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Jahresbericht 2005 - IPHT Jena

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86<br />

Fig. 4.6: EFISH signal development (cf. text) at<br />

Si/SiO 2 surfaces with oxidized silicon of low<br />

(upper part) and high p-type doping (lower part).<br />

across the Si/SiO 2 interface is steadily compensated<br />

and overwhelmed by laser induced electron<br />

injection into the SiO 2 layer building up an<br />

electric field of opposite direction. In addition the<br />

SSHG method was successfully applied to detect<br />

the damage of monomolecular surface layers<br />

induced by excimer laser irradiation.<br />

Further investigations of optical materials and<br />

components in <strong>2005</strong> refer to the laser durability of<br />

fused silica (undesired microchannel formation),<br />

CaF 2 (HELD = high energy laser durability project),<br />

optical layers (impurity and defect detection)<br />

as well as the performance of optical functional<br />

elements.<br />

Combustion processes<br />

(Dirk Müller, Wolfgang Paa, Wolfgang Triebel)<br />

Laser diagnostics is applied to investigate steady<br />

state and dynamic flames up to pulse repetition<br />

rates of 1 kHz. The well-established detection of<br />

OH radicals by LIF now has – in cooperation with<br />

the Optics division – also successfully been<br />

applied to flames of industrial burners containing<br />

particles (loaded flames) and used to determine<br />

local gas temperatures. On the other hand, the LIF<br />

method is capable of characterising very small<br />

flames created by microburners which were prepared<br />

in the division for Microsystems (Fig. 4.7).<br />

The breadboard model of the advanced disk<br />

laser system (ADL) at <strong>IPHT</strong> <strong>Jena</strong> was further<br />

LASERTECHNIK / LASER TECHNOLOGY<br />

Fig. 4.7: 2D-LIF image of OH in small flame on<br />

top of microburner with 380 µm channel width.<br />

improved and tested to generate 2D-LIF images<br />

of OH in flames. This required generating the<br />

third harmonic of the ADL pulses efficiently with<br />

sufficiently high pulse energy. Furthermore, some<br />

preliminary work has been performed towards<br />

fast wavelength switching of the ADL system<br />

using the available tuning components at the high<br />

laser pulse repetition rate.<br />

Moreover the ADL-FT (Fallturm) system was tested<br />

in several drops with maximum deceleration of<br />

about 35 g in polystyrene granulate: Evidently the<br />

laser system survives these procedures. Convection,<br />

however, is still present in front of the laser<br />

disk and changes when microgravity conditions<br />

start. These changes are small but sufficient to<br />

influence the laser operation so that some revisions<br />

of the laser system and operation are required.<br />

4.3 Appendix<br />

Partners (in alphabetical sequence)<br />

in <strong>Jena</strong> and Thuringia:<br />

• CiS Institut für Mikrosensorik, Erfurt<br />

• Ersol Solar Energy AG, Erfurt<br />

• Fachhochschule (University of Applied Sciences)<br />

<strong>Jena</strong><br />

• Fraunhofer-Institut für Angewandte Optik und<br />

Feinmechanik (IOF), <strong>Jena</strong><br />

• Friedrich-Schiller-Universität, <strong>Jena</strong><br />

Institut für Festkörperphysik und Astrophysikalisches<br />

Labor<br />

• Institut für Fügetechnik und Werkstoffprüfung<br />

(IFW), <strong>Jena</strong><br />

• ITP GmbH, Weimar<br />

• Jenoptik Laser.Optik.Systeme GmbH, <strong>Jena</strong><br />

• Jenoptik Laserdiode GmbH, <strong>Jena</strong><br />

• Layertec GmbH, Mellingen<br />

• LLT Applikation GmbH, Ilmenau<br />

• MWS Schneidwerkzeuge GmbH&Co. KG,<br />

Schmalkalden

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