Sub-100 nanometer
Ion Beam Probe for Applications in Biology and Many Other
Disciplines+
S. K. Guharay1,
V. Jabotinski1, J. Orloff2
1FM
Technologies, Inc., 4431-H Brookfield Corporate Dr., Chantilly, VA
20151
2Institute
for Research in Electronics and Applied Physics, University of
Maryland, College Park, MD 20742.
e-mail: sguharay@fm-technologies.com
Focused
ion beams (FIB), at sub-100 nanometer scale, have utility for a wide
range of applications in both basic and applied science covering
geology, materials science, microelectronics and biology. An example
of current interests is imaging by FIB-SIMS (Secondary Ion Mass
Spectrometry). In biology and medicine its utility is recognized
[1-2] due to the relevance of SIMS to study fundamental problems,
for example mapping distributions of targeted chemical species in
tissues. The critical role of ion beams is realized in ion beam
milling and diagnostics instruments including in-line inspection of
semiconductor devices for defect management.
While
significant progress has been made to design an efficient
ion-optical column, the critical issues to achieve a high-resolution
ion beam probe with target beam intensity of about 1 A/cm2
are governed by beam characteristics from the ion source, namely,
virtual source size, beam brightness, and energy spread. An acute
need prevails to advance the state-of-the art of sources so that
desirable beam characteristics for a variety of beam species,
especially, for hydrogen, oxygen, argon, and many complex molecular
ions, can be achieved.
This
article especially focuses on developing high-brightness negative
ion beams and coupling the beams to an ion-optical column. The goal
is to achieve a sub-100 nm ion beam probe. Negative ions have unique
merits for applications involving beam-materials interactions. When
negative ions strike a surface, especially an electrically isolated
surface, the surface charging voltage does not exceed a few volts,
and the charging voltage is independent of the beam energy [3].
Figure 1 shows an example of the charging voltage of an isolated
alumina surface due to irradiation by H- beams [4]. This
property can be effectively utilized to circumvent problems due to
surface charging that can cause device or sample damage and ion-beam
defocusing.
A
compact plasma source, with the capability to produce negative as
well as positive ion beams, is developed. Intense ion beams,
including H-, O- and Ar+, have been generated.
The unnormalized beam brightness for 10 keV H- beams is
~105Acm-2sr-1[5]. Figure 2 shows an
example of H-
beam spot when the beam is focused using a simple einzel lens with
magnification of about 0.1. This spot size of about 2 µm
suggests that a focused spot size of about 20 nm is achievable by an
additional magnification of 0.01. The results of ion-optical
calculations, in Fig. 3, for a three-lens column show the required
beam focusing for sub-100 nm spot size[4]. Experiments on
measurements of beam characteristics, design and development of
ion-optical column and application goals will be discussed.
+Supported
by SBIR Grant from National Cancer Institute, National Institute of
Health.
[1]
P. J. Todd, T. G. Schaaff, P. Chaurand, R. M.
Caprioli, J. Mass. Spectrom. 36, 355(2001).
[2]
S. Chandra and D. R. Lorey, Cell. Mol. Biol. 47,
503 (2001).
[3]
P. N. Guzdar, A. S. Sharma, S. K. Guharay, “Charging
of substrates irradiated by particle beams” Appl. Phys. Lett. 71,
3302 (1997).
[4]
S. K. Guharay, S. Douglass and J. Orloff, “High
resolution primary ion beam probe for SIMS”, Applied Surface Science
231-232, 926 (2004).
[5]
S. K. Guharay, E. Sokolovsky, J. Orloff,
“Characteristics of ion beams from a Penning source for focused ion
beam applications” J. Vac. Sci Technol. B17, 2779 (1999).
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