Low-order optical nonlinearities of PbS quantum dot liquids and films
Introduction
During last two decades, the small-sized nanoparticles, like quantum dots, became an important subject of studies. Among studied species are the depositions of metal nanoparticles in dielectrics [[1], [2], [3], [4]], semiconductor nanoparticles synthesized during laser ablation in liquids [5], chalcogenide nanoparticles doped in thin films [6], etc. Nonlinear optical properties of quantum dots (QDs) attract the attention due to their potential applications in optoelectonics and laser physics. Being presented in different forms (colloidal quantum dots, thin films, laser-induced plasmas), these QDs can notably increase the nonlinear optical response due to specific properties related with the quantum confinement and growing role of the local field, which can dramatically increase the response of the medium in the presence of laser field. The potential application can be related with the attractive properties of QDs to adjust the saturable absorption (SA), which can be used for the mode-locking of lasers and shortening the pulse duration from master oscillators. The reported large nonlinear susceptibilities of QD-containing materials allow expecting the modulation of the characteristics of laser pulses propagating through such species. One o such attractive materials is the lead sulfide.
Lead sulfide (PbS) is an important IV-VI group chalcogenide semiconductor that has attracted considerable attention due to its numerous optical and optoelectronic properties and useful applications in solar cells, optoelectronic devices, photoconductors, sensors and infrared detector devices [7,8]. Two decades of research on PbS colloidal QDs (CQDs) manifested in the development of synthetic procedures for QDs with narrow size distribution and good colloidal stability [9,10]. PbS thin films has direct optical bandgap that can be changed from 0.39 up to 5.20 eV [11]. PbS nanoparticles have been successfully examined for use in solar cells exhibiting the efficiency up to 13.8% [12,13]. PbS is sensitive to radiation at the wavelengths between approximately 1 and 2.5 μm.
The impressive third-order nonlinear optical properties make nanoscale PbS potentially useful in electroluminescent devices like light-emitting diodes and optical devices such as optical switches [14]. Special attention to the thin films containing these QDs is also related with the growth of such parameters as the nonlinear refractive indices (γ), nonlinear absorption coefficients (β) and saturation intensities (Isat). The optical nonlinearities of nanoscale semiconductors in the quantum confinement regime have been frequently reported in the literature. Quantum confinement is found to enhance the nonlinear optical response, and a number of reports have discussed the physical processes underlying the mechanism of optical nonlinearity in QDs [15]. Particularly, the reduction of the PbS QDs to 2 nm showed the increase in band gap energy to 5.4 eV [16].
Most of previous studies of PbS QDs were carried out using ultrafast lasers. Particularly, saturable absorbers on the base of lead sulfide QDs for lasers emitting at 1, 1.3, 1.5, 2.1 μm can be used both for mode-locking and Q-switching of near IR lasers [17]. For PbS QDs, the nonlinear refraction index was found to be 5.1 × 10−16 cm2 W−1 in the case of 35 fs, 800 nm probe pulses [18]. Authors of [18] revealed that, contrary to the theory, PbS QDs’ nonlinear refractive index increases with size. The application of longer probe pulses (i.e. those in the range of a few nanoseconds) can reveal new peculiarities in the low-order nonlinear optical response of these QDs, especially in the case when they presented in liquid and thin film forms.
Here we present the results of our studies of the low-order nonlinearities of the PbS CQDs of different sizes being synthesized in liquids in the case of 10 ns pulses using different wavelengths of the probe radiation. We demonstrate the variations of the nonlinear absorption in the suspensions of PbS QDs of different sizes (9 and 2.5 nm) and show that these colloidal quantum dots possess the negative nonlinear refraction and reverse saturable absorption (RSA). The almost ten-fold growth of the nonlinear optical parameters in the visible range compared with the near infrared region was attributed to the stronger influence of the excitonic states on the propagation effects in the former case. We discuss the difference in the optical nonlinearities of 9-nm and 2.5-nm QDs, as well as analyze the signs of nonlinear refraction and nonlinear absorption of these quantum dots. Finally, we show that thin films containing these quantum dots demonstrate SA, while the suspensions show mostly RSA or two-photon absorption (TPA) depending on the wavelength of probe radiation. The enhancement of the nonlinear refractive index of films compared with suspensions, as well as a notable growth of nonlinear absorption coefficient in the former case, is demonstrated.
Section snippets
Synthesis and characterization of QDs
For the study of optical and nonlinear optical properties both small- and medium-sized PbS QDs were synthesized. The preparation of small colloidal quantum dots of lead chalcogenides (<3 nm) with good size-distribution requires special procedures [19]. In our case, the synthesis of small-sized lead sulfide QDs was performed by the modified procedure developed by Durmusoglu et al. [20]. It proceeds in the presence of dodecanethiol-1 in order to slow down the growth of nanocrystals.
9-nm sized quantum dots
The concentration of 9-nm sized QDs was C = 10−5 M. The thickness of used cell was 0.2 mm. The red filled circles in Fig. 2a correspond to CA z-scan at which negative nonlinear refraction was the dominating nonlinear optical process. These data were obtained using relatively low-energy 1064 nm pulses (E = 0.09 mJ). The four-fold growth of pulse energy (E = 0.36 mJ) led to the dominant influence of the positive nonlinear absorption attributed to TPA over nonlinear refraction (green empty
Discussion
Exciton Bohr radius for PbS is estimated to be about 18 nm. Therefore PbS quantum dots with mean size below 18 nm should demonstrate the quantum-confinement effect. These nanoparticles possess different absorption spectra, photoluminescence and photoelectric properties. 2.5 nm nanoparticles were selected as a first object for our study. Meanwhile, larger (9 nm) nanostructures could be very beneficial in comparison with smaller-sized QDs due to the difference in optical properties. As it was
Conclusions
Our studies of PbS QDs have shown that larger particles demonstrate stronger nonlinear optical effects compared with smaller QDs. The reason of such response of QDs corroborates with earlier suggested explanations of this effect. We have shown that these colloidal quantum dots possess the thermal-lens related negative nonlinear refraction and reverse saturable absorption while probing by nanosecond pulses. The larger nonlinear absorption coefficient of 9-nm quantum dots compared with 2.5-nm
Funding
European Regional Development Fund (1.1.1.5/19/A/003), State Assignment to Higher Educational Institutions of Russian Federation (FZGU-2020-0035), Russian Foundation for Basic Research (18-29-20062).
Disclosures
The authors declare no conflicts of interest.
Data availability statement
The data that support the findings of this study are available on request from the corresponding author.
CRediT authorship contribution statement
R.A. Ganeev: Conceptualization, Writing – review & editing. I.A. Shuklov: Methodology, Data curation. A.I. Zvyagin: Investigation. D.V. Dyomkin: Investigation. S.I. Bocharova: Investigation. V.S. Popov: Investigation. V.F. Toknova: Investigation. A.A. Lizunova: Investigation. O.V. Ovchinnikov: Writing – review & editing. V.F. Razumov: Supervision.
Declaration of competing interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
References (50)
- et al.
Physica B
(2005) - et al.
Mater. Lett.
(2012) - et al.
Int. J. Electrochem. Sci.
(2014) - et al.
Joule
(2020) - et al.
Mater. Today Chem.
(2020) J. Phys. Chem. Solid.
(1959)- et al.
Opt. Mater.
(2020) - et al.
Phys. Status Solidi B
(2003) - et al.
Phys. Status Solidi B
(2004) - et al.
Phys. Status Solidi B
(2004)
Appl. Phys. B
J. Opt. A
Mater. Sci. Eng.
Science
J. Am. Chem. Soc.
Adv. Funct. Mater.
J. Phys. Chem.
Opt. Lett.
J. Appl. Phys.
Proc. SPIE
Photonics
Russ. Chem. Rev.
J. Phys. Chem. C
Cryst. Growth Des.
J. Am. Chem. Soc.
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