{"title":"空间振荡光伏电流诱导铁电体的动态全息效应","authors":"B. Sturman","doi":"10.1364/JOSAB.8.001333","DOIUrl":null,"url":null,"abstract":"It’s well known that the main mechanisms of holographic grating formation in photorefractive crystals are the diffusion of carriers, their drift in the electric field, and the photovoltaic effect (PVE). We shall concentrate on the last mechanism. It’s often supposed that the PVE in ferroelectrics can be characterized by the current along the polar \nc→-axis, j=α G I, where α is the absorption coefficient, G: the Glass coefficient, I: the light intensity. In this case, the PVE effect is analogous to the effect of supplementary electric field E\n ph\n =j(σ\n d\n +σ\n ph\n )−\n 1\n , where σ\n d\n , σ\n ph\n are dark- and photoconductivity. The photoinduced field E\n ph\n reaohes 10\n 5\n v/cm in LiNbO3 and LiTaO3. However, the effect of the PVE does not come to longitudinal current.","PeriodicalId":385625,"journal":{"name":"Topical Meeting on Photorefractive Materials, Effects, and Devices II","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"1991-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"11","resultStr":"{\"title\":\"Dynamic Holography Effects in Ferroelectrics Induced by Spatially-Oscillating Photovoltaic Currents\",\"authors\":\"B. Sturman\",\"doi\":\"10.1364/JOSAB.8.001333\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"It’s well known that the main mechanisms of holographic grating formation in photorefractive crystals are the diffusion of carriers, their drift in the electric field, and the photovoltaic effect (PVE). We shall concentrate on the last mechanism. It’s often supposed that the PVE in ferroelectrics can be characterized by the current along the polar \\nc→-axis, j=α G I, where α is the absorption coefficient, G: the Glass coefficient, I: the light intensity. In this case, the PVE effect is analogous to the effect of supplementary electric field E\\n ph\\n =j(σ\\n d\\n +σ\\n ph\\n )−\\n 1\\n , where σ\\n d\\n , σ\\n ph\\n are dark- and photoconductivity. The photoinduced field E\\n ph\\n reaohes 10\\n 5\\n v/cm in LiNbO3 and LiTaO3. However, the effect of the PVE does not come to longitudinal current.\",\"PeriodicalId\":385625,\"journal\":{\"name\":\"Topical Meeting on Photorefractive Materials, Effects, and Devices II\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1991-06-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"11\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Topical Meeting on Photorefractive Materials, Effects, and Devices II\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1364/JOSAB.8.001333\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Topical Meeting on Photorefractive Materials, Effects, and Devices II","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/JOSAB.8.001333","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 11
摘要
众所周知,光折变晶体中全息光栅形成的主要机制是载流子的扩散、在电场中的漂移和光伏效应(PVE)。我们将集中讨论最后一种机制。通常认为铁电体的PVE可以用沿极性c→-轴的电流来表示,j=α G I,其中α为吸收系数,G为玻璃系数,I为光强。在这种情况下,PVE效应类似于补充电场E ph =j(σ d +σ ph)−1的效应,其中σ d和光电导率分别为暗电导率和光电导率。在LiNbO3和LiTaO3中,光致场eph达到了10.5 v/cm。然而,PVE的影响并不体现在纵向电流上。
Dynamic Holography Effects in Ferroelectrics Induced by Spatially-Oscillating Photovoltaic Currents
It’s well known that the main mechanisms of holographic grating formation in photorefractive crystals are the diffusion of carriers, their drift in the electric field, and the photovoltaic effect (PVE). We shall concentrate on the last mechanism. It’s often supposed that the PVE in ferroelectrics can be characterized by the current along the polar
c→-axis, j=α G I, where α is the absorption coefficient, G: the Glass coefficient, I: the light intensity. In this case, the PVE effect is analogous to the effect of supplementary electric field E
ph
=j(σ
d
+σ
ph
)−
1
, where σ
d
, σ
ph
are dark- and photoconductivity. The photoinduced field E
ph
reaohes 10
5
v/cm in LiNbO3 and LiTaO3. However, the effect of the PVE does not come to longitudinal current.