2000
DOI: 10.1134/1.1309459
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Periodic domain structure in Czochralski-grown LiNbO3: Y crystals

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Cited by 10 publications
(4 citation statements)
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“…admixture has been studied in rotational growth figures of LiNbO 3 :Y single crystals [11]. By measuring distribution of the admixture along the normal of domain boundaries it was found that domains are formed near yttrium concentration maximums and minimums.…”
Section: Resultsmentioning
confidence: 99%
“…admixture has been studied in rotational growth figures of LiNbO 3 :Y single crystals [11]. By measuring distribution of the admixture along the normal of domain boundaries it was found that domains are formed near yttrium concentration maximums and minimums.…”
Section: Resultsmentioning
confidence: 99%
“…The ferroelectric domain structure of period ⌳ Ϸ 24 m is a result of rotation-induced striations and Y doping ͑1 wt % Y 2 O 3 in the melt͒. 5 A single-domain sample of Y-doped LiNbO 3 ͑1 wt % Y 2 O 3 in the melt, grown by Polgár͒ and a nominally undoped LiNbO 3 wafer ͑c Fe Ͻ 5 ppm, purchased from Crystal Technology, Inc.͒ served for reference. All crystals were thermally reduced by vacuum annealing ͑p Ͻ 10 −4 mbar͒ at elevated temperatures for a duration of 6 h. Hence, the properties of small bound Nb Li 4+ polarons ͑ abs = 760 nm, 1.6 eV͒, Nb Li 4+ :Nb Nb 4+ bipolarons and O − hole polarons ͑both at 500 nm, 2.5 eV͒ ͑Refs.…”
Section: Methodsmentioning
confidence: 99%
“…These methods enable to create domain structures with the periods down to 2 µm, but they fail to yield bulk (more than 2 mm thick) elements with precise RDS. The samples with RDS of enlarged thickness can be produced using rotational growth striations obtained in the crystals doped by rare-earth elements [5][6][7][8][9][10]. The impurities Y 3+ , Nd 3+ , Hf 3+ [11], Dy 3+ , Gd 3+ have a big ionic radius, an uncompensated charge, and value of effective distribution coefficient less than unity.…”
Section: Introductionmentioning
confidence: 99%