Photoluminescence Spectroscopy of Doped and Undoped BaTiO3

R. A. Mullen, K. L. Schumacher, B. Wechsler, M. Klein
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Abstract

Despite the many important potential applications for photorefractive BaTiO31, the precise nature and the depth of the photorefractive trapping centers has yet to be positively identified. In one study2, a correlation was noted between the iron concentration as measured with EPR, the photorefractive trap density determined by two-beam coupling versus grating wavevector measurements, and the optical absorption coefficient. This tentatively identified iron as the photorefractive center in commercially-grown, nominally undoped crystals. More recently, high photorefractive gains were reported in nominally iron-free BaTiO3 crystals3, and evidence was presented3,4 that, in purposely iron-doped crystals, the most common valence states for iron are Fe+3 and Fe+4.
掺杂和未掺杂BaTiO3的光致发光光谱
尽管光折变BaTiO31有许多重要的潜在应用,但光折变俘获中心的精确性质和深度尚未得到明确确定。在一项研究中,发现了EPR测量的铁浓度、双光束耦合测定的光折变阱密度与光栅波矢量测量的光吸收系数之间的相关性。这初步确定了铁作为商业生长的光折变中心,名义上不掺杂晶体。最近,在名义上不含铁的BaTiO3晶体中报道了高光折变增益,并且有证据表明,在故意掺杂铁的晶体中,铁最常见的价态是Fe+3和Fe+4。
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