Congruent SBN and BCT crystals doped with Fe, Cr, Ce to enhance photorerractive properties. are investigated at low temperature (T> I K) under illumination with Art-and Kr+ -laser light. Light-induced absorption changes in a wide spectral range from UV to IR indicate photoinduced charge transfer processes from impurities to polaronic centers. Broad NIR absorptions (at about 0,7 eV) associated with Ti 1 + polarons in BCT or with Nb 4 + polarons in SBN are observed and their non-linear behaviour with illumination intensity, polarization and temperature is described on the basis of the simple model for the photo charge transport (in SBN: Ce-'+ + NbH-Ce 4 + + Nb4+). A broad visible absorption VIS (at about 2 eV) appearing together with the NIR polarons, is shown by photodissociation (with a Kr+ -laser) to consist at least partly of small polarons (in BCT and SBN).
INTRODUCTIONBoth promising photorefractive crystal systems Ba 1 _rCa rTi03 and Sr:,Ba J-xNb206 possess a congruently melting mixture (for SBN x=0,61 and for BCTy=0.23), where melt and crystal have the same composition [I, 2]. This allows to grow large, homogeneous crystals of excellent optical quality, which is the basis for a wide range of optical applications [3]. Further favourable features of these crystals are the lack of a destructive phase transition (in contrast for instance to BaTi0 3 ) and the ease of poling of the crystals into a monodomain state [I]. Due to the statistical distribution of the constituents and a partially unfilled (tungsten bronze) structure for SBN, the ferroelectric phase transition (Tc ~ 373 K for congruent BCT pure and Tc ~ 353 K for congruent SBN pure) shows a relaxor type character with polar contributions well above Tc· The addition of doping ions (like Fe, Ce, Cr) in most cases shifts Tc toward lower temperatures with increasing doping content (for instance from 353 K in SBN pure to about room temperature for dopings of 20 000 ppm, p. f.u., Ce or Cr [ 4]. The electro-optical coefficients of the pure crystals are already large and can be enhanced considerably by suitable doping with polyvalent ions like those mentioned above [5, 6]. For some of the dopants (like Ce and Cr in SBN) a majority charge state 3 + has been determined [7, 8], however with an individual site occupancy, Ce3+ replacing Sr+ ions and C~+ sitting on the Nb 5 + sites [9, 10]. These dopants can be identified by their broad impurity induced absorption bands in the visible range, a shift of the UV-absorption edge to longer wavelength in the case of Cr doping and additional Far-IR bands (near 2000 em -I) in the case ofCe-doping [7]. A light-induced charge transport from these doping ions and trapping in shallow polaronic states (Ti3+ in BCT respectively Nb 4 + in SBN) has been identified by photo-EPR [11] and optical experiments [12] to constitute the underlying processes for the enhanced photorefractive properties in doped crystals. The majority of photo-excited charge carriers has been determined by laser beam coupling experiments [13] and Hall -effect [14...