn/1071-1023..."Publishers version/PDF may be used on author's personal website, institutional website or institutional repository" from SHERPA/RoMEO site (as at 6/11/15). Copyright 2006 American Institute of Physics. This article may be downloaded for personal use only. Any other use requires prior permission of the author and the American Institute of Physics. The following article appeared in Journal of Vacuum Science & Technology B and may be found at https://doi.org/10.1116/1.2366617 | |
| dc.source | Journal of Vacuum Science & Technology B: Microelectronics and Nanometer Structures | |
| dc.subject | Keywords: Current density; Imaging techniques; Ion beams; Lenses; Optical properties; Optical resolving power; Angular intensity; Imaging capabilities; Spherical aberration; Inductively coupled plasma | |
| dc.title | High brightness inductively coupled plasma source for high current focused ion beam applications | |
| dc.type | Journal article | |
| local.bibliographicCitation.issue | 6 | en_AU |
| local.bibliographicCitation.lastpage | 2906 | |
| local.bibliographicCitation.startpage | 2902 | en_AU |
| local.contributor.affiliation | Smith, N.S., FEI Company, United States of America | en_AU |
| local.contributor.affiliation | Skoczylas, W.P., FEI Company, United States of America | en_AU |
| local.contributor.affiliation | Kellogg, S M, FEI Company, United States of America | en_AU |
| local.contributor.affiliation | Kinion, D.E., FEI Company, United States of America | en_AU |
| local.contributor.affiliation | Tesch, P.P., FEI Company, United States of America | en_AU |
| local.contributor.affiliation | Sutherland, Orson, College of Physical and Mathematical Sciences, CPMS Research School of Physics and Engineering, Plasma Research Laboratory, The Australian National University | en_AU |
| local.contributor.affiliation | Aanesland, Ane, College of Physical and Mathematical Sciences, CPMS Research School of Physics and Engineering, Plasma Research Laboratory, The Australian National University | en_AU |
| local.contributor.affiliation | Boswell, Roderick, College of Physical and Mathematical Sciences, CPMS Research School of Physics and Engineering, Plasma Research Laboratory, The Australian National University | en_AU |
| local.contributor.authoruid | u9708862 | en_AU |
| local.description.notes | Imported from ARIES | en_AU |
| local.identifier.absfor | 020204 | en_AU |
| local.identifier.ariespublication | u4048219xPUB4 | en_AU |
| local.identifier.citationvolume | 24 | en_AU |
| local.identifier.doi | 10.1116/1.2366617 | en_AU |
| local.identifier.scopusID | 2-s2.0-33845242768 | |
| local.publisher.url | https://www.aip.org/ | en_AU |
| local.type.status | Published Version | en_AU |
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