1Key Lab of Optoelectronic Devices and Systems of Ministry of Education/Guangdong Province, College of Optoelectronic Engineering, Shenzhen University, Shenzhen 518060, China
2College of Information Engineering, Shenzhen University, Shenzhen 518060, China
Shuai Ye, Guangsheng Wang, Maozhen Xiong, Jun Song, Junle Qu, Weixin Xie. Pure red visible emission via three-photon excitation of colloidal Na3ZrF7:Er nanoparticles using a telecom-band laser[J]. Chinese Optics Letters, 2017, 15(1): 011601
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We provide the first demonstration of pure red emission in the visible light region via three-photon excitation in monodisperse nanoparticles (NPs) by using a laser operating in the telecommunication band. NPs of in diameter are synthesized at 260°C by the thermal decomposition method. The experimental results reveal that the NPs exhibit pure red emission in the visible region under 1480 nm laser excitation, and the emission intensity is significantly influenced by the ion concentration. The decay times of the and transitions of the ions at 540 and 655 nm, respectively, are reduced by increasing the ion concentration in the
The multiphoton effect based on two-photon or three-photon technology is receiving increasing attention due to its comprehensive applications in biomedicine, photovoltaics, optical telecommunications, etc.[1–10]. Similar to other nonlinear optical technologies, the common multiphoton effect has very low efficiency to upconvert the energy of excited photons, as the intermediate levels are virtual[11]. In comparison, lanthanide-doped upconversion nanoparticles (UCNPs) can effectively convert low-energy photons (always infrared light) into ultraviolet, visible, or near-infrared (NIR) photons, owing to their ladder-like system of energy levels[12]. Until now, owing to their high efficiency, the most frequently used UCNPs have been hexagonal nanoparticles (NPs) doped with (, Tm, Ho)[13,14]. Upon laser excitation at 980 nm, these UCNPs emit visible light by a two-photon process.
For biomedical applications, it is often important for the excitation light to penetrate far into the sample; however, the penetration depth is limited by Rayleigh scattering, owing to the effect on the beam quality. Since Rayleigh scattering scales as , long-wavelength multiphoton excitation seems promising for biomedical applications, e.g., in vivo biological imaging and photo dynamics therapy (PDT) of deep tumors. It has been shown that an optimum wavelength window, owing to scattering and absorption in tissue, lies close to the telecom band[15]. Recently, ions have been considered to be a promising choice, owing to their strong absorption at , which corresponds to the energy transfer from the energy level to the energy level[16]. NPs were first reported by Chen et al.[17] to exhibit multicolor emission under 1490 nm laser excitation by three-photon upconversion (UC) process. Subsequently, UCNPs excited at 1550 or 1523 nm were reported[18,19], and it was found that the emission intensity could be largely enhanced by the inert shell[20]. These UCNPs irradiated almost multicolor light containing nm (green), nm (red), and NIR wavelengths. However, red emission is widely considered to be the most promising candidate for deep tissues, owing to its penetration capabilities[21,22]. Additionally, the most frequently used photosensitizer in PDT applications strongly absorbs in the red light region[23].
Many studies have investigated UCNPs with pure red emission under a 980 nm laser excitation by a two-photon UC process[24–29], but no studies were published on NPs upconverting from the telecom band to red light by a three-photon process. In this work, -doped NPs were synthesized by following a procedure that had been previously used[30]. Upon 1480 nm laser excitation, these UCNPs irradiated pure red light centered at 660 nm in the visible light region. The effect of the ion concentration on the emission intensity of -doped NPs was investigated. The mechanism behind the pure red emission was explained by considering the cross-relaxation effect.
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Figure 1(a) shows the X-ray diffraction (XRD) patterns of -doped NPs with different ion concentrations. The patterns revealed that all the as-synthesized NPs had a pure tetragonal phase structure (according to the standard host lattice of JCPDS No. 12-0562). No other phase was detected. This result indicated that the dopant ions completely replaced ions in the lattice. The typical transmission electron microscope (TEM) morphology of NPs is shown in Fig. 1(b). The as-synthesized NPs were monodispersed and tetragonal and exhibited a size of . Notably, the concentration of ions had a negligible effect on the size of the -doped NPs.
Figure 1.(a) XRD patterns of -doped NPs with different concentrations, and (b) typical TEM image of NPs.
Figure 2 shows the UC emission spectra of the synthesized -doped NPs under 980 and 1480 nm laser excitations. In our previous report, we confirmed that Er/Yb co-doped NPs displayed a single red emission under 980 nm laser excitation. However, the -doped NPs displayed multiband emission under 980 nm laser excitation even at the ion concentration of 20%, as shown in Fig. 2(b). Upon 1480 nm laser excitation, the -doped NPs displayed pure red emission (, corresponding to ) in the visible light region, whereas the green emission corresponding to the energy transfer from the level to the level almost disappeared, as shown in Fig. 2(a). A weak emission at (corresponding to ) and a strong emission at (corresponding to ) were observed in the NIR region. The emission intensity of -doped NPs was significantly affected by the concentration of ions. The emission intensity of the NPs was very weak, whereas the NPs displayed the strongest emission.
Figure 2.Spectra of -doped NPs with different concentrations excited by (a) 1480 and (b) 980 nm lasers. The insets are the photographs of the NPs dispersed in hexane.
To investigate the influence of the concentration on the emission intensity of NPs, the decay profiles of the and transitions of ions at 540 and 655 nm, respectively, were also measured under 1480 nm laser excitation, as shown in Fig. 3. The effective lifetime is given by the following formula: where is the intensity of the emission at time . The effective decay times were 73.7, 54.3, and 31.6 μs for the states and 580.9, 534.3, and 415.6 μs for the states of ions in NPs with concentrations of 5%, 10%, and 20%, respectively. The decay curves of the NPs were ignored, as the signal was very low and could be hardly detected. Clearly, the emission intensity of the NPs was closely related to the decay times: as the decay time decreased, the emission intensity of the NPs significantly declined. The short lifetime was mainly attributed to the appearance of defect-related quenching effects. When trivalent ions replaced tetravalent ions, extra ions and vacancies were formed in the matrix to re-balance the charge. These defects resulted in quenching effects that reduced the emission intensity of the NPs. By increasing the concentration in the NPs, the defect-related quenching effects were enhanced, and the emission intensity was reduced. The very weak emission of NPs was mainly related to two aspects: weak absorption to the excited photons, and weak energy transfer between neighboring ions, due to the low concentration.
Figure 3.Decay profiles of transitions of ions under 1480 nm laser excitation: (a) at 540 nm and (b) at 655 nm.
Figure 4 shows the ion energy levels and the proposed energy transfer UC mechanisms under the 1480 and 980 nm laser excitations. As shown in Fig. 4(a), under 1480 nm laser irradiation, the excitation of ions from the ground state to the state occurs through a ground state absorption (GSA) process, followed by energy transfer to the neighboring ions, which are then promoted to the higher and states. The emission centered at 820 nm [shown in Fig. 2(a)] was generated from the radiative decay from the state to the state by two-photon emission. Simultaneously, nonradiative relaxations occur from the state to the state, which produce the emission centered at 980 nm [Fig. 2(a)]. The radiative decay from the and state to the state by two-photon emission could produce the emissions at 525 and 540 nm (green emission). The disappearance of the green emission in the spectrum of NPs [Fig. 2(a)] was attributed to the cross relaxation between ions. Notably, clusters can easily form in the matrix because of the large mismatch between ions and ions, which reduced the distance between ions and enhanced the cross relaxation between ions [ (); Fig. 4(a)]. Owing to the cross-relaxation effect, the red emission (660 nm) was enhanced, whereas the green and 800 nm emissions were reduced, resulting in pure red emission in the visible light regions of the NP spectra [Fig. 2(a)]. When the NPs are excited by the 980 nm laser, excitation of the ions from the ground state to the state through a GSA process occurs, followed by a transfer of energy to the state of neighboring ions. The energy of the state is partly transferred to the state by the cross relaxation between ions [ ()] to enhance the red emission. Meanwhile, nonradiative relaxation occurs from the state to the and states, producing green emissions centered at 525 and 540 nm. This mechanism explains exactly why the NPs exhibit pure red emission under 1480 nm laser excitation, whereas they show strong red emission and weak green emission under 980 nm laser excitation.
Figure 4.Diagram of UC via energy transfer UC processes between two ions under (a) 1480 and (b) 980 nm laser excitation.
Monodisperse NPs with different ion concentrations are synthesized at 260°C. A negligible effect of the concentration on the NP microstructure and sizes is observed. These NPs irradiate pure red emission in the visible light region under 1480 nm laser excitation. The emission intensity is influenced significantly by the ion concentration. The suppression of the emission intensity with the increase in the ion concentration in the NPs results from the defect-related quenching effect, which emerges when tetravalent ions are replaced by trivalent ions. The pure red emission of the NPs under 1480 nm excitation is related to the cross relaxation [ ()] between ions, which becomes closer to each other owing to the formation of clusters.
Shuai Ye, Guangsheng Wang, Maozhen Xiong, Jun Song, Junle Qu, Weixin Xie. Pure red visible emission via three-photon excitation of colloidal Na3ZrF7:Er nanoparticles using a telecom-band laser[J]. Chinese Optics Letters, 2017, 15(1): 011601