Threshold conditions for bulk second-order nonlinearity and near-surface second-order nonlinearity in thermally poled infrasil silica

Mingxin Qiu, Toru Mizunami, Teruo Shimomura, Michitaka Ohtaki

    研究成果: ジャーナルへの寄稿記事

    4 引用 (Scopus)

    抄録

    Generation of bulk second-order nonlinearity in silica glass requires higher poling temperature or longer poling time than that of near-surface second-order nonlinearity. The threshold conditions for initiating the bulk second-order nonlinearity are studied on Infrasil fused silica glass. The threshold poling time is strongly dependent on the poling temperature. The near-surface second-order nonlinearity is also studied, especially the dependence of thickness of the nonlinear layer on the poling temperature, poling voltage and poling time. Secondary-ion mass-spectroscopy measurement showed depletion of Na+ ions at the anodic surface. We assume there is an ionic wave during poling traveling from the anodic surface to generate the dipolar electric field that induces the near-surface second-order nonlinearity.

    元の言語英語
    ページ(範囲)159-162
    ページ数4
    ジャーナルOptical Review
    8
    発行部数3
    DOI
    出版物ステータス出版済み - 1 1 2001

    Fingerprint

    nonlinearity
    silicon dioxide
    thresholds
    silica glass
    ionic waves
    ions
    depletion
    mass spectroscopy
    temperature
    electric fields
    electric potential

    All Science Journal Classification (ASJC) codes

    • Atomic and Molecular Physics, and Optics

    これを引用

    Threshold conditions for bulk second-order nonlinearity and near-surface second-order nonlinearity in thermally poled infrasil silica. / Qiu, Mingxin; Mizunami, Toru; Shimomura, Teruo; Ohtaki, Michitaka.

    :: Optical Review, 巻 8, 番号 3, 01.01.2001, p. 159-162.

    研究成果: ジャーナルへの寄稿記事

    @article{9a77300b2f4a452dbcc17046cb2d4602,
    title = "Threshold conditions for bulk second-order nonlinearity and near-surface second-order nonlinearity in thermally poled infrasil silica",
    abstract = "Generation of bulk second-order nonlinearity in silica glass requires higher poling temperature or longer poling time than that of near-surface second-order nonlinearity. The threshold conditions for initiating the bulk second-order nonlinearity are studied on Infrasil fused silica glass. The threshold poling time is strongly dependent on the poling temperature. The near-surface second-order nonlinearity is also studied, especially the dependence of thickness of the nonlinear layer on the poling temperature, poling voltage and poling time. Secondary-ion mass-spectroscopy measurement showed depletion of Na+ ions at the anodic surface. We assume there is an ionic wave during poling traveling from the anodic surface to generate the dipolar electric field that induces the near-surface second-order nonlinearity.",
    author = "Mingxin Qiu and Toru Mizunami and Teruo Shimomura and Michitaka Ohtaki",
    year = "2001",
    month = "1",
    day = "1",
    doi = "10.1007/s10043-001-0159-5",
    language = "English",
    volume = "8",
    pages = "159--162",
    journal = "Optical Review",
    issn = "1340-6000",
    publisher = "Springer-Verlag GmbH and Co. KG",
    number = "3",

    }

    TY - JOUR

    T1 - Threshold conditions for bulk second-order nonlinearity and near-surface second-order nonlinearity in thermally poled infrasil silica

    AU - Qiu, Mingxin

    AU - Mizunami, Toru

    AU - Shimomura, Teruo

    AU - Ohtaki, Michitaka

    PY - 2001/1/1

    Y1 - 2001/1/1

    N2 - Generation of bulk second-order nonlinearity in silica glass requires higher poling temperature or longer poling time than that of near-surface second-order nonlinearity. The threshold conditions for initiating the bulk second-order nonlinearity are studied on Infrasil fused silica glass. The threshold poling time is strongly dependent on the poling temperature. The near-surface second-order nonlinearity is also studied, especially the dependence of thickness of the nonlinear layer on the poling temperature, poling voltage and poling time. Secondary-ion mass-spectroscopy measurement showed depletion of Na+ ions at the anodic surface. We assume there is an ionic wave during poling traveling from the anodic surface to generate the dipolar electric field that induces the near-surface second-order nonlinearity.

    AB - Generation of bulk second-order nonlinearity in silica glass requires higher poling temperature or longer poling time than that of near-surface second-order nonlinearity. The threshold conditions for initiating the bulk second-order nonlinearity are studied on Infrasil fused silica glass. The threshold poling time is strongly dependent on the poling temperature. The near-surface second-order nonlinearity is also studied, especially the dependence of thickness of the nonlinear layer on the poling temperature, poling voltage and poling time. Secondary-ion mass-spectroscopy measurement showed depletion of Na+ ions at the anodic surface. We assume there is an ionic wave during poling traveling from the anodic surface to generate the dipolar electric field that induces the near-surface second-order nonlinearity.

    UR - http://www.scopus.com/inward/record.url?scp=0035528329&partnerID=8YFLogxK

    UR - http://www.scopus.com/inward/citedby.url?scp=0035528329&partnerID=8YFLogxK

    U2 - 10.1007/s10043-001-0159-5

    DO - 10.1007/s10043-001-0159-5

    M3 - Article

    VL - 8

    SP - 159

    EP - 162

    JO - Optical Review

    JF - Optical Review

    SN - 1340-6000

    IS - 3

    ER -