APS March Meeting 2011
Volume 56, Number 1
Monday–Friday, March 21–25, 2011;
Dallas, Texas
Session A16: Focus Session: Magnetic Nanostructures I
8:00 AM–11:00 AM,
Monday, March 21, 2011
Room: D173
Sponsoring
Units:
DMP GMAG
Chair: Guoxing Miao, Massachusetts Institute of Technology
Abstract ID: BAPS.2011.MAR.A16.7
Abstract: A16.00007 : Focused electron beam induced deposition of magnetic nanostructures*
9:12 AM–9:48 AM
Preview Abstract
Abstract
Author:
Jose M. De Teresa
(CSIC-University of Zaragoza (Spain))
Nanopatterning strategies of magnetic materials normally rely on
standard
techniques such as electron-beam lithography using
electron-sensitive
resists. Focused electron beam induced deposition (FEBID) is
currently being
investigated as an alternative single-step route to produce
functional
magnetic nanostructures. Thus, Co-based [1] and Fe-based [2]
precursors have
been recently investigated for the growth of magnetic
nanostructures by
FEBID. In the present contribution, I will give an overview of
the existing
literature on magnetic nanostructures by FEBID and I will focus
on the
growth of Co nanostructures by FEBID using Co$_{2}$(CO)$_{8}$ as
precursor
gas. The Co content in the nanostructures can reach 95{\%} [3].
Magnetotransport experiments indicate that full metallic
behaviour is
displayed with relatively low residual resistivity and standard
anisotropic
magnetoresistance (0.8{\%}) [3]. The coercive field of nanowires
with
changing aspect ratio has been determined in nanowires with width
down to
150 nm by means of Magneto-optical Kerr Effect [4] and the
magnetization
reversal has been imaged by means of Magnetic Force Microscopy,
Scanning
Transmission X-ray Microscopy as well as Lorentz Microscopy
experiments.
Nano-Hall probes have been grown with remarkable minimum
detectable magnetic
flux. Noticeably, it has been found that the domain-wall
propagation field
is lower than the domain-wall nucleation field in L-shaped
nanowires, with
potential applications in magnetic logic, sensing and storage
[5]. The spin
polarization of these Co nanodeposits has been determined through
Andreev-Reflection experiments in ferromagnetic-superconducting
nanocontacts
and amounts to 35{\%} [6]. Recent results obtained in Fe-based
nanostructures by FEBID using Fe$_{2}$(CO)$_{9}$ precursor will
be also
presented [7].
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[1] I. Utke et al., Appl. Phys. Lett. 80 (2002) 4792-4794
\\[0pt]
[2] M. Takeguchi et al., Nanotechnology 16 (2005) 1321-1325
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[3] A. Fern\'{a}ndez-Pacheco et al, J. Phys. D: Appl. Phys. 42
(2009) 055005
\\[0pt]
[4] A. Fern\'{a}ndez-Pacheco et al, Nanotechnology 20
(2009) 475704
\\[0pt]
[5] A. Fern\'{a}ndez-Pacheco et al, Appl. Phys. Lett. 94
(2009) 192509
\\[0pt]
[6] S. Sangiao et al, Solid State Communications, in press
\\[0pt]
[7] R. Lavrijsen et al, Nanotechnology, submitted
*I acknowledge the collaboration in this field with A. Fernandez-Pacheco, R. Cordoba, L. Serrano, S. Sangiao, L.A. Rodriguez, C. Magen, E. Snoeck, L. Morellon, M.R. Ibarra.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2011.MAR.A16.7