Confining energy migration in upconversion nanoparticles towards deep ultraviolet lasing

Abstract

Manipulating particle size is a powerful means of creating unprecedented optical properties in metals and semiconductors. Here we report an insulator system composed of NaYbF₄ :Tm in which size effect can be harnessed to enhance multiphoton upconversion. Our mechanistic investigations suggest that the phenomenon stems from spatial confinement of energy migration in nanosized structures. We show that confining energy migration constitutes a general and versatile strategy to manipulating multiphoton upconversion, demonstrating an efficient five-photon upconversion emission of Tm³⁺ in a stoichiometric Yb lattice without suffering from concentration quenching. The high emission intensity is unambiguously substantiated by realizing room-temperature lasing emission at around 311 nm after 980-nm pumping, recording an optical gain two orders of magnitude larger than that of a conventional Yb/Tm-based system operating at 650 nm. Our findings thus highlight the viability of realizing diode-pumped lasing in deep ultraviolet regime for various practical applications.

ARTICLE

Received 17 Sep 2015 | Accepted 27 Nov 2015 | Published 7 Jan 2016

Xian Chen1,*, Limin Jin2,*, Wei Kong1, Tianying Sun1, Wenfei Zhang2, Xinhong Liu3, Jun Fan1,4, Siu Fung Yu2

& Feng Wang1,4

Manipulating particle size is a powerful means of creating unprecedented optical properties in metals and semiconductors. Here we report an insulator system composed of NaYbF4:Tm in which size effect can be harnessed to enhance multiphoton upconversion. Our mechanistic investigations suggest that the phenomenon stems from spatial connement of energy migration in nanosized structures. We show that conning energy migration constitutes a general and versatile strategy to manipulating multiphoton upconversion, demonstrating an efcient ve-photon upconversion emission of Tm3 in a stoichiometric Yb lattice without suffering from concentration quenching. The high emission intensity is unambiguously substantiated by realizing room-temperature lasing emission at around 311 nm after 980-nm pumping, recording an optical gain two orders of magnitude larger than that of a conventional Yb/Tm-based system operating at 650 nm. Our ndings thus highlight the viability of realizing diode-pumped lasing in deep ultraviolet regime for various practical applications.

DOI: 10.1038/ncomms10304 OPEN

Conning energy migration in upconversion nanoparticles towards deep ultraviolet lasing

1 Department of Physics and Materials Science, City University of Hong Kong, 83 Tat Chee Avenue, Hong Kong SAR, China. 2 Department of Applied Physics, The Hong Kong Polytechnic University, Hung Hom, Hong Kong SAR, China. 3 Department of Electronic Engineering, City University of Hong Kong,83 Tat Chee Avenue, Hong Kong SAR, China. 4 City University of Hong Kong Shenzhen Research Institute, Shenzhen 518057, China. * These authors contributed equally to this work. Correspondence and requests for materials should be addressed to S.F.Y. (email: mailto:[email protected]

Web End [email protected] ) or toF.W. (email: mailto:[email protected]

Web End [email protected] ).

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The construction of functional materials with designable optical properties is fundamentally important for scientic research and technological applications in diverse elds

encompassing energy, environment and biomedicine111. Given the constraints in designing materials using different combinations of elements, nanoscale manipulation of matters has become a promising alternative to the creation of novel functional materials1219. Particularly, by taking the advantage of size connement effects, the energy band structure in semiconductors can be precisely modied to offer size-tunable emission wavelengths20,21. Despite the attractions, the size effect is largely unexplored in lanthanide-doped upconversion nano-particles, which represents an important family of optical materials characterized by large anti-Stokes shift, narrow emission bandwidths and long excited-state lifetimes.

Photon absorption and emission in upconversion nano-particles are due to the lanthanide dopants localized on the lattice sites22,23. In principle, a high concentration of lanthanide dopants enhances upconversion processes as a result of an elevated capacity to sustain excitation energy2427. However, a high lanthanide content also enhances energy migration through the crystal lattice, which usually leads to a depletion of the excitation energy24,28. To minimize nonradiative energy losses, energy migration is typically inhibited by doping low concentrations of lanthanide ions27,28 or by using special host lattices24. Currently, there lacks a general approach to maximize upconversion luminescence in stoichiometric lanthanide lattices.

In this work, we describe an investigation of energy migration in a nanosized NaYbF4 lattice. We demonstrate ne tuning of energy migration through controlling the dimensions of the crystal lattice. Our mechanistic investigation reveals a spatial connement of energy migration that prevents energy loss to the crystal lattice and increases the local density of excitation energy. Through the use of Tm3 ion as an energy accumulator, the excitation energy can be maximally amassed to generate intense ultraviolet emissions on near-infrared excitation. We show that the technological advancement may revolutionize the fabrication of cost effective and compact diode-pumped solid-state deep ultraviolet lasers that are useful for environmental, life science and industrial applications29.

ResultsSynthesis and characterization. As a proof-of-concept experiment, we conned Yb3 ions in the inner shell layer of a hexagonal phase NaYF4@NaYbF4:Tm@NaYF4 host (Fig. 1a), which is known to render high upconversion efciencies3. In our study, the concentration of Tm3 was xed at 1 mol% to maximize upconversion emission in the ultraviolet region (Supplementary

Fig. 1). We did not employ a NaYbF4:Tm@NaYF4 coreshell structure because existing synthetic protocols give essentially no access to sub-10 nm b-NaYbF4 nanoparticles of a tunable particle size, which is critical prerequisite for assessing the effect of conning energy migration on upconversion. Although Yb-doped b-NaYF4 nanoparticles with small feature size can be synthesized by several complimentary methods23,30, pure b-NaYbF4 tends to form big particles (Supplementary Fig. 2a) due to rapid growth of the crystal31. Through the use of preformed NaYF4 core nanoparticle as a template, the growth of the NaYbF4 crystal can be effectively regulated, thereby offering exquisite control over the lattice dimensions (Supplementary Note 1). Note that it is also critical to enclose the Yb sublattice in an inert protection layer (that is, NaYF4) because a NaYF4@NaYbF4:Tm coreshell structure yields luminescence that is substantially weak due to surface quenching (Supplementary Fig. 2b,c).

The nanoparticles were fabricated by a layer-by-layer epitaxial growth process (Supplementary Note 1). Transmission electron microscope (TEM) images (Fig. 1b) reveal a highly uniform morphology of the nanoparticles with an average size of 38 nm. High-resolution TEM (inset of Fig. 1b) and X-ray powder diffraction (Supplementary Fig. 3) experiments conrm the single-crystalline nature of the as-synthesized nanoparticles with a hexagonal phase. To verify the formation of the multilayer structure, we intentionally doped Gd3 ions in the inner shell layer to create a contrast under electron energy loss spectroscopy analysis. The difference in the elemental distribution of Y and Gd clearly indicates the presence of multiple coreshell interfaces (Supplementary Fig. 4).

Figure 1c shows a representative upconversion emission spectrum of NaYF4@NaYbF4:Tm@NaYF4 nanoparticles on 980 nm excitation with a continuous wave (CW) laser diode at a power density of 20 W cm 2. The spectrum consists of characteristic emission peaks that can be assigned to 1I6-3H6 and 3F4 (290 and 350 nm), 1D2-3H6 and 3F4 (360 and 450 nm),

1G4-3H6 and 3F4 (475 and 650 nm) and 3H4-3H6 (800 nm) transitions of Tm3 , respectively. Both the violet and overall emissions surpass that of the NaYF4@NaYbF4:Tm/Y@NaYF4 counterparts comprising lower Yb3 contents (inset of Fig. 1c and Supplementary Figs 5 and 6). Notably, Tm3 emission at 290 nm originating from a ve-photon upconversion declined by over 45-fold when the Yb3 concentration dropped to 19 mol%, which in conventional systems typically produces the maximum emission of Tm3 ions24,28.

Connement of energy migration. We attribute the observations to conned migration of excitation energy within the nanoshells, which prevents the excitation energy from travelling a long distance at a high Yb3 concentration (99 mol%). The absence of long-distance energy migration is likely to suppress energy loss to the crystal lattice accounting for luminescence quenching. Furthermore, the localization of excitation energy raises the rate

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Figure 1 | Deep ultraviolet upconversion in coreshellshell nanoparticles. (a) Schematic design of a NaYF4@NaYbF4:Tm@NaYF4 coreshellshell nanoparticle for conning the migration of excitation energy generated in the Yb3 ions. (b) TEM image of the as-synthesized nanoparticles. Inset: high-resolution TEM image reveals single-crystalline nature of the particle. (c) Upconversion emission spectrum of the nanoparticles under 980 nm excitation (CW laser diode, 20 Wcm 2).

Inset: 2F5/2 lifetime of Yb3 , emission intensity at 290 nm and integrated emission intensity over 250850 nm range versus dopant concentration of

Yb3 , respectively. Note that the solid lines are intended to guide the eye.

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of energy transfer to a nearby Tm3 activator, which facilitates the multiphoton upconversion process.

An assessment of a series of NaYF4@NaYbF4:Tm@NaYF4 nanoparticles of varying inner shell thickness from 1 to 17 nm veried the spatial connement of energy migration (Supplementary Fig. 7). Luminescence decay studies reveal a markedly lengthened lifetime of the Yb3 by a factor of over nine with decreasing inner shell thickness from 17 to 1 nm (Supplementary Fig. 8a), conrming the suppression of energy loss to the host lattice in thin shells. In contrast, the decay time of localized Tm3 transition was only increased by less than twofold for the same series of samples (Supplementary Fig. 8b), suggesting that the defect density in the host lattice were marginally modied. Therefore, the suppressed depletion of excitation energy of Yb3 may be dominantly ascribed to the spatial connement of energy migration, which reduces the quantity of defects accessible to the Yb sublattice. In line with the reduced energy loss, we observed a steady enhancement of upconversion emission, especially the part in the 280 356 nm

range that originates from the ve-photon process, accompanied by a decrease of the inner shell thickness (Fig. 2a; Supplementary Fig. 9). The slight drop in the ratio of ve-photon upconversion to overall emission for substantially thin shells (that is, 1 and 2 nm) can be attributed to the reduced amount of Yb3 ions in the vicinity of a Tm3 activator (Fig. 2b), which limits the quantity of energy that can be captured by a Tm3 activator in a photo cycle. It is noted that the spatial connement of energy migration also plays a role in cubic phase NaYbF4:Tm (1%)@NaYF4 coreshell nanoparticles (Supplementary Fig. 10)32, implying that the geometry of the host lattice is not a formative factor in restraining the migration of excitation energy.

To shed more light on energy migration in the coreshellshell nanostructure, we calculated the probability distribution function

of excitation energy as a function of space within the Yb shell. For simplication, we assumed that the excitation energy randomly hops in the inner shell layer through the Dexter energy transfer (Supplementary Note 2). As shown in Fig. 2c, the energy migrates to smaller areas with decreasing thickness of the Yb shell from 12 to 6 and 3 nm, supporting reduced coupling of excitation energy to defects. The high probability of nding the excitation energy in a thin Yb shell further validates a favourable energy transfer to an adjacent Tm3 activator.

Lasing through upconversion. To facilitate the use of the upconversion nanoparticles as gain media for lasing applications, we further developed a Gd3 doping method for optimizing the optical properties (Supplementary Fig. 11). We used a 3-nm inner shell for the study due to a high-intensity ratio of ve-photon upconversion emission and a relatively low mass ratio of the optically inert NaYF4 layers. Gd3 ions are able to extract the excitation energy of Tm3 ions and generate a new emission peak centred at around 311 nm, owing to the reasonably matched energy levels (that is, 6P7/2 level of Gd3 and

1I6 level of Tm3 ) (Fig. 3a,b). Importantly, the large energy gap (32,200 cm 1) in Gd3 favours the preservation of the excitation energy as supported by time decay studies (Fig. 3c). The long-lived excited state contributes to high optical gains of around 150 cm 1 through ve-photon upconversion (Fig. 3d), which is comparable to that of the GaN-based semiconductor quantum wells operating in deep ultraviolet at room temperature33,34. The optical gain is also two orders of magnitude higher than that of a conventional Yb/Tm-based system operating at 650 nm through three-photon upconversion35. Moreover, efcient emission is attained at a high Gd3 concentration (30 mol%; Supplementary Fig. 12), which provides abundant

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Figure 2 | The effect of inner shell thickness on upconversion. (a) Upconversion emission intensity versus inner shell thickness (117 nm). The emission intensities were calculated by integrating the spectral intensity of the emission spectra that are normalized to the absorption of Yb3 at 980 nm.

(b) Schematic illustration showing proposed energy transfer from Yb3 to Tm3 in Yb-sublattice of varying dimensions. Note that only partial lattice sites are shown for clarication. (c) The probability of nding the excitation energy on the equatorial section of coreshellshell nanoparticles of varying inner shell thickness. With increasing inner shell thickness (from left to right panels), the energy migrates to a larger area and the probability of nding the excitation energy in the vicinity of the starting point drops signicantly.

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Figure 3 | The effect of Gd3 doping on the deep ultraviolet upconversion. (a) Simplied energy level diagram showing the energy gaps inTm3 and Gd3 activators, respectively. (b) Upconversion emission spectra of the coreshellshell nanoparticles co-doped Gd3 (30 mol%) in the inner shell layer (CW laser diode, 20 Wcm 2). (c) A comparison of the excited state lifetime between 1I6 state of Tm3 and 6P7/2 state of Gd3 in the

NaYF4@NaYbF4:Tm/Gd (1/30%)@NaYF4 coreshellshell nanoparticles. (d) Gain spectra of the nanoparticles in b as a function of excitation power (pulse laser). The inset gives the corresponding optical gain versus pump power at a wavelength of 310.5 nm. The straight line is the linear regression of the measured data. Error bars shown represent the s.d.s from ve sets of repeated measurements.

carriers to sustain optical gains at high excitation powers without saturation (Fig. 3d).

To realize lasing emission, we constructed a ve-pulse pumping scheme to excite the upconversion process (Fig. 4a). The pulse excitation scheme is primarily intended to alleviate the problems of catastrophic optical damage and the thermal effects associated with CW excitation, which terminates upconversion lasing actions. Furthermore, the ve-pulse system is advantageous over the single-pulse system for pumping the multiphoton upconversion (Supplementary Fig. 13), as a result of improved alignment with the excitation process where the absorption of photons occurs sequentially36.

The laser cavity was fabricated by coating a drop of silica resin containing the nanoparticles onto a standard optical bre. Driven by surface tension, the silica resin tends to form a bottle-like microresonator, which supports whispering gallery modes at a thin equatorial ring near the surface of the microresonator (Fig. 4b). Notably, the emission features such as mode spacing and threshold pump power of the microresonator can be readily tuned by controlling the diameter (Dm) of the resonator (Fig. 4b)37,38, which provides a general platform for assessing the optical characteristics of the upconversion nanoparticles.

We validated the lasing action by measuring the optical emission in a typical microresonator (Dm 75 mm) under

excitation of varying powers at room temperature. The light inputoutput curve shown in Fig. 4c exhibits a well-dened nonlinear excitation power-dependent behaviour with three distinct regions separated by two threshold pump powers (that is, Pa B78 mJ cm 2 and Pth B86 mJ cm 2). This S-like

spectrum clearly indicates a transition from a spontaneous emission to an amplied spontaneous emission and to a lasing emission. Figure 4d shows the corresponding emission spectra under various pumping powers. At low pump power (oPa), a relatively broad spontaneous band is observed. As the excitation power increases slightly above Pa, a sharp peak ascends from the emission spectrum. Through further increases in the excitation power above Pth, well-dened sharp peaks with a linewidth o0.11 nm emerge from the spectrum. The measured mode spacing (0.25 0.27 nm) is in good agreement with the

theoretical value (B0.26 nm), conrming that lasing emissions have been achieved. Notably, single-mode lasing was also obtained by using a thinner microresonator (Dm 20 mm;

Fig. 4e). The single-mode emission is a result of a relatively large mode spacing (B1.0 nm) with respect to the full width at half maximum of the resonant frequency. This narrow gain bandwidth is a unique signature of the upconversion nanoparticles and unlikely to be realized from semiconductor nanostructures. The Q factor, which is dened as the ratio of

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Figure 4 | Upconversion lasing characteristics of the microresonator. (a) Schematic diagram of the optical set-up for the ve-pulse excitation scheme. (b) Plots of measured Dl and Pth of the microresonator as a function of Dm. The red and black lines are tted and calculated curves, respectively. The insets show photographs of the microresonator with and without optical excitation. Df and Dm denote the diameters of the bre and microcavity, respectively. (c) Logarithmic plot of output intensity versus excitation power of a microresonator with Dm 75 mm. The red line is tted curve. (d) The corresponding

lasing spectra at different excitation power (Dm 75 mm). (e) Single mode lasing spectra measured from a microresonator with Dm 20 mm.

the resonant frequency to its full width at half maximum, was estimated to be B2,800, revealing the high quality of the upconversion-based laser system. It is also worth noting that the lasing emission can be readily extended to violet and blue spectral regions with the same upconversion nanoparticles (Supplementary Fig. 14).

DiscussionOur investigation of energy migration in nanostructured hosts highlights an innovative strategy to manipulating optical transitions in lanthanide-doped upconversion nanoparticles. In addition, it initiates a novel tactic to obtain effective upconversion laser materials in deep ultraviolet regime with very narrow optical gain bandwidth to support single-mode excitation. Emission, in principle, can be tuned to shorter wavelengths (that is, well below 300 nm) by further rening the upconversion process. Hence, our study will lead to the development of near-infrared diode-pumped deep ultraviolet lasers which can avoid the difculty of shifting the operating wavelength of GaN-based laser diodes below 300 nm (ref. 39), evade using nonlinear optical crystal that requires tight control in optical alignment, antireective coating and environmental control and adopt inexpensive Q-switched near-infrared diode as the pumping source to construct compact, deep ultraviolet lasers for unexplored applications in the elds of information technology, biomedicine and biophotonics.

Methods

Nanoparticle synthesis. We synthesized the coreshellshell nanoparticles using the method described in ref.16. Additional experimental details are provided in the Supplementary Note 1.

Optical gain measurement. Net optical gain of the nanoparticle colloid was measured using variable stripe length method40. The longer side of a quartz cuvette lled with nanoparticle colloid was excited by a pump stripe with width and length of B30 mm and L, respectively in the orientation perpendicular to the length of the cuvette. Photoluminescence intensity emitted from the shorter side of the cuvette, Itot(l), was recorded by the monochromator set-up. The net optical gain, G(l), was deduced by tting Itot (L, l) Isp(l) [exp(G(l)L) 1]/G(l) with the measured

values of Itot(l), where l is the wavelength and Isp(l) is the spontaneous emission intensity.

Five-pulse excitation scheme. The optical set-up consists of a Powerlite DLS 9010 Q-switched Nd:YAG laser and a continuum Panther EX optical parametric oscillator. A 980-nm laser pulse (6 ns, 10 Hz) with a diameter of B10 mm was generated from the optical parametric oscillator system under the excitation of the Nd:YAG laser. By splitting the 980-nm pulse into ve equal-power pulses through the use of four beam splitters (that is, one 80/20 and three 50/50 beam splitters), we can obtain a ve-pulse (time delay between adjacent pulses is 10 ns) laser beam. This is possible because the pulses are forced to travel in ve different distances to obtain a time delay of 10 ns between the adjacent pulses. These ve pulses are then combined through two polarization-dependent beam splitters and two l/2 waveplates to form three laser beams. All the laser beams, which are spatially overlapped, are focussed onto a sample through three cylindrical lenses to form a pump stripe of width equal to B30 mm. Photoluminescence emission from the sample was collected and analysed by an optical bre (core diameter of 400 mm) coupled to an Oriel MS257 monochromator attached with a photomultiplier tube. The spectral resolution of the monchromator is about 0.1 nm.

Fabrication and excitation of microresonators. For the fabrication of the bottle-like microresonator, a bared standard optical bre was coated with a tiny drop of nanoparticles and silica resin mixture. The prolate surface-tention-induced microresonator was then solidied in an arid and clean atmosphere. The surrounding temperature of the sample was kept at 23 C to avoid deformation due to the inuence of thermal effects. Whispering gallery modes can be excited by optically pumping the equatorial zone of the microresonator. Notably, the pump stripe is oriented perpendicular to the length of the bre. Light emitted from the surface of the microresonator can be collected through an optical bre.

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Acknowledgements

This work was supported by the Research Grants Council of Hong Kong (CityU 109413, 21300014 and PolyU 153036/14P) and the National Natural Science Foundation of China (Nos. 21303149, 51332008 and 21403182).

Author contributions

X.C., L.J., S.F.Y. and F.W. conceived the project and wrote the paper. X.C., W.K., T.S. andF.W synthesized and characterized the nanoparticles. L.J., W.Z. and S.F.Y. fabricated and tested the lasers. X.L. and J.F. solved the probability of nding the excitation energy. All authors contributed to the analysis of this manuscript.

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How to cite this article: Chen, X. et al. Conning energy migration in upconversion nanoparticles towards deep ultraviolet lasing. Nat. Commun. 7:10304doi: 10.1038/ncomms10304 (2016).

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