EFONGA
- European Forum on New Glass Applications
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Introduction to Glasses for Optoelectronics
Current developments in
optoelectronics and photonics need materials and devices with increasing optical
functionality and more and more complexity. Novel or advanced glasses can
respond to these demands: application areas range from special coatings for
optical components (including transparent conductive or electrochromic films) to
optical telecommunications, from displays to optical
storage, and to biomedical and sensing. In
the optical communications area, the extension of optical functionality
within networks, that are already optical, and the implementation of optics at
lower levels, particularly the access network, have been major goals in recent
years. Both these development areas will impose new requirements for optical
components, demands for which a number of different technologies are already
competing. Implementation of all-optical functionality (e.g. all-optical
switching) by exploiting nonlinear properties of special glasses and low-cost
manufacturing are two key objectives. A specific attention is being devoted to
glasses for waveguides,
optical amplifiers and lasers In
the wider optoelectronics area, researches on flat panel displays and on
luminescent materials that may be efficiently excited by low-cost light sources,
such as LEDs, constitute a main concern. In
this scenario, composite and nanostructured glasses have great relevance.
For instance, there is an increasing interest in the development of
nanostructured materials for innovative photonic devices. Since the discovery of
the quantum size effect in semiconductor nanoparticles, academic and
professional researchers have been interested in the potential applications of
similar effects in metallic nanoparticles. Noble-metal elements are particularly
attractive in such an area, due to the well-known surface plasmon resonance,
which originates from a confinement effect on the electronic properties in metal
systems of finite size. This phenomenon corresponds to the collective excitation
of the free electrons, classically described as the oscillation of the
electronic cloud with respect to the ionic background of the nanoparticle, and
results in a potentially large local field enhancement around the excited
nanoparticle. It has to be noted that, in addition to the optical applications,
metal nanocluster composite glasses synthesised with transition elements are
important for their magnetic properties as well. Hybrid
materials, where inorganic glasses may be mixed, for instance, with organic
materials or with inorganic crystalline materials, may well exhibit peculiar
properties and/or extended functionality. Their study will extend further the
range of optical properties available. Laser
micro-machining and nano-structuring of glasses
by interaction with high
power ultra-short pulse lasers are also attracting much attention. Femtosecond
laser writing of optical structures and self-organised nano-gratings formation
probably due to laser-induced birefringence are two examples of new phenomena,
which can be exploited for integrated optics and information storage,
respectively. Finally,
the possibility of implementing periodic structures in glasses acting as
photonic crystals (that has already been very successfully demonstrated in
optical fibres) by using low-cost processes will be another matter of
investigation in the next few years. Optical
fibres
are now almost universally used in telecommunication systems for
point-to-point high bandwidth links. The more recent developments of fibre
communication systems often rely on the availability of integrated optical
circuits, namely of devices involving waveguides on planar substrates. Related
manufacturing technologies include CVD, flame-hydrolysis, RF-sputtering and
sol-gel deposition processes, or diffusion, ion-exchange and ion-implantation
processes. Direct
uv-laser or fs-pulse laser writing is now challenging conventional
photolithographic patterning of the circuits. A
key requirement of materials and integrated optical components is that they must
be optimised for 1.55 mm
operation, because this is the wavelength of minimum attenuation in silica
fibres and is currently the standard operational wavelength of most telecom
systems. In future, however, other wavelengths, in combination with non-silicate
fibres and planar waveguides, may gain a foothold. Erbium-doped fibre amplifiers are now the commercially available choice for optical amplification in telecom systems operating near 1.55 mm, using laser diode pumping at 980 nm or 1480 nm. The use of integrated optical amplifiers, on the other hand, permits significant savings in space occupied and the integration of other optical components such as switches, splitters, and wavelength-division-multiplexers together with the amplifier on the same glass chip, with minimal losses. The shorter interaction length, however, requires higher erbium doping levels to achieve an acceptable gain, with the disadvantage of increased ion-to-ion interactions. Materials issues to be addressed include the reduction of multiphonon quenching of the lasing excited-state lifetime, the minimising of the effects of amplified spontaneous emission and of up-conversion processes, and therefore the identification of optimal glass matrices and the corresponding optimal rare-earth doping concentration. In
the area of glass optical amplifiers the key goals are: -
To achieve a broader emission band, that could
allow the system designers to fully exploit wavelength division multiplexing in
order to increase the transmission capacity, and a higher net optical gain. -
Similar considerations apply to the
identification of the most appropriate matrix-dopant combination for the
manufacturing of integrated optical Er:glass lasers. -
Having in mind future developments towards
longer wavelength bands, non-oxide glass matrices and rare earth elements other
than erbium will also be carefully investigated.
References to the optical glasses which are commercially available and to their specifications are provided in the data page. |
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© EFONGA gcr 2006Website established on 31-01-2006; updated on 10-01-07. |