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Key Engineering Materials Vol. 451 (2011) pp 21-27<br />

Online available since 2010/Nov/11 at www.scientific.net<br />

© (2011) Trans Tech Publicati<strong>on</strong>s, Switzerland<br />

doi:10.4028/www.scientific.net/KEM.451.21<br />

<str<strong>on</strong>g>Dye</str<strong>on</strong>g>-<str<strong>on</strong>g>sensitized</str<strong>on</strong>g> <str<strong>on</strong>g>Solar</str<strong>on</strong>g> <str<strong>on</strong>g>Cells</str<strong>on</strong>g> <str<strong>on</strong>g>Based</str<strong>on</strong>g> <strong>on</strong> <strong>Nitrogen</strong>-<strong>doped</strong> <strong>Titania</strong> Electrodes<br />

Wei Guo, Qingqing Miao, Gang Xin, Liqi<strong>on</strong>g Wu, and Tingli Ma a<br />

State key laboratory of fine chemicals, School of Chemical Engineering, Dalian University of<br />

Technology, 116012, China<br />

a<br />

tinglima@dlut.edu.cn<br />

Keywords: nitrogen-doping; titania; dye-<str<strong>on</strong>g>sensitized</str<strong>on</strong>g> solar cell; stability; efficiency<br />

Abstract <str<strong>on</strong>g>Dye</str<strong>on</strong>g>-<str<strong>on</strong>g>sensitized</str<strong>on</strong>g> solar cell(DSC) is a new type of photovoltaic device. This paper mainly<br />

describes the research results of the development of a novel nitrogen-<strong>doped</strong> photoanode for DSC in<br />

our group. Highly efficient dye-<str<strong>on</strong>g>sensitized</str<strong>on</strong>g> solar cells (DSCs) of 7.6-10.1% were fabricated using<br />

nitrogen-<strong>doped</strong> titania electrodes. The photoelectrochemical properties of the nitrogen-<strong>doped</strong> titania<br />

powder, film, and solar cell were systemically investigated. We c<strong>on</strong>firmed the substituti<strong>on</strong> of<br />

oxygen sites and oxygen deficiency with nitrogen atoms in the titania structure by X-ray<br />

photoemissi<strong>on</strong> spectroscopy (XPS). The UV-Vis spectra of the nitrogen-<strong>doped</strong> powder and film<br />

showed visible light absorpti<strong>on</strong> in the wavelength range between 400 nm and 535 nm. The results<br />

of the stability test indicated that the DSCs fabricated by the nitrogen-<strong>doped</strong> titania exhibited great<br />

stability.<br />

Introducti<strong>on</strong><br />

Since Grätzel and coworkers developed a new type of solar cells based <strong>on</strong> the nanocrystalline TiO 2<br />

electrode,[1-3] dye-<str<strong>on</strong>g>sensitized</str<strong>on</strong>g> solar cells (DSCs) have attracted much attenti<strong>on</strong> for their high energy<br />

c<strong>on</strong>versi<strong>on</strong> efficiency as well as the possibility of becoming the a low-cost alternative to<br />

commercial solar cells based <strong>on</strong> silic<strong>on</strong>.[4-8] In order to successfully commercialize DSCs,<br />

however, it is necessary to further improve the energy c<strong>on</strong>versi<strong>on</strong> efficiency. Although many<br />

methods have been undertaken in the past to improve the c<strong>on</strong>versi<strong>on</strong> efficiency of the DSC, we<br />

have not seen significant improvement. Another problem is that the nanostructure TiO 2 electrode in<br />

DSCs has oxygen deficiency in TiO 2 crystal structure.[5-7] It is well known that the oxygen<br />

deficiency can create electr<strong>on</strong>-hole pairs and the oxidizing holes can react with the dye or be<br />

scavenged by iodide i<strong>on</strong>s.[8] Those deficiencies are able to cause shortening the lifetime of the<br />

DSCs. In order to solve the problems menti<strong>on</strong>ed above, we have developed a DSC system based <strong>on</strong><br />

N-<strong>doped</strong> titania. As a result, we have successfully achieved high energy c<strong>on</strong>versi<strong>on</strong> efficiency and<br />

high stability of DSCs using N-<strong>doped</strong> titania photoanodes. [9]<br />

Aiming to further understand the influence of the N-<strong>doped</strong> titania <strong>on</strong> the DSC system, we<br />

recently carried out detailed investigati<strong>on</strong>s such as preparing N-<strong>doped</strong> titania powders by several<br />

methods, and comparing the photoelectrochemical properties and electr<strong>on</strong> lifetime and transport<br />

time of the DSCs through intensity-modulated spectroscopic analysis. We also investigated the<br />

effect of electr<strong>on</strong> injecti<strong>on</strong> of the DSCs based <strong>on</strong> N-<strong>doped</strong> electrodes by surface photovlotage<br />

spectrum (SPS). In this review, we will summarize some of the results obtained by our group.<br />

Lately, Dai et al. also reported the results of retarded charge recombinati<strong>on</strong> in dye-<str<strong>on</strong>g>sensitized</str<strong>on</strong>g><br />

nitrogen-<strong>doped</strong> TiO 2 solar sells.[10] They prepared the N-<strong>doped</strong> titian using sol-gel method and<br />

discussed the mechanism of charge recombinati<strong>on</strong> of DSCs based <strong>on</strong> nitrogen-<strong>doped</strong> TiO 2<br />

electrodes. They indicated that the enhanced electr<strong>on</strong> lifetime for <strong>doped</strong> TiO 2 solar cells could be<br />

attributed to the formati<strong>on</strong> of O-Ti-N in the TiO 2 electrode to retard the recombinati<strong>on</strong> reacti<strong>on</strong> at<br />

the TiO 2 photoelectrode/electrolyte interface, as compared to the un<strong>doped</strong> TiO 2 solar cells. They<br />

also carried out the stability test under <strong>on</strong>e sun light soaking and a high temperature c<strong>on</strong>diti<strong>on</strong> (70<br />

°C) for more than 1000 hs, they observed that the DSC based <strong>on</strong> the N-<strong>doped</strong> TiO 2 photoanode is<br />

more stable than that of un<strong>doped</strong> TiO 2 .[10] These results are c<strong>on</strong>sistent with those of our group.[9]<br />

Yang et al. designed a device to generate TiN x O 2–x powders using NH 3 as a gaseous precursor.<br />

[11] They observed that the photoelectrochemical property of the solar cells appeared to be highly<br />

All rights reserved. No part of c<strong>on</strong>tents of this paper may be reproduced or transmitted in any form or by any means without the written permissi<strong>on</strong> of TTP,<br />

www.ttp.net. (ID: 59.46.193.241-20/11/10,08:28:50)


22 A New Sight towards <str<strong>on</strong>g>Dye</str<strong>on</strong>g>-<str<strong>on</strong>g>sensitized</str<strong>on</strong>g> <str<strong>on</strong>g>Solar</str<strong>on</strong>g> <str<strong>on</strong>g>Cells</str<strong>on</strong>g>: Material and Theoretical<br />

sensitive to the c<strong>on</strong>centrati<strong>on</strong> of N-<strong>doped</strong> in the TiO 2 . [11] Thus, they c<strong>on</strong>cluded that the research<br />

has offered proof of the relati<strong>on</strong>ships am<strong>on</strong>g the c<strong>on</strong>centrati<strong>on</strong>, the band gap, the nanoparticle size,<br />

and the photoelectric c<strong>on</strong>versi<strong>on</strong> efficiency of the N-<strong>doped</strong> TiO 2 photoelectrodes.[11] These results<br />

indicate that we can find an effective way to adjust the relati<strong>on</strong>ship between the c<strong>on</strong>centrati<strong>on</strong> and<br />

the band gap of the N-<strong>doped</strong> TiO 2 photoelectrodes. [11]<br />

Experimental<br />

Preparati<strong>on</strong> of -<strong>doped</strong> and un<strong>doped</strong> titania powders. Commercial titania powders of ST-01<br />

(Ishihara Sangyo, Ltd.) was used as the starting materials for preparing N-<strong>doped</strong> titania through dry<br />

and wet methods developed by our group. 17 Preparati<strong>on</strong> of the N-<strong>doped</strong> titania powder was<br />

attempted using the hydrolysis of titanium tetraisopropoxide (TTIP) and triethylamine or urea, the<br />

obtained powders were denoted as N-<strong>doped</strong> T and N-<strong>doped</strong> U. The un<strong>doped</strong> titania was prepared by<br />

the same process without notrogen source and they were denoted as un<strong>doped</strong> T and un<strong>doped</strong> U.<br />

Preparati<strong>on</strong> of -<strong>doped</strong> and un<strong>doped</strong> titania photoanodes. The pastes of the N-<strong>doped</strong> and<br />

un<strong>doped</strong> titania were prepared according to the procedure developed by our group, <strong>on</strong>ly adding<br />

polyethylene glycol (PEG) 600 as a dispersi<strong>on</strong> medium without any other binder.[12] The prepared<br />

titania paste was printed <strong>on</strong> the fluorine-<strong>doped</strong> tin oxide c<strong>on</strong>ducting glass (FTO glass, Asahi Glass;<br />

sheet resistance: 10 ohm/square) by screen-printing technique and sintered at 500 o C for 30 mins in<br />

the air.<br />

Fabricati<strong>on</strong> of the DSCs based <strong>on</strong> the -<strong>doped</strong> and un<strong>doped</strong> titania photoanodes. The<br />

sandwich-type solar cell c<strong>on</strong>sisted of the titania electrode adsorbed a Ru dye (<str<strong>on</strong>g>Solar</str<strong>on</strong>g><strong>on</strong>ix, N719), and<br />

the counter electrodes of Pt coated FTO-glass. The thickness and the area of the titania electrode<br />

were ca. 18 µm and 0.20 cm 2 respectively. The electrolyte soluti<strong>on</strong> was composed of 0.1 M LiI, 0.3<br />

M 1,2-dimethyl-3-propylimidazolium iodine, 0.05 M I 2 and 0.5 M tert-butylpyridine in 3-<br />

methoxypropi<strong>on</strong>itrile.<br />

Photovoltaic measurement of DSCs. The UV-Vis spectra were taken <strong>on</strong> a JASCO V-550 using<br />

an integrating sphere setup. The current-voltage measurements of the N-<strong>doped</strong> and un<strong>doped</strong> titania<br />

were performed using a 300 W solar simulator as the light source. Intensity-modulated photocurrent<br />

and photovoltage spectroscopy (IMPS and IMVS) were performed using a white light-emitting<br />

diode (Lumiled Luxe<strong>on</strong> Star 1W) as the light source at room temperature.<br />

Fig.1. X-ray diffractogram for N-<strong>doped</strong> titania powder of T and U.


Key Engineering Materials Vol. 451 23<br />

Fig.2. XPS spectra of N-<strong>doped</strong> titania powders, (a.b) N-<strong>doped</strong> ST-01; (c) N-<strong>doped</strong> T; (d) N-<strong>doped</strong> U.<br />

Results and Discussi<strong>on</strong><br />

Structural characterizati<strong>on</strong>s of the titania powders were performed by X-ray diffracti<strong>on</strong> patterns<br />

(XRD). Fig.1 displays the data for the N-<strong>doped</strong> titania prepared by the wet method. The results<br />

indicated that the crystal phase of the N-<strong>doped</strong> powder was anatase, and no crystal phase of the<br />

rutile was observed after annealing at 400ºC. At temperatures over 700 ºC, however, the crystal<br />

phase of the rutile was observed both in the case of N-<strong>doped</strong> tintania of T and U.<br />

The substituti<strong>on</strong> of the oxygen sites and oxygen deficiency site with nitrogen atoms in the titania<br />

structure was c<strong>on</strong>firmed by X-ray photoemissi<strong>on</strong> spectroscopy (XPS), as shown in Fig.2. Three<br />

binding energy peaks were observed at 396.2, 398.3, and 400.4 eV in the N 1s regi<strong>on</strong>. C<strong>on</strong>cerning<br />

the assignment of the peak feature in XPS for the nitrogen-<strong>doped</strong> titania, some c<strong>on</strong>troversy still<br />

exists in the literature. A detailed discussi<strong>on</strong> was performed in our previous publicati<strong>on</strong>. [9].<br />

We c<strong>on</strong>sidered that the signal at 396.2 eV is attributed to a chemically bound N - species and the<br />

weak peak around 398.3 eV is derived from the presence of the O-Ti-N linkages in the crystalline<br />

TiO 2 lattice (Fig. 2a). The formati<strong>on</strong> of the Ti-N and O-Ti-N structures is suggested to proceed<br />

during the substituti<strong>on</strong> doping process. It has been dem<strong>on</strong>strated that the N substitute O site or<br />

oxygen deficiency site in the crystalline TiO 2 lattice can stabilize the DSC system. [9, 10] On the<br />

other hand, the signal around 400.4 eV is c<strong>on</strong>sidered to be a molecularly adsorbed nitrogen species,<br />

which absorbs <strong>on</strong>to the surface and into the interstitial sites of the titania lattice (Fig. 2b). The XPS<br />

results of the N-<strong>doped</strong> titania T (Fig. 2c) and N-<strong>doped</strong> titania U (Fig. 2d) can be also assigned as<br />

discussing above. These results are c<strong>on</strong>sistent with those described in previous literature [13-15].<br />

The UV-Vis absorpti<strong>on</strong> spectra were measured using an integrating sphere setup for the N-<strong>doped</strong><br />

powders and films with adsorbed dye, as shown in Fig.3. For comparis<strong>on</strong>, the spectra of the N-


24 A New Sight towards <str<strong>on</strong>g>Dye</str<strong>on</strong>g>-<str<strong>on</strong>g>sensitized</str<strong>on</strong>g> <str<strong>on</strong>g>Solar</str<strong>on</strong>g> <str<strong>on</strong>g>Cells</str<strong>on</strong>g>: Material and Theoretical<br />

<strong>doped</strong> titania T powder is also illustrated (Fig. 3a). No absorpti<strong>on</strong> peak for the un<strong>doped</strong> T was<br />

observed above the wavelength of 400 nm. On the other hand, the N-<strong>doped</strong> titania T powders<br />

exhibited a new absorpti<strong>on</strong> peak in the visible light regi<strong>on</strong> between 400 nm and 550 nm (Fig. 3b).<br />

The visible light activity is possibly due to the N-doping in the titania crystalline structure, which<br />

was caused by the fact that the nitrogen doping induced a new state lying close to the valence band<br />

edge.[16] From Fig. 3, we also found that the amount of dye adsorpti<strong>on</strong> of N-<strong>doped</strong> T (Fig. 3d) was<br />

more than that of N-<strong>doped</strong> U (Fig. 3c).<br />

Fig.3. UV-Vis spectra of the N-<strong>doped</strong> and un<strong>doped</strong> titania powder and film, (a) un<strong>doped</strong> T powder;<br />

(b) N-<strong>doped</strong> T powder; (c) N-<strong>doped</strong> U film / N719 dye; (d) N-<strong>doped</strong> T film/ N719 dye.<br />

Fig.4. UV-Vis spectra of the N-<strong>doped</strong> and un<strong>doped</strong> titania powder after sintering at different<br />

temperature.


Key Engineering Materials Vol. 451 25<br />

In order to test the thermal stability of the N-<strong>doped</strong> titania prepared in this work, we measured<br />

the UV-Vis apectra after sintering at the range of 450-600˚C in the air. As shown in Fig. 4, the<br />

adsorpti<strong>on</strong> peaks were still observed after sintering at 600 ˚C for 30 mins, although the intensity of<br />

these peaks decreased as the sintering temperature increased. This result indicates that the nitrogen<strong>doped</strong><br />

titania has remarkable thermal stability.<br />

Table 1 shows the current-voltage data of the open cells based <strong>on</strong> the N-<strong>doped</strong> T and U, and the<br />

un<strong>doped</strong> titania photoelectrodes. We observed a pr<strong>on</strong>ounced increase in the photocurrent and<br />

photovoltage for the DSCs based <strong>on</strong> the N-<strong>doped</strong> titania. High energy c<strong>on</strong>versi<strong>on</strong> efficiencies of<br />

7.9% and 7.6% were achieved, and the enhancement of ca. 10% and 5% were observed due to the<br />

introducti<strong>on</strong> of the N-dped. A high efficiency of 10.1% for the DSC based <strong>on</strong> N-<strong>doped</strong> titania ST-<br />

01 was reached after the optimizati<strong>on</strong>. The details will be published in an another paper.<br />

Table 1. Performance of the DSCs based <strong>on</strong> the N-<strong>doped</strong> and un<strong>doped</strong> titania electrods<br />

Samples V OC (mV) J SC (mA) FF η(%)<br />

N-<strong>doped</strong> T 681 16.3 0.72 7.9<br />

N-<strong>doped</strong> U 780 15.8 0.62 7.6<br />

un<strong>doped</strong> TiO 2 747 14.8 0.65 7.2<br />

There was a c<strong>on</strong>cern that the visible-light-active titania can possibly accelerate the deteriorati<strong>on</strong><br />

of the dye and the electrolyte in the DSC system. Therefore, we performed studies <strong>on</strong> the stability<br />

of the DSCs based <strong>on</strong> the N-<strong>doped</strong> T (pink line) and U (blue line) electrodes during irradiati<strong>on</strong> for<br />

1000 hs under the white light (100 mW/cm 2 ) at 25 ºC(Fig.5). The stability of the DSCs based <strong>on</strong> the<br />

N-<strong>doped</strong> ST-01 (black line) was also tested for 2000 hs under the same c<strong>on</strong>diti<strong>on</strong>. As shown in<br />

Fig.5, no photodegradati<strong>on</strong> was observed for the cell involving the nitrogen-incorporated titania<br />

structure. We also carried out an outdoor stability test of the N719 dye/N-<strong>doped</strong> titania stored in the<br />

air for four years and complete solar cells exposed under <strong>on</strong>e sunlight for 109 days at ambient<br />

temperature in Dalian, China. The result implies that the deteriorati<strong>on</strong> of the dye did not happen<br />

during the test period. Recently, Dai et el. also carried out the stability test of the DSCs based <strong>on</strong> the<br />

N-<strong>doped</strong> titania. They observed that the DSC based <strong>on</strong> the N-<strong>doped</strong> titania photoanode was more<br />

stable under <strong>on</strong>e sun light soaking and a high temperature c<strong>on</strong>diti<strong>on</strong> (70 o C) for more than 1000 hs.<br />

These results reveal that the dye-<str<strong>on</strong>g>sensitized</str<strong>on</strong>g> solar cell fabricated with the N-<strong>doped</strong> titania electrode<br />

possesses an excellent stability.<br />

Furthermore, the electr<strong>on</strong> transport time, electr<strong>on</strong> lifetime, and electr<strong>on</strong> injecti<strong>on</strong>, in the dye<str<strong>on</strong>g>sensitized</str<strong>on</strong>g><br />

N-<strong>doped</strong> and un<strong>doped</strong> solar cells were studied by intensity-modulated spectroscopic<br />

analysis and the surface photovlotage spectrum (SPS). The detailed data will be summarized in an<br />

another paper.<br />

Summary<br />

In c<strong>on</strong>clusi<strong>on</strong>, the N-<strong>doped</strong> titania nanocrystalline materials were successfully synthesized by the<br />

dry and the wet methods. Three binding energy peaks were shown in the N 1s regi<strong>on</strong> of the XPS.<br />

The signals at 396.2 eV and 398.3 eV were attributed to a chemically bound N - species and the O-<br />

Ti-N linkages within the crystalline TiO 2 lattice, respectively. A new absorpti<strong>on</strong> was observed for<br />

the UV-Vis spectrum of the N-<strong>doped</strong> titania in the visible light regi<strong>on</strong>. The high energy c<strong>on</strong>versi<strong>on</strong><br />

efficiencies of 7.6% - 10.1% were achieved for the DSCs based <strong>on</strong> the N-<strong>doped</strong> titania electrodes.<br />

The results of the stability test dem<strong>on</strong>strated that the introducti<strong>on</strong> of nitrogen into the titania<br />

photoelectrode of the DSC can stabilize the DSC system. Further detailed studies are in progress to<br />

improve the efficiency through the optimizati<strong>on</strong> of the amount of nitrogen doping, and the<br />

mechanism to improve the efficiency in N-<strong>doped</strong> DSC system.


26 A New Sight towards <str<strong>on</strong>g>Dye</str<strong>on</strong>g>-<str<strong>on</strong>g>sensitized</str<strong>on</strong>g> <str<strong>on</strong>g>Solar</str<strong>on</strong>g> <str<strong>on</strong>g>Cells</str<strong>on</strong>g>: Material and Theoretical<br />

Fig. 5. Stability for the DSC based <strong>on</strong> N-<strong>doped</strong> T (pink line), U (blue line) and N-<strong>doped</strong> ST-<br />

01(black line) titania electrodes over 1000 hs and 2000 hs of c<strong>on</strong>tinuous illuminati<strong>on</strong> with white<br />

light of 100 mW/cm 2 intensity.


Key Engineering Materials Vol. 451 27<br />

Acknowledgment<br />

This research was supported by the Nati<strong>on</strong>al Natural Science Foundati<strong>on</strong> of China (Grant No.<br />

50773008). This work was also supported by the Nati<strong>on</strong>al High Technology Research and<br />

Development Program for Advanced Materials of China (Grant No. 2009AA03Z220) and State Key<br />

Laboratory of New Ceramic and Fine Processing Tsinghua University.<br />

References<br />

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[2] M.K. Nazeeruddin, A. Kay, I. Rodicio, R. Humphrey-Baker, E. Muller, P. Liska, N.<br />

Vlachopoulos, M. Grätzel: J. Am. Chem. Soc. Vol. 115 (1993), p. 6382.<br />

[3] K. Sayama, H. Sugihara, H. Arakawa: Chem. Mater. Vol. 10 (1998), p. 3825.<br />

[4] M. Grätzel: Prog. Photovolt. Res. Appl. Vol. 8 (2000), p. 171.<br />

[5] I. Inakamura, N. Negishi, S. Kutsuna, T. Ihara, S. Sugihara, K. Takeuchi: J. Mol. Catal. A:<br />

Chem. Vol. 161 (2000), p. 205.<br />

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(2003), p. 403.<br />

[7] H. Irie, Y. Watanabe, K. Hashimoto: J. Phys. Chem. B Vol. 107 (2003), p. 5483.<br />

[8] M. Mrowetz, W. Balcerski, A.J. Colussi, M.R. Hoffmann: J. Phys. Chem. B Vol. 108 (2004), p.<br />

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[9] T. Ma, M. Akiyama, E. Abe, I. Imai: Nano Lett. Vol. 5 (2005), p. 2543.<br />

[10] H. Tian, L. Hu, C. Zhang, W. Liu, Y. Huang, L. Mo, L. Guo, J. Sheng, S. Dai: J. Phys. Chem.<br />

C. Vol. 114 (2010), p. 1627.<br />

[11] X. Wang, Y. Yang, Z. Jiang, R. Fan: Eur. J. Inorg. Chem. (2009), p. 3481.<br />

[12] T. Ma, T. Kida, M. Akiyama, K. Inoue, S. Tsunematse, K. Yao, H. Noma, E. Abe:<br />

Electrochem. Commun. Vol. 5 (2003), p. 369.<br />

[13] N.C. Saha, H.G. Tompkins: J. Appl. Phys. Vol. 72 (1992), p. 3072.<br />

[14] J.C. Fuggle, E. Umbach, D.R. Menzel, K. Wandelt, C.R. Burndle: Solid State Commun. Vol.<br />

27, (1978), p. 65.<br />

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Vol. 191 (1990), p. 55.<br />

[16] T. Lindgraen, J.M. Mwabora, E. Avendano, J. J<strong>on</strong>ss<strong>on</strong>, A. Hoel, C. Granqvist, S. Lindquist : J.<br />

Phys. Chem. B Vol. 107 (2003), p. 5709.


A New Sight towards <str<strong>on</strong>g>Dye</str<strong>on</strong>g>-<str<strong>on</strong>g>sensitized</str<strong>on</strong>g> <str<strong>on</strong>g>Solar</str<strong>on</strong>g> <str<strong>on</strong>g>Cells</str<strong>on</strong>g>: Material and Theoretical<br />

doi:10.4028/www.scientific.net/KEM.451<br />

<str<strong>on</strong>g>Dye</str<strong>on</strong>g>-Sensitized <str<strong>on</strong>g>Solar</str<strong>on</strong>g> <str<strong>on</strong>g>Cells</str<strong>on</strong>g> <str<strong>on</strong>g>Based</str<strong>on</strong>g> <strong>on</strong> <strong>Nitrogen</strong>-Doped <strong>Titania</strong> Electrodes<br />

doi:10.4028/www.scientific.net/KEM.451.21

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