Abstract
We report on a strategy to realize simultaneous and efficient multi-band near-infrared (NIR) emission from Pr3+, Tm3+ and Er3+ that covers almost the entire optical communication wavelength region (from O to U band) by employing a nanocrystal-solvent colloidal system. The NIR emission spectra and fluorescent decay curves of different colloidal systems are investigated and compared. The results indicated that interaction among different RE ions that lead to quenching of the NIR emission could be effectively inhibited by solutions containing NCs doped with three different ion pairs (Yb3+-Pr3+, Yb3+-Tm3+ and Yb3+-Er3+) separately. The mechanism of this phenomenon is also discussed. This strategy may have potential applications in multi-band optical amplifiers for the optical communication window.
© 2019 Optical Society of America under the terms of the OSA Open Access Publishing Agreement
1. Introduction
Rare-earth (RE) ions activated inorganic compound nanocrystals (NCs) have been paid growing attention because of their excellent optical properties, low toxicity and high stability against photo-degradation, which lead to their application in various fields [1–10]. RE ions, such as Pr3+, Er3+ and Tm3+, which are capable of emitting near-infrared (NIR) light in the communication wavelength region, have aroused special interest as they can be used as activator ions for fiber amplifiers and planar waveguide amplifiers [11–16]. Since the NIR emissions of aforementioned RE ions are all f-f transitions and their bandwidths are narrow in nature, they can not meet the requirement of broadband fiber amplifiers and tunable lasers in the NIR region, which are indispensable in dense wavelength-division-multiplexing (WDM) network systems [17–19]. At present, searching for a broadband NIR emitter has prompted intensive research into the optical properties of transition metal ions (such as Ni2+ and Cr4+), bismuth activated glasses and crystals [20–30]. However, the emissions of these ions are strongly correlated with the host. Their efficiencies as well as gain properties still can not rival that of RE-activated materials.
RE ions are still attractive NIR emitters with well-understood electronic transitions. To broaden the NIR emission of RE ions activated materials, one may simply think that this can be realized by means of codoping. However, this strategy fails in most circumstance. For emission of different RE ions in the same host, quenching often occurs due to interaction among different electronic transitions of the activators. To circumvent this problem, here we propose a simple strategy to realize simultaneous and efficient multi-band NIR emission from Pr3+, Tm3+ and Er3+ that covers the entire communication wavelength region (from O to U band) by employing a nanocrystals-solvent colloidal system. Within the colloid system, each NC contains only one type of NIR emitting ion, and different types of NCs which doped with different ions are spatially separated by distances long enough from each other, so that interaction among different RE ions that located in different NCs can be inhibited. With appropriate pumping, the colloid exhibits a multi-band NIR emission spectrum contributed from the respective transitions of RE ions located in different NCs. This NIR emitting colloid is expected to be a potential multi-band liquid gain medium for WDM system.
2. Experimental section
Synthesis of nanocrystals and the preparation of colloidal dispersion: Nanocrystals of RE doped NaYF4 were synthesized by a solvothermal route using the liquid-solid-solution strategy [31]. In a typical procedure, 1.0 g NaOH was dissolved in a solution of 10 mL ethanol and 5 mL H2O, to which 15 mL oleic acid was added subsequently, and stirred continuously until the solution become transparent. Then, aqueous solution of 1.0 mL RE3+ (0.5 M in total, in the form of RECl3) and 2.5 mL (1.0 M) NaF were added into the above solution and vigorously stirred for another 20 min. The ratio of different RE ions Y:Yb:Er (Pr or Tm) varies according to the composition of the target nanocrystals. The milky solution was finally transfered into a Teflon-lined stainless steel autoclave and heated to 150°C for 240 min with a electric oven. After natural cooling to ambient temperature, the nanocrystals deposited at the bottom of the Teflon container was collected and washed with ethanol. Colloidal solutions were prepared by dispersing the as-synthsized nanocrystals in less-polar or non-polar organic solvent such as cyclohexane, benzene and carbon tetrachloride (CCl4) under ultrasonic agitation for around 20 min. The as-prepared colloidal solutions are stable without noticeable precipitation (for 24 h) at concentrations up to 1.0 wt.%. For preparing solution with multi-band NIR emission, we just mix the three solutions that contain single type of NCs (NaYF4:Yb, Er or NaYF4:Yb, Tm or NaYF4:Yb, Pr) and adjust their fractions to optimize emission spectrum.
Characterizations: Morphological observation of the NCs was performed with a JEM-200CX transmission electron microscope (TEM) equipped with a charge-coupled device (CCD) camera. The specimen for TEM observation was prepared by loading the NCs from the colloidal solution on a carbon-coated copper grid. Crystal structure of the NCs was examined with powder X-ray diffraction using a Rigaku D/MAX-RA system. Optical absorption spectra of the colloid with a NCs concentration of 0.5 wt.% (filled in a 1 cm × 1 cm × 5 cm quartz cuvette) was recorded by a JASCO V-570 spectrophotometer. Emission spectra were measured using a ZOLIX SPB-300 spectrofluorometer equipped with an InGaAs detector, which has a detective wavelength region from 800 to 1650 nm.
3. Results and discussion
In the present work, sodium yttrium tetrafluoride (NaYF4) was chosen as the nanocrystalline host for RE ions. Since NaYF4 has a relative low vibration energy, it allows RE ions to emit efficiently in the NIR spectral region. A solvothermal route based on a liquid-solid-solution strategy was employed here for the synthesis of NCs [31]. The experimental conditions, such as the reaction time and temperature, were carefully determined so as to prevent Oswald ripening during synthesis and to obtain a mono-dispersive size distribution of the NCs. We chose 150°C as the solvothermal temperature and keep it for 4 h. α-NaYF4 NCs with a cubic crystal structure (space group Fm3 m, a = 0.548 nm) were obtained. The structure of NCs was revealed by X-ray diffraction (Fig. 5 in the Appendix).
From the transmission electron microscope (TEM) image (Fig. 1(a)), it can be clearly observed that the NCs crystallized into polyhedrons, mostly nanocubes, with a average size of approximately 25 nm (Fig. 1(b)). Furthermore, The surface of the NCs is decorated by a layer of long-chained alkyl groups formed in-site during the solvothermal synthsis [31–33], manifested by its favorable solubility in non-polar or less-polar organic solvent (such as cyclohexane, benzene and carbon tetrachloride). Here, we choose carbon tetrachloride (CCl4) as the solvent for the NCs-colloid system, for it is optically inert in the entire visible and NIR range (400 ∼ 2500 nm) due to the low vibration energy of the C-Cl bond. The CCl4 colloid of the NCs is optically transparent (Fig. 6 in the Appendix). Moreover, the colloidal system withstands a NCs concentration up to 1.0 wt.% without any discernable decrease in optical transmission and sedimentation of the NCs for over 24 h.
RE ions of Pr3+, Er3+ and Tm3+ with NIR emissions covering O to U band, respectively, were selected as the activator ions. For the purpose of achieving multi-band NIR emission with the colloidal solution of RE-doped NCs, the first obstacle is caused by the fact that there is no electronic level with identical energy exists for these ions. Therefore, it is difficult to simultaneously excite the three different ions doped in different NCs to generate efficient NIR emission by single wavelength pumping. This problem is circumvented here by the use of an efficient sensitizer ion Yb3+, which has a large absorption cross section due to its 2F7/2→2F5/2 transition at around 980 nm. To maximize the fluorescence intensity from the NCs solution, in the first step we examine the dependence of NIR fluorescence intensity of NCs on the concentration of the sensitizer Yb3+ ion for the three different types of NCs doped with ion pairs of Yb3+-Pr3+, Yb3+-Tm3+, and Yb3+-Er3+ (Fig. 7 in the Appendix). The emission spectra are given in Fig. 2. For Yb3+-Pr3+ pair, energy transfer from 2F5/2 to 1G4 takes place upon excitation at 980 nm, and this is followed by emission peaking at 1310 nm from Pr3+ by transition of 1G4→3H5. Likewise, 1550 nm emission due to 4I13/2 → 4I15/2 of Er3+ occurs as a result of energy transfer from 2F5/2 to 4I11/2 after absorption of the 980 nm pumping light. The energy transfer process is quite different for Yb3+-Tm3+ pair, in which a consecutive excitation process occurs due to energy transfer from Yb3+ and excited state absorption: first the transition of 3H6→3H5, and then 3F4→3F2. Consequently, emission from Tm3+ comprises contributions from transition of 3H4→3F4 at approximately 1470 and 3F4→3H6 centered on 1620 nm (The maximum emission intensity for this transition is usually at around 1840nm, which is out of the detection range of the InGaAs detector used in this work) [34,35]. The spectral result shown in Fig. 2 indicates that the optimal concentrations of the sensitizer (Yb3+) is 5%, 50% and 20% for ion pairs of Yb3+-Pr3+, Yb3+-Tm3+, and Yb3+-Er3+, respectively. Hereinafter these nanocrystals with the optimal Yb3+ concentration exhibiting the strongest emission intensity are denoted as NC-YP, NC-YT, and NC-YE, respectively.
The second step involves the mixing of different NCs in a single colloid system with appropriate ratio to obtain the broadened NIR emission spectra. To clarify the feasibility of simultaneously observe NIR emission from all the three types of NCs in a solution, in which resonant energy transfer among different ions is negligible, we first give a preliminary analyses on the distance-dependent energy transfer process among different ions. From the Forster-Dexter model [36,37], the energy transfer rate from a donor to an acceptor is expressed by:
To obtain an in-depth understanding of the interaction among RE ions for the colloid system, the decay profiles of the three different types of NCs-colloid systems are recorded at the emission wavelengths of 1310 nm, 1470 nm and 1550 nm that belong to radiative transitions of Pr3+, Tm3+ and Er3+, respectively (Fig. 4). It can be seen that the decay rates for the colloids containing single types of NCs and mixture of NCs are almost comparable, in striking comparison to the remarkably increased decay rates for the colloids containing NCs codoped with four types of ions. The decay of luminescence is characterized by an average lifetime that can be expressed by
where $I(t)$ stands for the intensity at time t. The obtained lifetimes of the solution containing mixture of NC-YP, NC-YT and NC-YE are far longer than that of the results obtained from the colloid contained the codoped NCs (Fig. 4). These results clearly indicate that the effect of nonradiative transition by means of cross relaxation among different ions dominants the decay process for the codoped NCs, whereas it is effectively suppressed for the solution containing mixture of NC-YP, NC-YT, and NC-YE.To realize multi-band optical amplification in the communication wavelength region using the colloids containing NCs, it is indispensable to estimate the attenuation of light as a result of absorption and scattering. According to Beer-Lambert law the intensity of transmitted light can be expressed as:
where IT and I0 denote the intensities of the transmitted and the incident light, α is the absorption coefficient, σ is the turbidity which is caused by scattering. In the colloidal system, the concentration of the NIR emitting ions are estimated to be approximately 2.0 × 1017 ion/cm3 (for the solution with a NCs concentration of 0.5 wt.%), and the absorption cross section are in the magnitude of 10−20 cm2, therefore, the absorption coefficient is estimated to be ∼2.0 × 10−3 cm-1. As of light scattering by colloidal system containing widely separated scattering centers, the total turbidity is given by: where N is the nanocrystal number density, V is the volume of the nanocrystal, r is the radius of the nanocrystals (typically 20∼30 nm), k = 2π/λ (λ is the wavelength), n is the refractive index of the nanocrystal (approximately n = 1.6 for NaYF4), and Δn is the index difference between the nanocrystal and the solvent [40,41]. Based on an estimation using the equation above, we found that the effect of scattering is almost negligible (σ∼10−7 cm-1) compared with absorption in the NIR spectral region of 1000∼2000nm. Practically, the light attenuation for a colloidal solution (0.5wt%) with a thickness of 1 mm is around 1.3% - 2.5% in the NIR range, except for a few peaks due to the absorption by the capping agent (oleic acid).In the final discussion, we made a preliminary calculation of the optical gain for the colloidal amplifier using the equation developed for the four-level system as express by
The absorbed pump power Pabs can be written as where σe is the emission cross section of the RE ions, and hvp is the pump photon energy, and A is the cross section of the fiber core [42, 43]. We assume a fiber amplifier employing a capillary tube filled with the NCs colloid. For a fiber length of l = 2 cm, with the core diameter of 100 μm, the estimated optical gain is approximately in the range of 0.05∼0.5 dB/W at the peak wavelengths of 1310 nm, 1470 nm and 1550 nm. However, the presence of a large dip in the emission spectrum given in Fig. 3 centered at around 1360 nm indicate that broadband optical gain across the whole optical communication bandwidth is practically unattainable. These analyses suggest that the colloidal based capillary amplifier system might have the potential for practical multi-band optical amplification.4. Conclusions
To summarize, we have investigated the NIR emission of colloids containing nanocrystals doped with ion pairs of Yb3+-Pr3+, Yb3+-Tm3+ and Yb3+-Er3+. The results indicated that interaction among different RE ions that lead to quenching of the NIR emission could be effectively inhibitted by solutions containing NCs singly doped with three different ion pairs. Our detailed analyses suggest that the multi-band NIR emitting solution of NCs mixtures, or an index-matched polymer waveguide incorporating the NCs, may find potential applications in multi-band optical amplifiers in the optical communication wavelength region.
Appendix
Funding
National Natural Science Foundation of China (NSFC) (50872123, 51772270); State Key Laboratory of Precision Spectroscopy (SKLPS); State Key Laboratory of High Field Laser Physics; Opening Project of State Key Laboratory of High Performance Ceramics and Superfine Microstructure, Shanghai Institute of Ceramics, Chinese Academy of Sciences (SICCAS) (SKL201706SIC); National Key R and D Program of China (2018YFB1107200).
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