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Defects in inorganic photorefractive materials and their investigations

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<strong>Defects</strong> <strong>in</strong> <strong>in</strong>organic <strong>photorefractive</strong> <strong>materials</strong> <strong>and</strong> <strong>their</strong> <strong>in</strong>vestigations 25<br />

Analogous MCD-ODMR studies have been performed with KTaO 3 :Ni [142].<br />

Three low symmetry defects <strong>in</strong> various charge states were found.<br />

6 <strong>Defects</strong> <strong>in</strong> the sillenites Bi 12 MO 20<br />

(BMO, M = Si, Ge, Ti)<br />

In <strong>their</strong> review article, Arizmendi et al. [144] drew attention to the lack of<br />

knowledge concern<strong>in</strong>g the nature <strong>and</strong> role of defects <strong>in</strong> these <strong>materials</strong>. The<br />

situation has been clarified to a large extent, new spectroscopic evidence be<strong>in</strong>g<br />

the ma<strong>in</strong> object of this Section.<br />

6.1 Intr<strong>in</strong>sic defects <strong>in</strong> undoped crystals<br />

Fig. 11. Upper part (arbitrary<br />

ord<strong>in</strong>ate scale):<br />

Bleached state absorption<br />

of BGO at 80 K (dashed l<strong>in</strong>e)<br />

<strong>and</strong> additional absorption<br />

(10.7 cm −1 at maximum)<br />

<strong>in</strong>duced by an illum<strong>in</strong>ation<br />

with blue light (solid grey<br />

l<strong>in</strong>e). Lower parts: CD <strong>and</strong><br />

MCD spectra (1.4 K) <strong>in</strong> the<br />

bleached state (dotted l<strong>in</strong>es)<br />

<strong>and</strong><strong>in</strong>thecoloredstate(solid<br />

l<strong>in</strong>es).<br />

The most precise <strong>in</strong>formation has been obta<strong>in</strong>ed by comb<strong>in</strong>ed optical<br />

absorption, MCD <strong>and</strong> ODMR studies, performed with thermally bleached<br />

(e.g., 1/2 hour at 500 ◦ C) as well as optically colored crystals <strong>in</strong> Paris<br />

[145, 146, 147, 148, 149, 150] <strong>and</strong> <strong>in</strong> Osnabrück [149, 151]. Several important<br />

conclusions are summarized <strong>in</strong> Ref. [152] <strong>and</strong> <strong>in</strong> a forthcom<strong>in</strong>g article<br />

[153]. As illustrated <strong>in</strong> the central part of Fig. 11 for BGO as an example,<br />

an undoped <strong>and</strong> thermally bleached BMO sample does not exhibit any MCD<br />

signal <strong>in</strong> the near-IR to UV spectral range. This means that the ’shoulder’ observed<br />

near 3 eV <strong>in</strong> the correspond<strong>in</strong>g absorption spectrum (top of Fig. 11) is<br />

necessarily correlated with a diamagnetic defect. The ’shoulder’ has obviously<br />

a counterpart <strong>in</strong> the natural circular dichroism spectrum (CD, ’0’ <strong>in</strong> Fig. 11)<br />

with a m<strong>in</strong>imum at the same energy. Illum<strong>in</strong>at<strong>in</strong>g the bleached BMO crystal<br />

with light energies ly<strong>in</strong>g with<strong>in</strong> the range of this CD b<strong>and</strong>, causes a slight decrease<br />

of its amplitude. Simultaneously <strong>in</strong>tense additional absorption (b<strong>and</strong>s

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