“…Second, bandgap excitations (Fig. 4(i)) at room temperature seem to produce markedly different effects on SiO 2 and As 2 S 3 , i.e., defect formation [23] and photodarkening (PD), respectively [24]. Hosono et al suggest for SiO 2 that bandgap photons excite unstrained normal bonds (≡Si-O-Si≡), creating Si wrong bonds and interstitial oxygen as forms of peroxy-radicals (PORs, ·O-O-Si≡) and O 2 [31].…”
Section: Nonlinear Optical Excitationmentioning
confidence: 99%
“…super-gap (ћω > E g ) Si-Si [20], small ring [21] photodecomposition [22] bandgap (ћω ≃ E g ) Si-Si [23] PD, +ΔV, +Δn (D 0 at low T) [24] sub-gap (ћω < E g ) -ΔV and +Δn [25] by 7.9eV 2S excitation [26], E' centers and NBOHCs by 2P [27] PD, +ΔV, +Δn by 2.0eV 1P excitation [28] half-gap (ћω ≃ E g /2) E', -ΔV and +Δn by 6.4eV photons [25] PORs destruction by 5.0eV photons [29] 1P excitation gives no effects 2P excitation gives +Δn and As-As, but no PD [30] Although research trends in SiO 2 and As 2 S 3 are substantially different, reflecting different bandgap energies of ~9 eV and 2.4 eV, we can point out several interesting features. First, responses to super-gap excitations appear to resemble.…”
Linear and nonlinear optical properties in oxide and chalcogenide glasses have been studied comparatively. Applying a semiconductor concept to these glasses, we show that maximal nonlinear refractive-index at optical communication wavelengths is ~10 -4 cm 2 /GW, which can be obtained in materials with bandgap energy of ~1.6 eV. It is also shown for SiO 2 and As 2 S 3 that linear and nonlinear optical excitations induce different photostructural changes, which are attributable to different photo-electronic transition probabilities.
“…Second, bandgap excitations (Fig. 4(i)) at room temperature seem to produce markedly different effects on SiO 2 and As 2 S 3 , i.e., defect formation [23] and photodarkening (PD), respectively [24]. Hosono et al suggest for SiO 2 that bandgap photons excite unstrained normal bonds (≡Si-O-Si≡), creating Si wrong bonds and interstitial oxygen as forms of peroxy-radicals (PORs, ·O-O-Si≡) and O 2 [31].…”
Section: Nonlinear Optical Excitationmentioning
confidence: 99%
“…super-gap (ћω > E g ) Si-Si [20], small ring [21] photodecomposition [22] bandgap (ћω ≃ E g ) Si-Si [23] PD, +ΔV, +Δn (D 0 at low T) [24] sub-gap (ћω < E g ) -ΔV and +Δn [25] by 7.9eV 2S excitation [26], E' centers and NBOHCs by 2P [27] PD, +ΔV, +Δn by 2.0eV 1P excitation [28] half-gap (ћω ≃ E g /2) E', -ΔV and +Δn by 6.4eV photons [25] PORs destruction by 5.0eV photons [29] 1P excitation gives no effects 2P excitation gives +Δn and As-As, but no PD [30] Although research trends in SiO 2 and As 2 S 3 are substantially different, reflecting different bandgap energies of ~9 eV and 2.4 eV, we can point out several interesting features. First, responses to super-gap excitations appear to resemble.…”
Linear and nonlinear optical properties in oxide and chalcogenide glasses have been studied comparatively. Applying a semiconductor concept to these glasses, we show that maximal nonlinear refractive-index at optical communication wavelengths is ~10 -4 cm 2 /GW, which can be obtained in materials with bandgap energy of ~1.6 eV. It is also shown for SiO 2 and As 2 S 3 that linear and nonlinear optical excitations induce different photostructural changes, which are attributable to different photo-electronic transition probabilities.
“…Actually, an argon excimer laser light has the ability to convert quartz glass or silicon nitride into elemental silicon without any chemical assist. [4,8] In this case, the intense laser light formidably raises the material temperature at the same time. Fortunately, for the wafer cleaning, the excimer lamp provides light with a moderate power.…”
Section: Discussionmentioning
confidence: 97%
“…Takigawa et al demonstrated experimentally that an Ar excimer laser is capable of the dissociation of SiO 2 only by the irradiation. [4] This is because the photon energy (9.8 eV) is larger than the binding energy of Si-O bonds. Hence, a light source of high photon energy has the possibility to realize a new process technology.…”
“…The microscopic processes which occur in Si-O network under VUV excitation by high energy photons are still far from completely understood. VUV or multiphoton UV irradiation is capable of inflicting a massive damage to SiO 2 network, as illustrated by recently observed steady desorption of Si-O molecules and Si and O atoms or positive ions from the surface of F 2 -laser irradiated a-SiO 2 [20] or formation of elemental Si on Ar 2 (ħω = 9.8 eV) laser-irradiated surfaces of SiO 2 [21]. Another interesting recent finding is the creation of NBOHC in very large concentrations in surface layer by far VUV synchrotron irradiation [22].…”
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