27.12.2013 Views

PhD Thesis_RuiMSMartins.pdf - RUN UNL

PhD Thesis_RuiMSMartins.pdf - RUN UNL

PhD Thesis_RuiMSMartins.pdf - RUN UNL

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

In-situ XRD studies during growth of Ni-Ti SMA films and their complementary ex-situ characterization<br />

(a)<br />

(b)<br />

Fig. 2.4: Six-circle diffractometer in the MRH of ROBL; (a) view of the χ-circle (Eulerian<br />

cradle with inner diameter of 400 mm) with the x-y-z slide mounted directly on the<br />

azimuthal ϕ-circle (front view: detector side), (b) scheme of the diffractometer with<br />

identification of the axes (view from back: beam direction).<br />

In order to follow in situ the film growth and post-deposition annealing, Matz et al.<br />

[58] have designed a sputtering chamber that fits into the Huber six-circle diffractometer.<br />

Since the diffractometer is used as a multi-purpose instrument for many other experiments,<br />

the chamber has to be removed always after the beamtimes dedicated to this type of studies.<br />

During the period of this thesis work, a new chamber was built by Schell et al. [156] and was<br />

also tested and used in the deposition of the Ni-Ti films. The results were reproducible with<br />

both chambers and the main advantage of the new chamber for this work are the enlarged<br />

windows allowing the study of a higher number of Bragg peaks of the phases present in the<br />

sample. The “old” set-up (equipped with Kapton-capped flanges as X-ray entrance and exit<br />

windows) and the “new” set-up (sealed with Be foils) are described below.<br />

The chambers have been designed to be mounted on the ϕ-circle and limited in weight<br />

to 15 kg in order to guarantee the high precision of the goniometer settings of 0.001°. The<br />

other geometrical limitation results from the χ-circle perpendicular to the ϕ-circle. The χ-<br />

circle has an inner diameter of 400 mm but is located 85 mm off-centre of the ϕ-circle.<br />

Taking those limitations into account one can use all existing instalments/equipment at the<br />

diffractometer like detectors, slits, collimators, and filter units without additional<br />

modifications. The Eulerian cradle is fitted to the θ circle and with an identical rotation axis<br />

Chapter 2 – Experimental Details 81

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!