JP2015517194A - 電磁ビーム用散乱層を作製する方法および電磁ビームを散乱するための散乱層 - Google Patents
電磁ビーム用散乱層を作製する方法および電磁ビームを散乱するための散乱層 Download PDFInfo
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Abstract
Description
PbO−B2O3,
PbO−SiO2,
PbO−B2O3−SiO2,
PbO−B2O3−ZnO2,
PbO−B2O3−Al2O3,
から形成することができ、PbOを含有するガラスはんだはBi2O3を有し得る。または鉛フリーのガラス系、例えばBi2O3を含有する系、すなわち、
Bi2O3−B2O3,
Bi2O3−B2O3−SiO2,
Bi2O3−B2O3−ZnO,
Bi2O3−B2O3−ZnO−SiO2
から形成することができる。
PbO−B2O3,
PbO−SiO2,
PbO−B2O3−SiO2,
PbO−B2O3−ZnO2,
PbO−B2O3−Al2O3,
であり、PbOを含有するガラスはんだはBi2O3を有し得る。または上記のガラス系は、鉛フリーのガラス系、例えばBi2O3を含有する系、すなわち、
Bi2O3−B2O3,
Bi2O3−B2O3−SiO2,
Bi2O3−B2O3−ZnO,
Bi2O3−B2O3−ZnO−SiO2
である。
Claims (15)
- 電磁ビーム用散乱層(106)を作製する方法において、
該方法は、
・ 支持体(102,104)上に散乱中心体(306)を載置するステップと、
・ 前記散乱中心体(306)上にガラス(312)を載置するステップと、
・ 前記ガラス(312)を液状化して、液状化したガラス(312)の一部が前記散乱中心体(306)の間に流れ込んで前記支持体の表面(302)に到達するが、前記液状化したガラス(312)の一部がなお前記散乱中心体(306)の上方に残存しているようにするステップとを有する、
ことを特徴とする方法。 - 請求項1に記載の方法において、
前記散乱中心体(306)は、アーチ形の表面を有する、
ことを特徴とする方法。 - 請求項1または2に記載の方法において、
前記散乱中心体(306)は、約0.1μmから約3μmまでの平均粒径を有する、
ことを特徴とする方法。 - 請求項1から3までのいずれか1項に記載の方法において、
前記支持体(102,104)に載置される前記散乱中心体(306)は、約0.1μmから約10μmまでの厚さを有する層(304)を構成する、
ことを特徴とする方法。 - 請求項1から4までのいずれか1項に記載の方法において、
前記ガラス(312)は、約1.7よりも大きい屈折率を有する、
ことを特徴とする方法。 - 請求項1から5までのいずれか1項に記載の方法において、
前記散乱中心体(302)上または当該散乱中心体(302)の上方における前記ガラス(312)は、前記層断面における複数の別の層(110,112,114)の、層厚で重み付けした屈折率よりも大きいかまたはほぼ等しい屈折率を有する物質または物質混合物からなる、
ことを特徴とする方法。 - 請求項1から6までのいずれか1項に記載の方法において、
前記ガラス(312)を硬化した後、前記散乱層(106)は、前記ガラス(312)の屈折率と、前記散乱中心体(306)の屈折率との間に約0.05よりも大きな屈折率の差分を有する、
ことを特徴とする方法。 - 請求項1から7までのいずれ1項に記載の方法において、
ソーダ石灰ガラスを支持体(102)として使用する場合、前記ガラス粉末(312)は最大で約600℃までの温度においてガラス化する、
ことを特徴とする方法。 - 請求項1から8までのいずれか1項に記載の方法において、
前記支持体(102,104)上に約1μmから約40μmの厚さで前記散乱層(106)を被着する、
ことを特徴とする方法。 - 請求項1から9までのいずれか1項に記載の方法において、
前記支持体(102,104)上にまたは当該支持体(102,104)の上方に散乱中心体懸濁液ないしは散乱中心体ペーストからなる前記散乱中心体(306)を被着する、
ことを特徴とする方法。 - 請求項10に記載の方法において、
前記支持体(102,104)上または当該支持体(102,104)の上方で、気化性の構成成分を用いて前記散乱中心体懸濁液を乾燥する、
ことを特徴とする方法。 - 請求項1から11までのいずれ1項に記載の方法において、
粒子(312)の前記ガラス(312)を、ガラス粉末(312)として前記散乱中心体に被着する、
ことを特徴とする方法。 - 請求項12に記載の方法において、
前記ガラス粒子(312)は、約0.1μmから約30μmまでの直径を有する、
ことを特徴とする方法。 - 光学素子において、
該光学素子は、
支持体(102,104)および散乱層(106)を有しており、
該散乱層(106)は、
・ マトリクス(408)と、当該マトリクス(408)内に埋め込まれかつ前記マトリクス(408)よりも屈折率の高いまたは屈折率の低い第1のタイプの少なくとも1つの光学的散乱中心体(306,410)とを有しており、
・ 前記散乱層(106)と前記支持体(102,104)との前記境界面(404)は、0%より大きい前記マトリクス(408)の体積密度を有しており、
・ 前記散乱層(106)の前記表面(402)は、100%の前記マトリクス(408)の体積密度を有しており、
・ 前記散乱層(106)の前記マトリクス(408)は、前記支持体(102,104)の前記表面(404)から前記散乱層(106)の前記表面(402)までに至る隙間のない、つながった少なくとも1つの結合体を有しており、
・ 少なくとも1つのタイプの散乱中心体(306,410)の前記体積密度は、前記支持体(102,104)の前記表面(404)から減少している、
ことを特徴とする光学素子。 - 請求項14に記載された光学素子を有する有機発光ダイオード。
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