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Optics Express

Optics Express

  • Editor: Andrew M. Weiner
  • Vol. 21, Iss. 10 — May. 20, 2013
  • pp: 12635–12642
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Intense ultra-broadband down-conversion in co-doped oxide glass by multipolar interaction process

Zijun Liu, Luyun Yang, Nengli Dai, Yingbo Chu, Qiaoqiao Chen, and Jinyan Li  »View Author Affiliations


Optics Express, Vol. 21, Issue 10, pp. 12635-12642 (2013)
http://dx.doi.org/10.1364/OE.21.012635


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Abstract

We report that Eu2+ can be an efficient sensitizer for Yb3+ and a broadband absorber for blue solar spectra in the host of oxide glass. The greenish 4f→5d transition of Eu2+ and the characteristic near-infrared emission of Yb3+ were observed, with the blue-light of xenon lamp excitation. The 5d energy can be adjusted by the host and the energy transfer efficiency can be enhanced. The quantum efficiency is up to 163.8%. Given the broad excitation band, high absorption coefficient and excellent mechanical, thermal and chemical stability, this system can be useful as down-conversion layer for solar cells.

© 2013 OSA

1. Introduction

Although, QC phosphors via DC have been investigated for decades for their use in the lighting and display industry, only recently DC through a cooperative energy transfer (ET) process has attracted growing attention in enhance the efficiency of photovoltaic cells [2

2. Q. Y. Zhang and X. Y. Huang, “Recent progress in quantum cutting phosphors,” Prog. Mater. Sci. 55(5), 353–427 (2010). [CrossRef]

, 7

7. D. Chen, Y. Wang, Y. Yu, P. Huang, and F. Weng, “Near-infrared quantum cutting in transparent nanostructured glass ceramics,” Opt. Lett. 33(16), 1884–1886 (2008). [CrossRef] [PubMed]

10

10. K. Deng, X. Wei, X. Wang, Y. Chen, and M. Yin, “Near-infrared quantum cutting via resonant energy transfer from Pr3+ to Yb3+ in LaF3,” Appl. Phys. B: Lasers O, 1–4 (2011).

]. The most widely used solar cells are based on crystalline silicon (Si). The thermalization of electron–hole pairs, generated by the absorption of high-energy photons, is one of the major energy loss mechanisms in a conventional solar cell [2

2. Q. Y. Zhang and X. Y. Huang, “Recent progress in quantum cutting phosphors,” Prog. Mater. Sci. 55(5), 353–427 (2010). [CrossRef]

, 11

11. V. D. Rodríguez, V. K. Tikhomirov, J. Méndez-Ramos, A. C. Yanes, and V. V. Moshchalkov, “Towards broad range and highly efficient down-conversion of solar spectrum by Er3+-Yb3+ co-doped nano-structured glass-ceramics,” Sol. Energy Mater. Sol. Cells 94(10), 1612–1617 (2010). [CrossRef]

]. Thermalization losses can be reduced by using DC whereby, for example, a photon with twice the energy of the band gap transforms into two photons with energy is just above the band gap of a single junction Si (Eg = 1.12 eV, 1100 nm). Theoretically, for a single junction Si-based solar cell in conjunction with an ideal DC layer, the conversion efficiency can be up to 40%, which is a significant improvement over the limiting efficiency of 30.9% for conventional solar cells [6

6. J. Zhou, Y. Teng, S. Ye, X. Liu, and J. Qiu, “Broadband down-conversion spectral modification based on energy transfer,” Opt. Mater. 33(2), 153–158 (2010). [CrossRef]

11

11. V. D. Rodríguez, V. K. Tikhomirov, J. Méndez-Ramos, A. C. Yanes, and V. V. Moshchalkov, “Towards broad range and highly efficient down-conversion of solar spectrum by Er3+-Yb3+ co-doped nano-structured glass-ceramics,” Sol. Energy Mater. Sol. Cells 94(10), 1612–1617 (2010). [CrossRef]

].

Ion pairs of Re3+-Yb3+ (Re = Tb, Pr, Er or Tm) have been demonstrated with optical spectroscopy for cooperative DC in various hosts, including glasses and crystalline phosphors [2

2. Q. Y. Zhang and X. Y. Huang, “Recent progress in quantum cutting phosphors,” Prog. Mater. Sci. 55(5), 353–427 (2010). [CrossRef]

, 8

8. Y. Xu, X. Zhang, S. Dai, B. Fan, H. Ma, J. Adam, J. Ren, and G. Chen, “Efficient Near-Infrared Down-Conversion in Pr3+–Yb3+ Codoped Glasses and Glass Ceramics Containing LaF3 Nanocrystals,” J. Phys. Chem. C 115(26), 13056–13062 (2011). [CrossRef]

, 11

11. V. D. Rodríguez, V. K. Tikhomirov, J. Méndez-Ramos, A. C. Yanes, and V. V. Moshchalkov, “Towards broad range and highly efficient down-conversion of solar spectrum by Er3+-Yb3+ co-doped nano-structured glass-ceramics,” Sol. Energy Mater. Sol. Cells 94(10), 1612–1617 (2010). [CrossRef]

, 12

12. Q. Y. Zhang, G. F. Yang, and Z. H. Jiang, “Cooperative downconversion in GdAl3 (BO3) 4: RE3+, Yb3+ (RE= Pr, Tb, and Tm),” Appl. Phys. Lett. 91(5), 051903 (2007). [CrossRef]

]. However, these DC materials are still far from practical application, because the absorption of the sensitizer ion (Tb3+, Pr3+, Er3+ or Tm3+) arises from the parity-forbidden 4f-4f transitions, which are naturally weak in intensity and narrow in bandwidth. On the contrary, Eu2+ ion might be an ideal broadband sensitizer for Yb3+, as its 4f-5d transition covers a broad spectral range and more importantly, the energy of its 4f-5d transitions can be tuned by changing the crystal field strength as well as the covalency of the host [13

13. J. Zhou, Y. Teng, X. Liu, Z. Ma, and J. Qiu, “Broadband spectral conversion of visible light to near-infrared emission via energy transfer from Ce3+ to Nd3+/Yb3+ in YAG,” J. Mater. Res. 26(05), 689–692 (2011). [CrossRef]

, 14

14. Z. Liu, Y. Yu, N. Dai, Q. Chen, L. Yang, J. Li, and Y. Qiao, “Super Broadband Reddish Emitting Glass with Eu 2+ Doped for Warm-White Light-Emitting Diodes,” Appl. Phys., A Mater. Sci. Process. 108(4), 777–781 (2012). [CrossRef]

].

In the present work, we chose the low silica calcium aluminosilicate glass (LSCAS) as the host lattice, which have high concentration quenching limit [14

14. Z. Liu, Y. Yu, N. Dai, Q. Chen, L. Yang, J. Li, and Y. Qiao, “Super Broadband Reddish Emitting Glass with Eu 2+ Doped for Warm-White Light-Emitting Diodes,” Appl. Phys., A Mater. Sci. Process. 108(4), 777–781 (2012). [CrossRef]

17

17. L. G. Hwa, S. L. Hwang, and L. C. Liu, “Infrared and Raman spectra of calcium alumino-silicate glasses,” J. Non-Cryst. Solids 238(3), 193–197 (1998). [CrossRef]

]. The host is proper for Eu2+, in which the energy of the 4f-5d transition of Eu2+ locate in the visible region and matches well with the twice energy of the 2F5/22F7/2 transition of Yb3+. Besides, the absorption region also matches the high-energy part of the solar spectrum well. Therefore, the Eu2+-Yb3+ dual ions combination is a promising system to realize NIR QC, and we observed ET from Eu2+ to Yb3+ by a cooperative process.

2. Experiment

The compositions of the host used in this experiment were 8%SiO2-58%CaO-27%Al2O3-7%MgO in mole percentage. The Eu2+-Yb3+ doped glasses are referred to as LSCAS:Eu,Yb. Analytical reagent of SiO2, CaCO3, Al2O3, MgCO3, Eu2O3, and Yb2O3 were used as starting materials. Detailed glass-preparation procedure was described as follows. The homogenously mixed batch with 20g was melted at 1480°C in a graphite crucible for 2 hours in vacuum atmosphere. The glass melt was poured on the pre-heated steel mold and then annealed for 2 hours near the glass transition temperature to enhance the mechanical property by releasing the stress induced during the quenching process. Finally the samples were then cut into 15mm × 15mm × 1.5mm sizes and polished for optical measurements.

3. Results and discussion

Part of the energy-level diagram of Eu2+ and Yb3+ in LSCAS glass is shown in Fig. 1
Fig. 1 Schematic energy-level diagram of LSCAS: Eu2+,Yb3+ shows the concept of NIR QC with visible excitation at 405nm.
to illustrate the possible cooperative ET from Eu2+ to Yb3+. In this system Eu2+ was doped as a sensitizer and Yb3+ was doped as an activator, whereby to convert one visible photon into two NIR photons. The doped Eu2+ ions absorb energy from the excitation source and are excited to the 4f65d1 level. Then, parts of the energy of the Eu2+ ions are relaxed to the split excited state, along with a Stokes-shift. The emission occurs in terms of the parity-allowed transition from the excited state to the ground state (4f7). Meanwhile, another part of the Eu2+ ions releases the energy absorbed by activating two NIR photons due to the Yb3+:2F5/22F7/2 transitions. The Eu2+:4f-5d transition is located at approximately twice the energy of the Yb3+:2F5/2-2F7/2 transition and Yb3+ has no other levels up to the UV region [2

2. Q. Y. Zhang and X. Y. Huang, “Recent progress in quantum cutting phosphors,” Prog. Mater. Sci. 55(5), 353–427 (2010). [CrossRef]

, 8

8. Y. Xu, X. Zhang, S. Dai, B. Fan, H. Ma, J. Adam, J. Ren, and G. Chen, “Efficient Near-Infrared Down-Conversion in Pr3+–Yb3+ Codoped Glasses and Glass Ceramics Containing LaF3 Nanocrystals,” J. Phys. Chem. C 115(26), 13056–13062 (2011). [CrossRef]

10

10. K. Deng, X. Wei, X. Wang, Y. Chen, and M. Yin, “Near-infrared quantum cutting via resonant energy transfer from Pr3+ to Yb3+ in LaF3,” Appl. Phys. B: Lasers O, 1–4 (2011).

]. Therefore, there would not be resonant radiation transfer, resonant non-radiation transfer or cross relaxation transfer. Non-resonant ET maybe takes place by the assist of phonons. While the low phonon property of the host and the large difference band gap between the ground and excited states of Eu2+ and Yb3+ makes phonon assist non-resonant ET negligible. Therefore, the cooperative DC process may become the dominant relaxation process in this system, which is opposite to the UC phenomenon [18

18. P. Vergeer, T. J. H. Vlugt, M. H. F. Kox, M. I. den Hertog, J. P. J. M. van der Eerden, and A. Meijerink, “Quantum cutting by cooperative energy transfer in YbxY1−xPO4:Tb3+,” Phys. Rev. B 71(1), 014119 (2005). [CrossRef]

].

The emission band of Eu2+ ion is due to the 5d→4f transition which can vary from long-wavelength ultraviolet to yellow by choosing different glass matrix. The host lattice influence on the emission color of the Eu2+ ion is mainly determined by several factors such as covalency effect and crystal field effect [14

14. Z. Liu, Y. Yu, N. Dai, Q. Chen, L. Yang, J. Li, and Y. Qiao, “Super Broadband Reddish Emitting Glass with Eu 2+ Doped for Warm-White Light-Emitting Diodes,” Appl. Phys., A Mater. Sci. Process. 108(4), 777–781 (2012). [CrossRef]

]. The influence of the surroundings on Eu2+ ion is expected to be large indeed, despite the 4f electrons are well shielded from the surroundings by completely filled 5s and 5p orbits, however the 5d electrons of Eu2+ are exposed to the surroundings and the influence is large [3

3. G. Blasse and B. C. Grabmaier, Luminescent Materials. Berlin: Springer, (1994).

,14

14. Z. Liu, Y. Yu, N. Dai, Q. Chen, L. Yang, J. Li, and Y. Qiao, “Super Broadband Reddish Emitting Glass with Eu 2+ Doped for Warm-White Light-Emitting Diodes,” Appl. Phys., A Mater. Sci. Process. 108(4), 777–781 (2012). [CrossRef]

]. If the crystal field is strong and the amount of covalency high, the lowest component of the 4f65d configuration of the Eu2+ ion may shift to some low energy level, that the excitation source have a red-shift and the absorption band focus much more energy on the blue range. And the energy difference between Eu2+ excited state and twofold Yb3+ excited state will become much smaller with the redshift of Eu2+ excited state. The smaller the difference the bigger the ET efficiency will be. Therefore, the Eu2+-Yb3+ co-doped LSCAS glass have potential advantage for solar cells down-conversion layer.

Figure 2
Fig. 2 Absorption of the matrix glass and the Eu2+-Yb3+ co-doped glass.
compares the absorption spectra of un-doped and co-doped glasses. The curve b is the net absorption of rare-earth ions without the influence of host. It shows that the matrix glass has no absorption except the UV absorption sideband. The broadband absorption peak from 300nm to 500nm is due to Eu2+ ions. The intrinsic absorption of Eu3+ at 394nm cannot be observed here. The infrared peaks are the Yb3+ ions absorption. Since the Eu2+ ions are the main absorbers and sensitizers. Besides, there is no apparent effect of Eu3+ ions on IR luminescence from Yb3+ ions. Thus we focus the discussion on the effect of Eu2+ ions. The ion valence in glass can be tuned by varying the reducing atmosphere in the melting process, tuning the optical basicity of the host and adding reducing agent. In this work, the vacuum atmosphere is good enough to maintain the europium valence. It is obviously, this material has excellent transmission efficiency in the visible and infrared region. Thus it can be made into DC layer and covered at solar cells front surface.

Figure 3
Fig. 3 Excitation spectra of Eu2+-Yb3+ co-doped samples monitored at 600nm and 980nm compared in Fig. 3. And the visible and near infrared emission spectra of Eu2+-Yb3+ co-doped borosilicate glasses excited by 405nm are shown in Fig. 3. The Eu2+ fixed concentration is 0.2mol% and Yb3+ varied concentration are 0.2, 0.4 and 0.6mol% for sample a, b and c, respectively.
presents the excitation spectra of LSCAS:Eu2+,Yb3+. It can be seen from Fig. 3 that the excitation spectra shape monitored the Yb3+ emission at 980nm and the Eu2+ emission at 460nm matches quite well. This similarity in the shape of the excitation spectra can be considered as direct evidence of ET from Eu2+ to Yb3+. Besides, there is no absorption transition for Yb3+ ion in blue range. The broad peak ranging from 300nm to 500nm is ascribed to the first allowed 4f-5d transition of Eu2+ [13

13. J. Zhou, Y. Teng, X. Liu, Z. Ma, and J. Qiu, “Broadband spectral conversion of visible light to near-infrared emission via energy transfer from Ce3+ to Nd3+/Yb3+ in YAG,” J. Mater. Res. 26(05), 689–692 (2011). [CrossRef]

, 14

14. Z. Liu, Y. Yu, N. Dai, Q. Chen, L. Yang, J. Li, and Y. Qiao, “Super Broadband Reddish Emitting Glass with Eu 2+ Doped for Warm-White Light-Emitting Diodes,” Appl. Phys., A Mater. Sci. Process. 108(4), 777–781 (2012). [CrossRef]

]. This broad excitation band indicates that the glasses are suitable for excitation by blue and violet sun light.

The Eu2+-Yb3+ dual ions combination is one of the promising systems to realize NIR QC, since the Eu2+ ion 4f-5d transition is located at approximately twofold the energy of the Yb3+ 2F7/2-2F5/2 transition (~1000 nm). Moreover, the 2F5/2-2F7/2 emission is just above the band-gap energy of Si solar cells. It will be favorable to increase the solar cell conversion efficiency.

Figure 3 also shows the visible and NIR photoluminescence emission spectra of LSCAS: Eu2+,Yb3+ glasses. Excited by 405nm lights these samples gave rise to emission both from Eu2+ and Yb3+ ions. The emission spectrum ranging from 460nm to 780nm is due to the 5d-4f transition of Eu2+. The 5D0-7F1,2 emission of Eu3+ ions was totally covered by the strong emission of Eu2+. The Eu3+ concentration is nearly negligible compared to Eu2+ concentration.

It is also noticed that, from sample (a) to sample (c), the emission intensity of Eu2+ at 600nm decreases monotonically, while the intensity of the NIR emission at 980nm increases rapidly with increasing Yb3+ concentration. This phenomenon proved the ET rate of this process strongly depends on the ions distance. In the case of the Eu2+ and Yb3+ system with the Yb3+ concentration increase, the distance between Eu2+ and Yb3+ decreased, which alleviate the ET efficiency and Yb3+ emission. In addition, this also facilitates to form ions group with one Eu2+ ion and two Yb3+ ions, that is to say the probability of Eu2+ donor have two Yb3+ acceptors in critical distance increased. Using the Dexter’s theory the ET rate can be expressed as a function of the distance between donor and acceptor, so that the ET probability depends upon the distance between donor and acceptor. The distance dependence varies with the interaction type. For exchange interaction it is exponential, while it is of the type R-n (where R is the distance between donor and acceptor) for the multipolar interaction. Therefore, the ET efficiency and the QE rose with the increased Yb3+ concentration [3

3. G. Blasse and B. C. Grabmaier, Luminescent Materials. Berlin: Springer, (1994).

5

5. Z. Liu, N. Dai, H. Luan, Y. Sheng, J. Peng, Z. Jiang, H. Li, L. Yang, and J. Li, “Enhanced green luminescence in Ce-Tb-Ca codoped sintered porous glass,” Opt. Express 18(20), 21138–21146 (2010). [CrossRef] [PubMed]

].

Figure 4
Fig. 4 The blue background is the solar spectrum (AM1.5G) in visible and NIR region. The white slash area is the maximum fraction available for DC. The curves a, b, and c are spectral response of single junction Si, excitation spectrum monitored at 980nm and IR emission spectrum excited at 400nm of our Eu2+-Yb3+ co-doped sample, respectively.
shows the global solar spectrum (AM1.5G, blue background), the spectral response of Si solar cells (a), the excitation spectrum of Yb3+ at 980nm (b) and the IR emission spectrum excited at 405nm (c). As the shown in Fig. 4 the single junction Si solar cells photoelectric transformation efficiency is the highest near the band gap (1.1 eV). While the response become weak in the high energy region, due to thermalization loss. Especially in the 300nm–500nm region, while the solar spectrum is still very strong. Therefore, the excitation spectrum monitored at NIR emission of DC material should located in the above mentioned region as shown in curve (b). The curve (c) in Fig. 4 is the NIR emission, which matches quite well with the response spectrum of Si. By using the glasses developed in this work, the broad region 300nm–500nm light can be converted to around 1000nm, where the response is highest. This process was realized by the second-order DC mechanism. In general one photon with twice the energy of the Si band gap absorbed by Eu2+ ions, and then transfers the energy simultaneously to two Yb3+ ions with the emission of exactly the energy of the Si solar cell band gap, resulting in a great improvement in conversion efficiency of Si solar cells.

Assuming that the interaction is multipolar type and no migration takes place, the Eu2+ decay curves could be analyzed using the well-known direct quenching mechanism. There is no energy migration effect or less energy migration effect in the 5d level because it is obviously suppressed by faster relaxation. Usually, the interaction scheme involves both the dipole-dipole and the dipole-quadrupole interactions, which can be described by Inokuti-Hirayama formula [3

3. G. Blasse and B. C. Grabmaier, Luminescent Materials. Berlin: Springer, (1994).

5

5. Z. Liu, N. Dai, H. Luan, Y. Sheng, J. Peng, Z. Jiang, H. Li, L. Yang, and J. Li, “Enhanced green luminescence in Ce-Tb-Ca codoped sintered porous glass,” Opt. Express 18(20), 21138–21146 (2010). [CrossRef] [PubMed]

]. The rare earth ions doped in oxide glass tend to accumulate, therefore the concentration of rare-earth ions is different everywhere. Thus parts of Eu2+ ions doped in oxide glass clustered and these ions have no or less contribution to the emission. The non-clustered Eu2+ ions can efficiently emit fluorescence, and can be classified into two types due to the distance from Eu2+ to Yb3+ ions, one isolated and with no interaction with Yb3+ ions, another with energy transfer by multipolar interaction. Therefore, the fluorescence from the former should decay exponentially and the latter should decay according to Inokuti-Hirayama formula. So the resultant fitting equation could be formulated as [3

3. G. Blasse and B. C. Grabmaier, Luminescent Materials. Berlin: Springer, (1994).

]:
I(t)=Aexp(tτ0)+(1A)exp[tτ0π(CC0)(tτ0)12]
(1)
The fitting equation consists of the emission without ET and the emission taking account of the ET. Where, A is the contributive parameter; t0 is the intrinsic lifetime of a single ion (1.2μs for our samples measured for a sample with very low Eu2+ concentration of 0.05mol%); C is the number of acceptors per unit volume; C0−1 is the volume of donor’s sphere of influence ( = 4πR03/3, R0 is the critical separation between donor and acceptor, at which the nonradiative rate equals that of the internal single ion relaxation); the ratio of C/C0 means the number of acceptors in donor’s sphere of influence. The fitted curves are depicted in Fig. 5
Fig. 5 Decay curves of the Eu2+ 5d-4f emission (600nm) in the LSCAS glasses with 405nm excitation. The red lines are the fitted decay curves. The concentration of Yb3+ is 0.2mol% (a), 0.4mol% (b) and 0.6mol% (c), respectively. The fixed Eu2+ concentration is 0.2mol%.
and the contributive parameter A values and the resultant C/C0 values are given in Table 1

Table1. Parameters for the fitted equation, decay life time, energy transfer efficiency and quantum efficiency of samples with different Yb3+ concentration.

table-icon
View This Table
. The overall fitting result shows that the analysis using the multipolar interaction scheme produces a relatively good fit between the theoretical calculation and the measured data. From the Table 1, it is shown that the contributive parameter A gradually decrease with the increasing of Yb3+ concentration which means that the increased Yb3+ concentration facilitated the ET. The ratio of C/C0 has an increasing tendency with increased Yb3+ concentration. C is the number of acceptors per unit volume, that is, Yb3+ concentration. Furthermore, we calculated the mean lifetime (τm) and the energy transfer efficiency (ηET) as follows [4

4. L. Yang, N. Dai, Z. Liu, Z. Jiang, J. Peng, H. Li, J. Li, M. Yamashita, and T. Akai, “Tailoring of clusters of active ions in sintered nanoporous silica glass for white light luminescence,” J. Mater. Chem. 21(17), 6274–6279 (2011). [CrossRef]

]:
τm=0I(t)tdt/0I(t)dt
(2)
and
ηET=1τmxYb/τ0
(3)
where I(t) is the luminescence intensity as a function of time t. The energy transfer efficiency ηET is defined as the ratio of donors that are depopulated by energy transfer to the acceptors over the total number of donors being excited. In our system, the Eu2+ acts as the donor and Yb3+ as the acceptor. By dividing the mean lifetime of the 5d emission of Eu2+ doped glass over the Yb3+ free glass, the transfer efficiency is obtained as a function of Yb3+ concentration. The total QE (ηQE) could be defined as the ratio of the number of photons emitted to the number of photons absorbed, assuming that all excited Yb3+ ions decay radiatively. This assumption leads to an upper limit of QE. The relation between the ET efficiency and the total QE is defined as [5

5. Z. Liu, N. Dai, H. Luan, Y. Sheng, J. Peng, Z. Jiang, H. Li, L. Yang, and J. Li, “Enhanced green luminescence in Ce-Tb-Ca codoped sintered porous glass,” Opt. Express 18(20), 21138–21146 (2010). [CrossRef] [PubMed]

9

9. K. Deng, T. Gong, L. Hu, X. Wei, Y. Chen, and M. Yin, “Efficient near-infrared quantum cutting in NaYF4: Ho3+, Yb3+ for solar photovoltaics,” Opt. Express 19(3), 1749–1754 (2011). [CrossRef] [PubMed]

]:

ηQE=ηEu(1ηET)+2ηET=1+ηET
(4)

It is very interesting to note that the ratio of C/C0 nearly equates to the concentration ratio of Yb3+/Eu2+. The C/C0 means the number of acceptors in donor’s sphere of influence, in this work that is the numbers of Yb3+ in a Eu2+ around. And this proved our hypothesis about the ions group formation with one Eu2+ ion and two Yb3+ ions, when the Yb3+ concentration increase.

In summary, Eu2+–Yb3+ co-doped LSCAS glasses were investigated as a downconversion layer candidate to enhance silicon solar cell efficiency. Excitation and emission measurements indicate the occurrence of cooperative energy transfer from Eu2+ to Yb3+ ions. The maximum value of QE approaches 163.8% in this work. The results show efficient conversion of broad 300nm–500nm light, which is not fully utilized by the existed solar cells, to 1000nm IR light, which can be efficiently absorbed by silicon solar cell and converted into electric energy. In addition, the excitation and luminescence due to f-d transition of Eu2+ is determined by the ligand field around Eu2+, it is possible to modify the excitation spectrum which fits well with solar spectrum below 500nm through controlling glass matrix. Besides, the modification of glass matrix can also raise the NBOs number, then decrease CQ effect, shorten ions distance, heighten ET efficiency and further promote QE. Our approach may open an effective way for the realization of efficient spectral modification of solar spectrum.

4. Conclusions

In conclusion, the LSCAS glasses impregnated with Eu2+ and Yb3+ ions were successfully prepared as efficient visible to NIR converters. Luminescence spectra, excitation spectra and quantum efficiency of Eu2+-Yb3+ co-doped glasses were measured and studied. The decay curves were well fitted and the energy transfer process was considered to be multipolar interaction. It is suggested that this dual ions system is one of the most efficient NIR DC systems. In view of their strong and broadband absorption in the range of 300nm-500nm and the efficient NIR emission, the DC glass system has a potential application in solar cell as DC phosphor converter layer.

Acknowledgments

This work was supported by “the National High-Technology Research and Development Program of China” (2013AA031501) and “Supported by Specialized Research Fund for the Doctoral Program of Higher Education” (SRFDP, No: 20110142120092). We would also like to thank the Hubei Optoelectronics Testing Center and Huazhong University of Science and Technology Analytical and Testing Center for sharing their equipments.

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2.

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3.

G. Blasse and B. C. Grabmaier, Luminescent Materials. Berlin: Springer, (1994).

4.

L. Yang, N. Dai, Z. Liu, Z. Jiang, J. Peng, H. Li, J. Li, M. Yamashita, and T. Akai, “Tailoring of clusters of active ions in sintered nanoporous silica glass for white light luminescence,” J. Mater. Chem. 21(17), 6274–6279 (2011). [CrossRef]

5.

Z. Liu, N. Dai, H. Luan, Y. Sheng, J. Peng, Z. Jiang, H. Li, L. Yang, and J. Li, “Enhanced green luminescence in Ce-Tb-Ca codoped sintered porous glass,” Opt. Express 18(20), 21138–21146 (2010). [CrossRef] [PubMed]

6.

J. Zhou, Y. Teng, S. Ye, X. Liu, and J. Qiu, “Broadband down-conversion spectral modification based on energy transfer,” Opt. Mater. 33(2), 153–158 (2010). [CrossRef]

7.

D. Chen, Y. Wang, Y. Yu, P. Huang, and F. Weng, “Near-infrared quantum cutting in transparent nanostructured glass ceramics,” Opt. Lett. 33(16), 1884–1886 (2008). [CrossRef] [PubMed]

8.

Y. Xu, X. Zhang, S. Dai, B. Fan, H. Ma, J. Adam, J. Ren, and G. Chen, “Efficient Near-Infrared Down-Conversion in Pr3+–Yb3+ Codoped Glasses and Glass Ceramics Containing LaF3 Nanocrystals,” J. Phys. Chem. C 115(26), 13056–13062 (2011). [CrossRef]

9.

K. Deng, T. Gong, L. Hu, X. Wei, Y. Chen, and M. Yin, “Efficient near-infrared quantum cutting in NaYF4: Ho3+, Yb3+ for solar photovoltaics,” Opt. Express 19(3), 1749–1754 (2011). [CrossRef] [PubMed]

10.

K. Deng, X. Wei, X. Wang, Y. Chen, and M. Yin, “Near-infrared quantum cutting via resonant energy transfer from Pr3+ to Yb3+ in LaF3,” Appl. Phys. B: Lasers O, 1–4 (2011).

11.

V. D. Rodríguez, V. K. Tikhomirov, J. Méndez-Ramos, A. C. Yanes, and V. V. Moshchalkov, “Towards broad range and highly efficient down-conversion of solar spectrum by Er3+-Yb3+ co-doped nano-structured glass-ceramics,” Sol. Energy Mater. Sol. Cells 94(10), 1612–1617 (2010). [CrossRef]

12.

Q. Y. Zhang, G. F. Yang, and Z. H. Jiang, “Cooperative downconversion in GdAl3 (BO3) 4: RE3+, Yb3+ (RE= Pr, Tb, and Tm),” Appl. Phys. Lett. 91(5), 051903 (2007). [CrossRef]

13.

J. Zhou, Y. Teng, X. Liu, Z. Ma, and J. Qiu, “Broadband spectral conversion of visible light to near-infrared emission via energy transfer from Ce3+ to Nd3+/Yb3+ in YAG,” J. Mater. Res. 26(05), 689–692 (2011). [CrossRef]

14.

Z. Liu, Y. Yu, N. Dai, Q. Chen, L. Yang, J. Li, and Y. Qiao, “Super Broadband Reddish Emitting Glass with Eu 2+ Doped for Warm-White Light-Emitting Diodes,” Appl. Phys., A Mater. Sci. Process. 108(4), 777–781 (2012). [CrossRef]

15.

P. L. Higby, R. J. Ginther, I. D. Aggarwal, and E. J. Friebele, “Glass formation and thermal properties of low-silica calcium aluminosilicate glasses,” J. Non-Cryst. Solids 126(3), 209–215 (1990). [CrossRef]

16.

L. Andrade, S. M. Lima, A. Novatski, A. Steimacher, J. H. Rohling, A. N. Medina, A. C. Bento, M. L. Baesso, Y. Guyot, and G. Boulon, “A step forward toward smart white lighting: Combination of glass phosphor and light emitting diodes,” Appl. Phys. Lett. 95(8), 081104 (2009). [CrossRef]

17.

L. G. Hwa, S. L. Hwang, and L. C. Liu, “Infrared and Raman spectra of calcium alumino-silicate glasses,” J. Non-Cryst. Solids 238(3), 193–197 (1998). [CrossRef]

18.

P. Vergeer, T. J. H. Vlugt, M. H. F. Kox, M. I. den Hertog, J. P. J. M. van der Eerden, and A. Meijerink, “Quantum cutting by cooperative energy transfer in YbxY1−xPO4:Tb3+,” Phys. Rev. B 71(1), 014119 (2005). [CrossRef]

OCIS Codes
(160.2750) Materials : Glass and other amorphous materials
(260.2160) Physical optics : Energy transfer
(300.6340) Spectroscopy : Spectroscopy, infrared
(350.6050) Other areas of optics : Solar energy

ToC Category:
Solar Energy

History
Original Manuscript: March 22, 2013
Revised Manuscript: May 8, 2013
Manuscript Accepted: May 8, 2013
Published: May 15, 2013

Citation
Zijun Liu, Luyun Yang, Nengli Dai, Yingbo Chu, Qiaoqiao Chen, and Jinyan Li, "Intense ultra-broadband down-conversion in co-doped oxide glass by multipolar interaction process," Opt. Express 21, 12635-12642 (2013)
http://www.opticsinfobase.org/oe/abstract.cfm?URI=oe-21-10-12635


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References

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  11. V. D. Rodríguez, V. K. Tikhomirov, J. Méndez-Ramos, A. C. Yanes, and V. V. Moshchalkov, “Towards broad range and highly efficient down-conversion of solar spectrum by Er3+-Yb3+ co-doped nano-structured glass-ceramics,” Sol. Energy Mater. Sol. Cells94(10), 1612–1617 (2010). [CrossRef]
  12. Q. Y. Zhang, G. F. Yang, and Z. H. Jiang, “Cooperative downconversion in GdAl3 (BO3) 4: RE3+, Yb3+ (RE= Pr, Tb, and Tm),” Appl. Phys. Lett.91(5), 051903 (2007). [CrossRef]
  13. J. Zhou, Y. Teng, X. Liu, Z. Ma, and J. Qiu, “Broadband spectral conversion of visible light to near-infrared emission via energy transfer from Ce3+ to Nd3+/Yb3+ in YAG,” J. Mater. Res.26(05), 689–692 (2011). [CrossRef]
  14. Z. Liu, Y. Yu, N. Dai, Q. Chen, L. Yang, J. Li, and Y. Qiao, “Super Broadband Reddish Emitting Glass with Eu 2+ Doped for Warm-White Light-Emitting Diodes,” Appl. Phys., A Mater. Sci. Process.108(4), 777–781 (2012). [CrossRef]
  15. P. L. Higby, R. J. Ginther, I. D. Aggarwal, and E. J. Friebele, “Glass formation and thermal properties of low-silica calcium aluminosilicate glasses,” J. Non-Cryst. Solids126(3), 209–215 (1990). [CrossRef]
  16. L. Andrade, S. M. Lima, A. Novatski, A. Steimacher, J. H. Rohling, A. N. Medina, A. C. Bento, M. L. Baesso, Y. Guyot, and G. Boulon, “A step forward toward smart white lighting: Combination of glass phosphor and light emitting diodes,” Appl. Phys. Lett.95(8), 081104 (2009). [CrossRef]
  17. L. G. Hwa, S. L. Hwang, and L. C. Liu, “Infrared and Raman spectra of calcium alumino-silicate glasses,” J. Non-Cryst. Solids238(3), 193–197 (1998). [CrossRef]
  18. P. Vergeer, T. J. H. Vlugt, M. H. F. Kox, M. I. den Hertog, J. P. J. M. van der Eerden, and A. Meijerink, “Quantum cutting by cooperative energy transfer in YbxY1−xPO4:Tb3+,” Phys. Rev. B71(1), 014119 (2005). [CrossRef]

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