Letter to the Editor
Surface morphology of silica nanowires at the nanometer scale
Cornelia Rodenburg
a
, Xiong Liu
b
, Mark A.E. Jepson
c
, Stuart A. Boden
d
, Gilberto Brambilla
e,
⁎
a
Department of Engineering Materials, University of Sheffield, Mappin Street S1 3JD, UK
b
Carl Zeiss NTS, Carl-Zeiss-Straße 56 73447, Oberkochen Germany
c
Department of Materials, Loughborough University, Loughborough LE11 3TU, UK
d
Electronics and Computer Science, University of Southampton, Southampton SO17 1BJ, UK
e
Optoelectronics Research Centre, University of Southampton, Southampton SO17 1BJ, UK
article info
Article history:
Received 12 November 2010
Received in revised form 8 March 2011
Available online 12 April 2011
Keywords:
Surface;
Silica;
Defects;
Optical fiber
Introduction
Surface quality has been recognized to be a fundamental limitation
to mechanical strength and optical transmission, particularly for sub-
micrometric structures.
Mechanical properties of nanowires are known to improve
significantly for decreasing diameters [1–9]. Materials with high
specific ultimate strength σ
ρ
(ratio between strength and density) are
highly desirable because they could have radical implications in
extreme engineering applications like aerospace structural materials,
wind turbines, powerboats, suspended bridges or even more futuristic
applications like the space elevator. The presence of defects degrades
the overall σ
ρ
: a single missing atom in an otherwise perfect CNT
would decrease its tensile strength by 20% [10]. This is a major
drawback since the great majority of nanostructures is crystalline and
can be fabricated flawlessly only for few millimeters. In contrast, a
silica glass does not have any long-distance atomic periodicity, thus it
can accommodate sub-nanometer defects, preserving a relatively high
σ
ρ
. Silica nanowires with diameters smaller than 50 nm and surface
smoothness at the atomic value have been manufactured [11] from
optical fibers. Yet, the strength of silica nanowires is affected by
abrupt changes in diameter and surface uniformity over a long range
is the single most crucial factor in their performance.
For optical applications, photonic bandgap fibers (PBGFs) have
been proposed as the means to reach the ultimate low loss [12] and to
change radically data transmission over long distances. While the
minimum transmission loss (~0.15 dB km
-1
) observed so far in
conventional fibers [13] is determined by fundamental scattering and
absorption processes in silica, in PBGFs over 99% of the light can
propagate in air [12] and avoid these loss mechanisms. Optimized
silica PBGFs could have a transmission loss as little as 0.03 dB km
-1
[12] if the only surface roughness were of intrinsic nature [14] and
came from ripplons (surface capillary waves). Optimized PBGFs
would have a hollow core bordered by very thin silica strands with
thickness of the order of ~ 100 nm, the surface quality of which will be
the single most important factor to minimize the transmission loss.
In this manuscript we analyze the surface morphology of silica
nanowires with unprecedented resolution and discuss the origin of
defects which can be as large as 20 nm.
Nanowires used in these experiments were manufactured from
commercial optical fibers by the “microheater brushing technique”,a
top–down technique originally developed to manufacture nanowires
from glasses with low processing temperature [15]. A commercial
telecom optical fiber (SMF-1300/1550-9/125-0.25-10641, manufac-
tured from Oz Optics), was held by two clamps mounted on
translational stages (WSX-300 provided by Rockwell Automation)
and heated by a ceramic microheater (manufactured by NTT-AT) with
a bore 20 mm long and 2 mm wide (Fig. 1a) in air. The fiber was pulled
Journal of Non-Crystalline Solids 357 (2011) 3042–3045
⁎ Corresponding author. Tel.: + 44 23 8059 3588; fax: + 44 23 8059 3149.
E-mail address: gb2@orc.soton.ac.uk (G. Brambilla).
LETTER TO THE EDITOR
0022-3093/$ – see front matter © 2011 Elsevier B.V. All rights reserved.
doi:10.1016/j.jnoncrysol.2011.03.005
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