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Photonics Driving Economic Growth in Europe - Photonics21

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2. <strong>Photonics</strong> Research and Innovation Challenges<br />

EIR sources<br />

As a consequence of the low concentration of<br />

many critical analytes, there is a huge need of cost-<br />

effective, narrow-band, medium-power (1–100<br />

mW) light sources, allow<strong>in</strong>g the measurement<br />

process to be done quickly and with the required<br />

resolution. Of particular <strong>in</strong>terest are solid-state<br />

lasers, such as QCLs (Quantum Cascade Lasers),<br />

VECSELs (Vertical External Cavity Surface Emitt<strong>in</strong>g<br />

Lasers), VCSELs (Vertical Cavity Surface Emitt<strong>in</strong>g<br />

Lasers), and fibre lasers. S<strong>in</strong>ce many technologies<br />

utilise electronic lock-<strong>in</strong> methods, it must be possible<br />

to modulate the lasers electrically. For stable,<br />

efficient operation <strong>in</strong> the MIR/FIR, the lasers must<br />

be cooled and temperature-controlled, and care<br />

must be taken that these cool<strong>in</strong>g requirements<br />

do not dom<strong>in</strong>ate the production cost of the complete<br />

laser sub-system. For low-cost laser systems,<br />

electrical emission wavelength tun<strong>in</strong>g capability is<br />

desirable, with tun<strong>in</strong>g ranges of several 10 nm or<br />

up to a few 100 nm.<br />

A specific goal is the development of a family of tunable<br />

EIR light emitters. Complete laser system costs,<br />

<strong>in</strong>clud<strong>in</strong>g cool<strong>in</strong>g, modulation control, and electrical<br />

power supply, should reduce to a few €100.<br />

Additionally, NIR/MIR light-emitt<strong>in</strong>g diodes (LEDs)<br />

may be of <strong>in</strong>terest as an alternative source <strong>in</strong><br />

sens<strong>in</strong>g systems that do not require narrow-band<br />

illum<strong>in</strong>ation. New and more powerful sources for<br />

wide-band IR spectroscopy are also needed, such<br />

as those based on fibre supercont<strong>in</strong>uum effects,<br />

offer<strong>in</strong>g convenient coupl<strong>in</strong>g to optical fibres. Here<br />

the goal is the development of NIR/MIR broadband<br />

light sources offer<strong>in</strong>g emission powers ≥1 mW,<br />

with ≤ €1 cost <strong>in</strong> large volumes.<br />

EIR photodetectors (0D, 1D, 2D)<br />

A large number of materials and detector types<br />

are currently employed for po<strong>in</strong>t, l<strong>in</strong>ear and<br />

image sensor devices for the NIR/MIR spectral<br />

range, <strong>in</strong>clud<strong>in</strong>g pyroelectric detectors, thermo-<br />

piles, microbolometers, narrow-bandgap photo-<br />

voltaic detectors, Schottky barrier detectors, ex-<br />

tr<strong>in</strong>sic photoconductors, multi-quantum-well semi-<br />

conductor heterostructures for QCDs and homo/<br />

heterojunction <strong>in</strong>ternal photoemitters (HIP). The<br />

challenge is to detect as many <strong>in</strong>com<strong>in</strong>g photons as<br />

possible, while reduc<strong>in</strong>g the effects of dark current.<br />

This corresponds to the primary task of maximis-<br />

<strong>in</strong>g the sensor’s detectivity, which is equivalent<br />

to m<strong>in</strong>imis<strong>in</strong>g its noise equivalent power. At the<br />

same time, material and packag<strong>in</strong>g costs must be<br />

reduced to <strong>in</strong>creas<strong>in</strong>gly lower values, and cool<strong>in</strong>g<br />

requirements kept to a m<strong>in</strong>imum.<br />

The primary goal is to develop novel types of highly<br />

cost-effective solid-state NIR/MIR sensors, based<br />

on new or optimised material systems, and ideally<br />

produced us<strong>in</strong>g well-established microelectronic<br />

fabrication techniques. It must be straightforward<br />

to produce these sensors as po<strong>in</strong>t detectors, l<strong>in</strong>e<br />

sensors or image sensors, and they must have a<br />

performance close to the ideal detector limit. Po<strong>in</strong>t<br />

detectors should cost no more than €10, whilst<br />

l<strong>in</strong>e or image sensors should cost less than €100,<br />

<strong>in</strong>clud<strong>in</strong>g the cool<strong>in</strong>g devices.<br />

CMOS-based s<strong>in</strong>gle-photon NIR image sens<strong>in</strong>g<br />

It has been demonstrated recently that novel<br />

types of CMOS-based image sensors are capable<br />

of detect<strong>in</strong>g <strong>in</strong>dividual <strong>in</strong>cident photons at room<br />

temperature. Accept<strong>in</strong>g the need for cool<strong>in</strong>g, it<br />

should also be physically possible to extend the<br />

cut-off wavelength from silicon’s 1.1 µm to higher<br />

values <strong>in</strong> the NIR, while still be<strong>in</strong>g sensitive to each<br />

<strong>in</strong>cident photon. This requires scientific progress<br />

<strong>in</strong> two doma<strong>in</strong>s. Firstly, novel CMOS-based charge<br />

detection circuits with sub-electron readout noise<br />

performance are needed. Secondly, it will be necessary<br />

to comb<strong>in</strong>e these charge detector circuits with<br />

semiconduct<strong>in</strong>g materials exhibit<strong>in</strong>g a cut-off wavelength<br />

above silicon’s 1.1 µm. Promis<strong>in</strong>g candidates<br />

<strong>in</strong>clude nanostructured (black) silicon, <strong>in</strong>organic<br />

narrow-bandgap crystall<strong>in</strong>e semiconductors (such<br />

as InGaAs), or novel types of organic semiconductors<br />

sensitive <strong>in</strong> the NIR spectral doma<strong>in</strong>.<br />

63

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