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28 CHAPTER 2. ATMOSPHERE AND REMOTE SENSING<br />

2.1.11 Applicability of light-emitting diodes as light sources for active<br />

DOAS measurements<br />

Holger Sihler (Christoph Kern, Ulrich Platt)<br />

Abstract The spectral stability of light-emitting diodes (LEDs) was studied in view of their applicability<br />

in Long Path Differential Optical A bsorption Spectroscopy (LP-DOAS). Beside a constant<br />

temperature also a highly accurate current source to drive the LEDs was found to be essential.<br />

intensity of LED [a.u.]<br />

10 18<br />

10 19<br />

10 20<br />

10 21<br />

400 420 440 460 480 500 520<br />

10 22<br />

540<br />

wavelength [nm]<br />

Figure 2.12: Spectral emission of a Luxeon LXHL-LR3C high power 3 W royal blue LED (at 700 mA,<br />

10 ◦ C, blue line) in comparison with the absorption cross sections of two trace gases – NO2 (Voigt<br />

2002, red line) and Glyoxal (Volkamer 2005, black line) – which have significant absoption structures<br />

in this spectral range.<br />

Background To date, high pressure xenon arc<br />

lamps have established themselves as the most<br />

common light sources for active DOAS instruments.<br />

However, these have several disadvantages<br />

including poor power efficiency in the required<br />

wavelength region and short lifetime resulting in<br />

high maintenance costs. Modern LEDs potentially<br />

represent a very advantageous alternative<br />

for both LP-DOAS [Kern et al. , 2006] and cavity<br />

enhanced absorption spectroscopy (CEAS) [Ball<br />

et al. , 2004; Langridge et al. , 2006]. Additionally<br />

LEDs are much easier to maintain considering the<br />

risk of explosions and interfering electromagnetic<br />

radiation.<br />

Methods and results As one may notice in<br />

the comparison between the emission of an LED<br />

and the trace gas absorption cross sections (Figure<br />

2.12), the LED spectrum contains some narrowband<br />

structures considered to be etalon structures.<br />

Only a slight variation of these structures<br />

during the measurement process increases<br />

the residual of a DOAS evaluation by one order of<br />

magnitude or even more in comparison to Xenon<br />

arc lamps. Stabilising their emission spectrum is<br />

therefore the key to make LEDs competitive as<br />

DOAS light-sources.<br />

The spectral position of the etalon structure<br />

depends on the chip temperature. A non-zero<br />

heat resistance between chip and heat sink yields<br />

optical density of trace gas [cm2/molecule]<br />

a dependency on both the heat sink tempearture<br />

and the dissipation of electrical energy inside the<br />

chip. In the special case of the LXHL-LR3C an<br />

already attained temperature stabilisation within<br />

0,1 K corresponds to 0,1 % of the current. Hence,<br />

a stabilisation of the LED drive current was found<br />

to be as important as controlling the temperature.<br />

A compact sealed LED housing with a peltiercooled<br />

heatsink and molecular sieve drying agent<br />

was designed to decouple the LED from the ambient<br />

temperature. Together with a standard PIDcontroller<br />

and a current source, the spectral noise<br />

of a LED could be reduced to a value lower than<br />

that of halogen lamps. The stability of an arc<br />

lamp has not been attained yet.<br />

Funding IUP<br />

Outlook/Future work Future experiments<br />

will concentrate on UV-LEDs to detect further<br />

trace gases (e.g., SO2, ClO, or CH2O). Also superluminescent<br />

LEDs (SLEDs) will be studied in<br />

respect to their applicability. The latter provide<br />

very high radiances but are only in the wavelength<br />

region above 650 nm available. Also the application<br />

of an even more precise temperature controller<br />

(TEC) is very promising. A newly customdesigned<br />

current source-TEC combination has to<br />

be tested and compared to industry standard components.

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