Journal of Applied Physics · 1997 · 16 citations · 17 references
Natural SciencesMaterials EngineeringMaterials ScienceMaterials ChemistryOptical MaterialsOpticsGlass MaterialsLaser Host MaterialsOptical GlassesOptical Properties Of MaterialsOptical Properties Of SolidsPhotonic MaterialsAbsorption Band AssignmentLaser Beam AbsorptionLaser MaterialsNetwork Structure Of GlassSilica-based MaterialsSilicate GlassesSoot DepositionStrained Layer Structures
Characteristics of ArF-excimer laser-induced absorption in various types of fused silica synthesized by the vapor-phase axial deposition-soot remelting method were investigated. Fused silica containing 2−6×1018 cm−3 of OH and no Cl shows an absorption band at 5.8 eV ascribed to the E′ center (≡ Si ⋅) and an absorption band at 4.8 eV ascribed to oxygen related centers. A sample containing about 3×1019 cm−3 of Cl and no OH shows only the 5.8 eV band. An OH- and Cl-free silica had a preexisting absorption band at 5.0 eV ascribed to an oxygen deficient center (ODC; ≡ Si ⋅⋅⋅ Si ≡) and a weak band at 5.8 eV; the 5.0 eV band changed into a 5.8 eV band by irradiating it with the ArF laser. These phenomena can be interpreted as follows: typical silica glasses are considerably deformed from the ideal network and terminal groups such as Si–OH and Si–Cl reduce some amount of highly strained bonds in the glass network. In the sample containing a considerable amount of Cl and no OH, Si–Cl could be the major precursor of the E′ center because only a weak 5.8 eV band is observed. In silica containing a relatively small amount of OH and no Cl, bond breakage is the major process by which laser induced defects are produced.
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Two types of oxygen-deficient centers in synthetic silica glass
Hiroaki Imai, Kazuo Arai, Hiroshi Imagawa et al. · Physical review. B, Condensed matter · 1988 · 287 citations