Second and third-order nonlinear optical properties of Er3+/Yb3+ doped PbO-GeO2-Ga2O3 glasses with Au nanoparticles
Graphical abstract
Introduction
Materials with large optical nonlinearities have recently become the topic of a broad scientific interest, mostly because of their possible application in high-speed optical switching devices, which have become increasingly important and are more commonly used [1], [2], [3], [4], [5], [6], [7], [8]. Compounds which may vary in their nonlinear optical response using external laser are of particular interest. The large interest in nonlinear optical materials has been motivated by their potential use in the fabrication of all-optical photonic devices. Among several interesting candidates for photonic applications, glasses receive special attention because of their chemical and mechanical stability and wide compositional range that can be explored to tune the desired property for a specific application. Despite the relatively low nonlinear optical (NLO) efficiencies, their applications have a principal advantage due to possible applications of the photoinduced treatment to operate by the NLO susceptibilities. Furthermore, glasses may present fast response time and high nonlinearities, features of foremost for photonic devices [9]. Glasses containing highly polarized atoms present good nonlinear optical properties on account of their easily deformable electron clouds. Heavy metal oxide glasses have shown to be promising materials for all-optical devices due to large hyperpolarizabilities of their heavy metals [10], [11]. Glasses containing lead oxide are of particular interest; they show significant laser-induced NLO effects [12], [13]. They are also adequate hosts to rare earth incorporation and have demonstrated important technological applications.
These glasses are a convenient technology for incorporation of rare earths [14]. They exhibit a large transmittance window from the visible to the infrared region, low cutoff phonon energy 700 cm−1 and high refractive index (2.0). Their high third-order nonlinearities, are fundamental to the development of all-optical devices [15]. Particularly, the presence of lead oxide was investigated in tellurite, germanate, silicate and borate glass [16], [17], [18], [19], [20]. Studies on binary systems have shown an enhancement of the third-order nonlinearities with increases in lead content due to Pb2+ ions [17], [19]. It is known, for instance, that glasses presenting high nonlinear index of refraction also exhibit strong two-photon absorption, which is deleterious for all-optical switching applications. The knowledge of both properties, the nonlinear refraction and absorption, can help select, for example, the optimum operational wavelength for an optical device using a certain sample. Metal dielectric composites have attracted much attention from the point of view of nonlinear optics for their large nonlinear susceptibilities and fast response time [21]. One of the promising ways to enhance their NLO efficiency is to add nano-sized metallic particles. Third-order susceptibilities of dielectric materials with noble metal are considerably enhanced around the surface plasmon resonance (SPR) frequency [21]. Optical materials containing metallic nanoparticles have been attracting a great deal of attention because they may contribute to the enhancement of the optical nonlinearities as well [22]. Such improvement is significant for the development of all-optical photonic devices, such as optical switches and limiters. So the role of plasmonics in nonlinear optics was exploited in bulk and thin films. The results were interesting in that they showed the enhancement of nonlinear optical properties caused by local field enhancement because of collective oscillation of the free electron on the metallic nanoparticle surface, under laser excitation with wavelengths larger than their size. Also, it was shown that smaller nanoparticles and those with sharp edges are more interesting for nonlinear effects as the local field effects enhance the hyperpolarizabilites for these cases [22], [23]. Besides the hyperpolarizability of the glass constituents, addition of metallic nanoparticles is also expected to improve the higher-order optical nonlinearities of glasses. So, when heavy metal oxide materials are doped with metallic nanoparticles, there may be even higher nonlinear effects caused by the local field enhancement in the vicinity of the metallic nanoparticles. PbO-GeO2 glasses with and without silver nanoparticles demonstrated to be suitable for all-optical switching at telecom wavelengths (700–1400 nm). Besides, at the visible range, a PbO-GeO2 glass with silver nanoparticles, annealed for 3 h, behaves either as a saturable absorber or as an optical limiter [24]. Also, the third-order nonlinear properties and the response time of GeO2–Bi2O3 glass, as well as the effect of gold nanoparticles on these properties was reported in the reference [15]. The results show that the presence of gold nanoparticles causes a saturable absorption effect that is overcome by the two-photon absorption process at higher light intensities, for wavelengths within the SPR band.
Besides results of nonlinear refractive index and nonlinear absorption coefficient for PbO-GeO2, thin films with gold nanoparticles were also reported recently [25]. A large value for the nonlinear absorption coefficient was obtained at 532 nm, in the presence of gold nanoparticles, indicating possible applications for optical limiting in the nano and picosecond regime. The nonlinear refractive indices at 532 nm (15 ps pulse duration) and at 800 nm (100 fs pulse duration), are larger than those measured under the absence of gold nanoparticles, by more than one order of magnitude. The potential applications of nonlinear optical (NLO) materials in wavelength conversion, generation of ultra-short pulses, optical signal processing and ultrafast switching has motivated several studies that have been reported in the literature.
This paper presents the second- and third- order nonlinear properties of Er3+/Yb3+ -doped PbO-GeO2-Ga2O3 glasses with Au nanoparticles. The NLO parameters were investigated using classic Z-scan and second harmonic generation (SHG) techniques. We report results of the nonlinear absorption and refractive index as well as the SHG efficiency. The correlation between the NLO parameters and the annealing for the nucleation of gold nanoparticles is presented, and it shows that the sample annealing process affects the NLO values. Understanding the influence of metallic nanoparticles on the NLO properties of metal-dielectric composites may be of crucial importance in designing nanoparticle -based components for special applications.
Section snippets
Production and characterization of the glasses
To the basic glass composition 17.0GeO2 – 72.8PbO – 10.2Ga2O3 (in wt.%) was added 0.5 wt.% of Er2O3, 1.0 of Yb2O3 and 3.0 wt% of Au2O3. The conventional melt-quenching method was used to prepare the glass [9]. Batches of 7.0 g of high purity (99.999%) compounds were fully mixed in a platinum crucible and melted at 1200 °C for 1 h. The melts were then poured into pre-heated brass molds, in air, and annealed at 392 °C for 1 h to avoid internal stress. Additional annealing was performed during 1, 12, 28
Results and discussion
In Fig. 7 we can see the absorption spectra of examined glasses. Absorption bands attributed to 4f-4f transitions of Er3+ ions corresponding to the transitions starting from the ground state (4I15/2) to the excited states are observed. The bands centered at 490, 522, 545, 654, 800, 973 and 1530 nm are due to the transitions: 4I15/2 → 4F7/2,4I15/2 → 2H11/2, 4I15/2 → 4S3/2, 4I15/2 → 4F9/2, 4I15/2 → 4I9/2, 4I15/2 → 4I11/2 and 4I15/2 → 4I11/2 respectively. The intense absorption band at ≈980 nm is mainly due to
Conclusion
We presented results of two-photon absorption parameters and of nonlinear refractive index for Er3+/Yb3+ doped PbO-GeO2-Ga2O3 glasses with Au nanoparticles annealed for 1, 12, 28 and 52 h. These parameters were obtained by Z-scan measurements, performed at 532 nm, the wavelength region associated to the SPR of gold. It was possible to observe that the presence of gold nanoparticles affects them within the SPR absorption band region. The highest value of the TPA coefficient was obtained for an
Acknowledgements
The work was performed in the framework of the National Institute of Photonics (INCT de Fotônica/ CNPq). We acknowledge the Nanotechnology National Laboratory (LNNano) for HR-TEM measurements.
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