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Optics Express

  • Editor: C. Martijn de Sterke
  • Vol. 15, Iss. 25 — Dec. 10, 2007
  • pp: 17010–17018

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Photochromic effect in LiNbO3: Fe :Co

Wenbo Yan, Yangxian Li, Lihong Shi, Hongjian Chen, Shiguo Liu, Ling Zhang, Ziheng Huang, Shaolin Chen, and Yongfa Kong  »View Author Affiliations


Optics Express, Vol. 15, Issue 25, pp. 17010-17018 (2007)
http://dx.doi.org/10.1364/OE.15.017010


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Abstract

In this paper, Co2O3 was codoped in LiNbO3: Fe crystals. It was found that Co codoping can give rise to the strong photochromic effect in LiNbO3: Fe. Based on the UV-VIS-NIR absorption spectra, photorefractive sensitivities, and EPR results for both virgin and sensitized states of the crystal, the photochromic mechanism in this material was suggested as follows. During sensitization, electrons transfer from O2- to Fe3+ directly while holes are thermally excited from O- into the valence band and then partly trapped by Co2+, which leads to the darkening of the crystal. In bleaching process, the electrons are excited from Fe2+ to the conduction band by green light and recombine with the holes on the Co2+ level. Sensitizing/bleaching experiments were also carried out in LiNbO3: Fe: Co crystals. Fast sensitization found for this material is beneficial to two-color recording.

© 2007 Optical Society of America

1. Introduction

In the past several decades, Fe-doped lithium niobate (LiNbO3: Fe, LN: Fe) crystals have been extensively studied as a material for volume holographic memory applications because of their excellent photorefractive properties [1

P. Günter and J. P. Huignard, Photorefractive Materials and Their Applications , Vols. I and II, (Springer-Verlag, Heidelberg, 1989).

]. In this material, electrons can be excited from Fe2+ by light and, upon migration, are retrapped by Fe3+, giving rise to the photorefractive effect. Element Mn and Cu can also be doped as photorefractive impurities, and Mn2+/Mn3+ and Cu+/Cu2+ act as photorefractive levels in singly-doped crystals [2

K. Buse, “Light-induced charge transport processes in photorefractive crystals II: Materials,” Appl. Phys. B 64, 391–407 (1997). [CrossRef]

]. Crystals doped with two types of impurities can be obtained through codoping. Recently, Mn or Cu was codoped with Fe in LN to form two different photorefractive levels in crystal for two-color recording [3

K. Buse, A. Adibi, and D. Psaltis, “Non-volatile holographic storage in doubly doped lithium niobate crystals,” Nature 393, 665–668 (1998). [CrossRef]

,4

L. Y Ren, L. R. Liu, D. A. Liu, Ch. H. Zhou, and G. G. Li, “Experimental and theoretical study of non-volatile photorefractive holograms in doubly doped LiNbO3:Fe:Cu,” Opt. Mater. 23, 261–267 (2003). [CrossRef]

]. Besides Fe, Mn and Cu mentioned above, other transition metal elements, such as Co, have also been investigated as dopants. Unfortunately, it was proved by many experiments that Co is not an efficient photorefractive center in singly-doped crystals [5

W. Phillips, J. J. Amodei, and D. L. Staebler, “Optical and holographic storage properties of transition metal doped lithium niobate,” RCA Rev. 33, 94–109 (1972).

,6

D. K. McMillen, T. D. Hudson, J. Wagner, and J. Singleton, “Holographic recording in specially doped lithium niobate crystals,” Opt. Express 12, 491–502 (1998). [CrossRef]

], because the visible absorption produced in LN doped with Co arises from localized electronic states and cannot be utilized for photoexciting electrons [5

W. Phillips, J. J. Amodei, and D. L. Staebler, “Optical and holographic storage properties of transition metal doped lithium niobate,” RCA Rev. 33, 94–109 (1972).

,7

H. Fujita, M. Inoue, and W. Phillips, “Optical properties of Cobalt-doped lithium niobate,” Jpn. J. Appl. Phys. 44, 1909–1917 (1978).

]. However, impurities without absorption suitable for photoexciting electrons sometimes also influence the photorefractive properties of the material. Recently, Lee et al. found out that the photorefractive properties of Fe-doped (or nominally pure) near-stoichiometric LN crystals can be affected significantly by Tb impurity [8

M. Lee, S. Takekawa, Y. Furukawa, Y. Uchida, K. Kitamura, H. Hatano, and S. Tanaka, “Photochromic effect in near-stoichiometric LiNbO3 and two-color holographic recording,” J. Appl. Phys. 88, 4476–4485 (2000). [CrossRef]

,9

M. Lee, I. G. Kim, S. Takekawa, Y. Furukawa, Y. Uchida, K. Kitamura, and H. Hatano, “Electron paramagnetic resonance investigation of the photochromic effect in near-stoichiometric LiNbO3 with applications to holographic storage,” J. Appl. Phys. 89, 5311–5317 (2001). [CrossRef]

]. In their work, Tb neither induces any obvious absorption in spectrum nor acts as a photorefractive center, but it can enhance and stabilize the UV-light-induced absorption (e.g. photochromic effect) in the crystals. The above discussion raises a question of whether Co can affect the photorefractive properties of material indirectly when it is codoped with Fe in LN.

In this paper, Co2O3 was codoped in LiNbO3: Fe crystals. It was revealed that Co codoping can give rise to the strong photochromic effect in LiNbO3: Fe and affect the photorefractive properties of the material significantly. Further investigations on UV-VIS-NIR absorption and EPR spectra showed that Fe and Co ions are all involved in the photochromic process. We also discussed the photochromic mechanism in LiNbO3: Fe: Co, which is slightly different from that in LiNbO3: Fe: Mn [10

A. Adibi, K. Buse, and D. Psaltis, “Two-center holographic recording,” J. Opt. Soc. Am. B 18, 584–601 (2001). [CrossRef]

]. Sensitizing/bleaching experiments were carried out on LiNbO3: Fe: Co crystals. The results indicate the potential of this material for two-color recording. Though the material focused by our work is still limited in the series of LN crystals doped with Fe, this work is of value in the search both for new phenomena in doubly-doped photorefractive crystals and for feasible applications in the optical-memory devices based on two-color recording.

2. Experimental setup

Samples used in this study were LN crystals codoped with 0.03 mol% Fe2O3 and 0.015 mol% Co2O3. Doubly-doped LN single crystal was grown along the c-axis from congruent melt by using the Czochralski technique. Then it was cut to rectangular-shaped y-oriented plates with thickness of 1.2 mm and polished to optical grade.

A 20-W mercury lamp was used as the incoherent UV light source. The spectrum of UV light was selected to peak at 365 nm by an appropriate optical filter. The UV light was loosely focused by a lens to irradiate the sample. In order to investigate the UV-light-induced absorption (ULIA) at different wavelengths, the unpolarized light absorption spectra along the y-axis from the sample were measured by shimadzu UV-365 spectrometer. EPR study was also performed to characterize the photochromic centers. For this study, the sample was prepared in rectangular rod and mounted on fused-silica glass tube with c-axis perpendicular to the magnetic field. EPR measurements were carried out at a radio frequency of 9.85 GHz with the modulation frequency of 100 kHz by using a Bruker EMX-6/1 X-band spectrometer at room temperature.

Fig. 1. (a). Schematic of the experimental arrangement for one-color recording. Two e-polarized beams with equal intensities of 110 mW/cm2 were used for the recording. The readout beam is denoted as “R”. (b). Schematic of the experimental arrangement for sensitizing and bleaching. UV light emitted from mercury lamp was used for sensitizing. The intensity of the NIR probe beam is 1mW/cm2. The expanded green beam for bleaching is omitted in the figure. The transmission and reference beams are denoted as “T” and “R”, respectively.

One-color recording was preformed to characterize the photorefractive properties. As shown in Fig. 1(a), the grating was written at a crossing angle of 30° on the sample by two extraordinary polarized beams, which were emitted from an Ar+ laser of 514 nm and with equal intensities of 110 mW/cm2. The grating wave vector was aligned along the c-axis of the sample. Sensitivity can be obtained through S=(d(η)1/2/dt|t=0)/(IRecL)=(A0/τr)/(IRecL), where A0 is the saturation hologram strength, η is diffraction efficiency, τr is recording time constant, IRec is the total recording intensity, and L is the thickness of the recording medium [11

A. Adibi, K. Buse, and D. Psaltis, “System measure for persistence in holographic recording and application to singly-doped and doubly-doped lithium niobate,” Appl. Opt. 40, 5175–5182 (2001). [CrossRef]

]. Note that (η)1/2=A, where A is the hologram strength. Diffraction efficiency is defined as ID/(ID+IT), where ID and IT are the diffracted and transmitted intensities of the readout beam, respectively. Recording time constant is defined as the period of time from commence to (1-1/e) of the saturation hologram strength.

Figure 1(b) shows the schematic of the experimental arrangement for sensitizing and bleaching. ULIA was probed by an unpolarized 780 nm beam emitted from diode laser. The probe light with the intensity of 1mW/cm2 impinged on the sample along the y-axis. The transmitted light was detected by a photo-detector with a filter placed in front to block scattered 365-nm pump UV light. A 514 nm beam was expanded for bleaching. In addition, another reference light was taken out from the probe light just before the sample. And the ULIA coefficient was obtained from ln[(IR1/IR0)/(IT1/IT0)]/d, where IT1 (IT0) and IR1 (IR0) are measured intensities of transmission and reference beams with (without) UV irradiation respectively, and d is the sample’s thickness. By this way, we can reduce as much as possible the drifts caused by power fluctuation of diode laser.

Fig. 2. Photograph of the sample with both virgin and sensitized states. The virgin state presents a purple color while the sensitized state exhibits the dark reddishness.
Fig. 3. Unpolarized light absorption spectra for both virgin and sensitized states. The left inset shows the UV-light-induced absorption, e.g. the absorption difference between the virgin and sensitized states. For comparison, the right inset shows the absorption difference between LN singly-doped with Fe and pure LN.

3. Results

The virgin sample presents a purple color and looks very like LN crystals singly-doped with Co [6

D. K. McMillen, T. D. Hudson, J. Wagner, and J. Singleton, “Holographic recording in specially doped lithium niobate crystals,” Opt. Express 12, 491–502 (1998). [CrossRef]

]. However, under UV irradiation, the sample color changes rapidly to the dark reddishness that is often exhibited by LN crystals singly-doped with Fe [6

D. K. McMillen, T. D. Hudson, J. Wagner, and J. Singleton, “Holographic recording in specially doped lithium niobate crystals,” Opt. Express 12, 491–502 (1998). [CrossRef]

]. This dark reddish sample can be recovered to its virgin state by irradiating with visible light. In other words, the sample can be sensitized by UV light and bleached by visible light. Figure 2 shows the photograph of the sample with both virgin and sensitized states.

Figure 3 illustrates the unpolarized light absorption spectra of the two different states. From the spectrum of the virgin state, we can see a series of bands overlap in the range from 500 to 1500 nm. These bands are consistent with the results obtained in LN crystals singly-doped with Co [6

D. K. McMillen, T. D. Hudson, J. Wagner, and J. Singleton, “Holographic recording in specially doped lithium niobate crystals,” Opt. Express 12, 491–502 (1998). [CrossRef]

]. Fujita et al. [7

H. Fujita, M. Inoue, and W. Phillips, “Optical properties of Cobalt-doped lithium niobate,” Jpn. J. Appl. Phys. 44, 1909–1917 (1978).

] suggested that they are all due to d-d transition of Co ions. Among them, the band at 1450 nm and those near 550 nm correspond to Co2+, and that centered at 750 nm is assigned to Co3+. After UV sensitization, it is interesting to find an increase of absorption below 820 nm. This ULIA, which is showed in the left inset of Fig. 3, apparently consists of two different components: the broad one centered at 500 nm and the relatively narrow one peaked at 750 nm. For comparison, the right inset shows the absorption difference between LN singly-doped with Fe and pure LN. One can see that the broad component of the ULIA is very similar in shape to the band induced by Fe2+-Nb5+ intervalence transfer in the right inset.

Fig. 4. Recording time constant and sensitivity plotted with the ULIA at 514 nm, where the variable ULIA was controlled by the UV exposure fluence.

One-color recording was preformed on the sample with different UV exposure fluence. For the virgin state, the sensitivity of holographic recording is very small, but it boosts up tens of times after UV irradiation. In Fig. 4, the recording time constant and sensitivity are plotted with the ULIA at 514 nm, where the variable ULIA was controlled by the UV exposure fluence. The above results show that the ULIA markly improves the performance of the sample in one-color recording.

The EPR spectra of the virgin LiNbO3: Fe: Co crystals are shown in Fig. 5. The EPR signals found there should not be assigned to Fe2+ and Co2+ ions because homogeneous broadening, due to rapid spin-lattice relaxations, prevents the observation of EPR signals from them at room temperature [12

H. Kurz, E. Krätzig, W. Keune, H. Engelmann, U. Gonser, B. Dischler, and A. Räuber, “Photorefractive centers in LiNbO3, studied by optical-, Mössbauer- and EPR-methods,” Appl. Phys. 12, 355–368 (1977). [CrossRef]

,13

Y. N. Choi, I. W. Park, S. S. Kim, S. S. Park, and S. H. Choh, “Electron paramagnetic resonance studies of Co2+ ions in congruent and nearly stoichiometric LiNbO3 single crystals,” J. Phys.: Condens. Matter 11, 4723–4730 (1999). [CrossRef]

]. Thus, these signals must arise from Fe3+, which can also be confirmed by the previous Fe3+ EPR spectra [14

D. J. Keeble, M. Loyo-Menoyo, Y. Furukawa, and K. Kitamura, “Electron paramagnetic resonance of Fe3+ in LiNbO3 ,” Phys. Rev. B 71, 224111 (2005). [CrossRef]

]. The insets of Fig. 5 show the EPR signals for the virgin and sensitized states, respectively. The reduction of Fe3+ signal intensity after UV sensitization is clearly seen.

Fig. 5. EPR spectra of LiNbO3: Fe: Co crystals. The left and right insets show the EPR signals near 2000 Gauss for the virgin and sensitized states, respectively.

Sensitizing/bleaching experiments were carried out on LiNbO3: Fe: Co crystals. Figure 6(a) shows the sensitizing curves of the ULIA in different UV intensities (IUV). The inset of Fig. 6(a) gives the dependence of sensitizing time constant (labeled as Time Cons. in the figure) on UV intensity, where sensitizing time constant is defined as the period of time from commence to (1-1/e) of the saturated absorption. Our results show that the sensitization of LiNbO3: Fe: Co is very fast. Even for the lowest UV intensity of 34 mW/cm2, we can obtain a short sensitizing time constant of 166 s in LiNbO3: Fe: Co. Note that in LiNbO3: Fe: Mn, tens of minutes is usually required for sensitization process [10

A. Adibi, K. Buse, and D. Psaltis, “Two-center holographic recording,” J. Opt. Soc. Am. B 18, 584–601 (2001). [CrossRef]

]. In addition, it is evident in the inset of Fig. 6(a) that, the sensitization time constant initially decreases rapidly with the increase of UV intensity, followed by a gradual saturation near 100 mW/cm2, indicating UV intensity of 100 mW/cm2 is suitable for highly efficient sensitization. Figure 6(b) shows the bleaching curves of the ULIA in different bleaching intensities (IB). The inset of Fig. 6(b) gives the dependence of bleaching time constant on bleaching intensity, where bleaching time constant is defined as the period of time from commence to (1/e) of the initial absorption.

Fig. 6. (a). Sensitizing curves of the ULIA in different UV intensities. The inset shows the dependence of sensitizing time constant on UV intensity. (b). Bleaching curves of the ULIA in different bleaching intensities. The inset shows the dependence of bleaching time constant on bleaching intensity.

4. Discussion

For LN crystals containing Fe impurity, the broad band centered at 500 nm usually appears owing to Fe2+-Nb5+ intervalence transfer [12

H. Kurz, E. Krätzig, W. Keune, H. Engelmann, U. Gonser, B. Dischler, and A. Räuber, “Photorefractive centers in LiNbO3, studied by optical-, Mössbauer- and EPR-methods,” Appl. Phys. 12, 355–368 (1977). [CrossRef]

]. However, it is nearly absent in the absorption spectrum of virgin LiNbO3: Fe: Co crystals, which indicates that few electrons are trapped by Fe3+ in the virgin state. After UV sensitization, a broad component centered at 500 nm is found in the ULIA and this component is very similar in shape to the band induced by Fe2+-Nb5+ intervalence transfer. Thus the ULIA at 500 nm is likely to be induced by the appearance of a large number of Fe2+. However, Co2+ can also give rise to the absorption near 500 nm, so further justifications are needed. In one-color recording with green light, sensitivity is found to increases with the ULIA, which gives another support to our above suggestion that the ULIA near 500 nm is caused by Fe2+, because sensitivity is generally in proportion to the amount of Fe2+ in crystal [15

K. Buse, “Light-induced charge transport processes in photorefractive crystals I: Models and experimental methods,” Appl. Phys. B 64, 391–407 (1997). [CrossRef]

]. The most decisive proof of our suggestion comes from the comparison of EPR signals between the virgin and sensitized states. The Fe3+ signal intensity decreases obviously after UV sensitization, which reveals that the ULIA near 500 nm is due to the valence change from Fe3+ to Fe2+.

The above discussion shows that electrons will transfer to Fe3+ ions after UV sensitization. But, where are the electrons from? We know that LN crystals, even nominally pure ones, maybe contain undesigned Mn impurity with low concentration of several ppm. But, in our case, electrons should not come from the deep traps formed by Mn impurity because no Mn2+ signals, consisting of several six-hyperline sets [8

M. Lee, S. Takekawa, Y. Furukawa, Y. Uchida, K. Kitamura, H. Hatano, and S. Tanaka, “Photochromic effect in near-stoichiometric LiNbO3 and two-color holographic recording,” J. Appl. Phys. 88, 4476–4485 (2000). [CrossRef]

], have been found in the EPR spectra of the virgin state. There is little likelihood of electrons photoexcited from Co2+ because the absorption of Co2+ arises from localized electronic states. One possible way is charge transfer (CT) from O2- to Fe3+ induced by UV irradiation. This CT process has been justified by many researchers from both experimental and theoretical aspects [2

K. Buse, “Light-induced charge transport processes in photorefractive crystals II: Materials,” Appl. Phys. B 64, 391–407 (1997). [CrossRef]

,12

H. Kurz, E. Krätzig, W. Keune, H. Engelmann, U. Gonser, B. Dischler, and A. Räuber, “Photorefractive centers in LiNbO3, studied by optical-, Mössbauer- and EPR-methods,” Appl. Phys. 12, 355–368 (1977). [CrossRef]

]. However, Fe3+ also exits in LN singly-doped with Fe, yet no obvious photochromic effect can be found even in the oxidized crystals. How can we explain this discrepancy and what is the role of Co in the photochromic process of LiNbO3: Fe: Co? Since the holes self-trapped at O2- ions (in the form of O- ions) are unstable at room temperature [16

O. Schirmer, O. Thiemann, and M. Wöehlecke, “Defects in LiNbO3. I. experimental aspects,” J. Phys. Chem. Solids 52, 185–200 (1991). [CrossRef]

], they are thermally excited into the valence band after the CT process. In LN singly-doped with Fe, all the holes will be retrapped by Fe2+ when UV light is absent. Thus we cannot observe the photochromic effect there. In the case of LiNbO3: Fe: Co, we tentatively give a hypothesis that holes have an opportunity to be trapped by Co2+. This hypothesis seems reasonable if we notice that holes can be captured by Co2+ in some cobalt-doped ABO3 compounds such as BaTiO3: Co [17

D. Rytz, B. A. Wechsler, M. H. Garrett, C. C. Nelson, and R. N. Schwartz, “Photorefractive properties of BaTiO3:Co,” J. Opt. Soc. Am. B 7, 2245–2254 (1990). [CrossRef]

,18

M. H. Garrett, J. Y. Chang, H. P. Jenssen, and C. Warde, “High beam-coupling gain and deep- and shallow-trap effects in cobalt-doped barium titanate, BaTiO3:Co,” J. Opt. Soc. Am. B 9, 1407–1415 (1992). [CrossRef]

]. As shown in Fig. 7, part of holes are trapped by Co2+ and cannot return to Fe2+ when UV light is absent, which leads to the dark reddishness of the sensitized state. Evidence for the above suggestions is the narrow ULIA component peaked at 750 nm, which should be assigned to Co3+ (Co2+ with trapped holes) according to the suggestion of Fujita et al [7

H. Fujita, M. Inoue, and W. Phillips, “Optical properties of Cobalt-doped lithium niobate,” Jpn. J. Appl. Phys. 44, 1909–1917 (1978).

]. Based on our discussion, the amount of Co2+ will reduce after UV irradiation, which seems conflicting with the nearly unchanged absorption at 1450 nm in the sensitized state. However, the absorption at 1450 nm is also influenced by other factors. Kurz et al. studied detailedly the photorefractive properties of LiNbO3: Fe crystals in combination with optical absorption-, Mössbauer- and EPR-measurments and drew a very important conclusion about the association of the optical band around 500 nm with Fe2+. Besides this result, they also suggested that Fe2+ can cause another broad band at 1200 nm due to the crystal-field splitting of Fe2+ level at 500 nm [12

H. Kurz, E. Krätzig, W. Keune, H. Engelmann, U. Gonser, B. Dischler, and A. Räuber, “Photorefractive centers in LiNbO3, studied by optical-, Mössbauer- and EPR-methods,” Appl. Phys. 12, 355–368 (1977). [CrossRef]

]. Thus, we believe that both Fe2+ and Co2+ contribute to the absorption at 1450 nm. Though the amount of Co2+ reduces after UV irradiation, the Fe2+ formed by UV irradiation may keep the absorption at 1450 nm unchanged. Figure 7 also shows the mechanism of bleaching: electrons are excited from Fe2+ to the conduction band by green light and then recombine with holes on Co2+ level.

Fig. 7. Sketch of the photochromic process in LiNbO3: Fe: Co. The solid and dash arrows denote the sensitizing and bleaching processes, respectively.

In LiNbO3: Fe: Co, two levels (Fe3+ and Co2+) are involved in the photochromic process, which is similar to the case of LiNbO3: Fe: Mn (Fe3+ and Mn2+) [10

A. Adibi, K. Buse, and D. Psaltis, “Two-center holographic recording,” J. Opt. Soc. Am. B 18, 584–601 (2001). [CrossRef]

]. However, in LiNbO3: Fe: Co, electrons transfer from O2- to Fe3+ level directly through CT process under UV irradiation, which is different from the indirect transfer of electrons from Mn2+ to Fe3+ level via the conduction band in LiNbO3: Fe: Mn. Faster sensitization is found in LiNbO3: Fe: Co, as compared with the previous result obtained in LiNbO3: Fe: Mn. This is probably because the direct transfer of electrons in LiNbO3: Fe: Co is more efficient than the indirect transfer of electrons in LiNbO3: Fe: Mn. Additionally, the Co2+ level in LiNbO3: Fe: Co cannot be photoexcited and only exists as the recombination center for holes and electrons, which is also different from the photorefractive levels in LiNbO3: Fe: Mn. In the work of Lee et al., Tb codoping can also induce significant ULIA in Fe-doped LN crystals, and the ULIA is attributed to the valence change from Fe3+ to Fe2+ as well. However, this phenomenon only exists in near-stoichiometric crystals and is not found in congruent ones [8

M. Lee, S. Takekawa, Y. Furukawa, Y. Uchida, K. Kitamura, H. Hatano, and S. Tanaka, “Photochromic effect in near-stoichiometric LiNbO3 and two-color holographic recording,” J. Appl. Phys. 88, 4476–4485 (2000). [CrossRef]

].

From the bleaching and sensitizing time constants, we can estimate the optimum ratio of recording and sensitizing intensities for two-color recording with green and UV light [10

A. Adibi, K. Buse, and D. Psaltis, “Two-center holographic recording,” J. Opt. Soc. Am. B 18, 584–601 (2001). [CrossRef]

]. Comparing the insets of Fig. 6(a) and (b), we find the optimum intensity ratio approximately ranging from 35 to 40. For example, if we choose 100 mW/cm2 as the UV intensity, we find the sensitizing time constant for this intensity is around 65s and the corresponding bleaching intensity with the same time constant is about 3700 mW/cm2, which yields a ratio of 37. The ratio range in our case is slightly higher than that (25~30) for LiNbO3: Fe: Mn [10

A. Adibi, K. Buse, and D. Psaltis, “Two-center holographic recording,” J. Opt. Soc. Am. B 18, 584–601 (2001). [CrossRef]

], which may be due to the fast sensitization in LiNbO3: Fe: Co. The higher ratio is advantageous to producing strong gratings in two-color recording.

The storage time of the photoinduced index is another important issue concerning two-color recording. Generally, the storage time is connected with the stability of the level on which the photoinduced index is recorded. For example, LiNbO3: Mn is proved to have a longer storage time than LiNbO3: Fe because the deeper Mn level is more stable than Fe level [19

Y. P. Yang, D. Psaltis, M. Luennemann, D. Berben, U. Hartwig, and K. Buse, “Photorefractive properties of lithium niobate crystals doped with manganese,” J. Opt. Soc. Am. B 20, 1491–1502 (2003). [CrossRef]

]. In LiNbO3: Fe: Co, the photoinduced index should be recorded finally in Co level. Thus, the energy and stability of the Co level may govern the storage time. As mentioned above, Co impurity has no absorption suitable for photoexciting electrons with visible light, which indicates that Co level should be relatively deep and stable as compared with Fe and Mn levels. Therefore, LiNbO3: Fe: Co is expected to have relatively long storage time. Further experiments are underway to prove this suggestion.

5. Conclusion

In this paper, the strong photochromic effect was found in LiNbO3: Fe: Co crystals. The crystal can be darkened by UV light and bleached by visible light. For both the virgin and sensitized states, UV-VIS-NIR absorption and EPR spectra were measured, and the one-color recording sensitivities were also studied. The results showed that a large number of Fe2+ and Co3+ ions appear in the sensitized state. Based on these results, we explained the photochromic mechanism in LiNbO3: Fe: Co as follows. During sensitization, electrons transfer from O2- to Fe3+ directly while holes are thermally excited from O- into the valence band and then partly trapped by Co2+, which leads to the darkening of the crystal. In bleaching process, electrons are excited from Fe2+ to the conduction band by green light and recombine with holes on the Co2+ level. Sensitizing/bleaching experiments were also carried out in LiNbO3: Fe: Co crystals. Fast sensitization process found for this material was attributed to the direct transfer of electrons from O2- to Fe3+ level through CT process. In addition, we also got the optimum ratio of the recording and sensitizing intensities for two-color recording. The relatively high ratio was attributed to the fast sensitization in LiNbO3: Fe: Co crystals.

Acknowledgements

This work is partly supported by the National Natural Science Foundation of China (Grant Nos. 60578019 and 50472034) and Hebei Natural Science Foundation (E2005000048 and 2007000119). We thank the referees for their valuable comments and Dr. Shengping Chen for his English polishing.

References and links

1.

P. Günter and J. P. Huignard, Photorefractive Materials and Their Applications , Vols. I and II, (Springer-Verlag, Heidelberg, 1989).

2.

K. Buse, “Light-induced charge transport processes in photorefractive crystals II: Materials,” Appl. Phys. B 64, 391–407 (1997). [CrossRef]

3.

K. Buse, A. Adibi, and D. Psaltis, “Non-volatile holographic storage in doubly doped lithium niobate crystals,” Nature 393, 665–668 (1998). [CrossRef]

4.

L. Y Ren, L. R. Liu, D. A. Liu, Ch. H. Zhou, and G. G. Li, “Experimental and theoretical study of non-volatile photorefractive holograms in doubly doped LiNbO3:Fe:Cu,” Opt. Mater. 23, 261–267 (2003). [CrossRef]

5.

W. Phillips, J. J. Amodei, and D. L. Staebler, “Optical and holographic storage properties of transition metal doped lithium niobate,” RCA Rev. 33, 94–109 (1972).

6.

D. K. McMillen, T. D. Hudson, J. Wagner, and J. Singleton, “Holographic recording in specially doped lithium niobate crystals,” Opt. Express 12, 491–502 (1998). [CrossRef]

7.

H. Fujita, M. Inoue, and W. Phillips, “Optical properties of Cobalt-doped lithium niobate,” Jpn. J. Appl. Phys. 44, 1909–1917 (1978).

8.

M. Lee, S. Takekawa, Y. Furukawa, Y. Uchida, K. Kitamura, H. Hatano, and S. Tanaka, “Photochromic effect in near-stoichiometric LiNbO3 and two-color holographic recording,” J. Appl. Phys. 88, 4476–4485 (2000). [CrossRef]

9.

M. Lee, I. G. Kim, S. Takekawa, Y. Furukawa, Y. Uchida, K. Kitamura, and H. Hatano, “Electron paramagnetic resonance investigation of the photochromic effect in near-stoichiometric LiNbO3 with applications to holographic storage,” J. Appl. Phys. 89, 5311–5317 (2001). [CrossRef]

10.

A. Adibi, K. Buse, and D. Psaltis, “Two-center holographic recording,” J. Opt. Soc. Am. B 18, 584–601 (2001). [CrossRef]

11.

A. Adibi, K. Buse, and D. Psaltis, “System measure for persistence in holographic recording and application to singly-doped and doubly-doped lithium niobate,” Appl. Opt. 40, 5175–5182 (2001). [CrossRef]

12.

H. Kurz, E. Krätzig, W. Keune, H. Engelmann, U. Gonser, B. Dischler, and A. Räuber, “Photorefractive centers in LiNbO3, studied by optical-, Mössbauer- and EPR-methods,” Appl. Phys. 12, 355–368 (1977). [CrossRef]

13.

Y. N. Choi, I. W. Park, S. S. Kim, S. S. Park, and S. H. Choh, “Electron paramagnetic resonance studies of Co2+ ions in congruent and nearly stoichiometric LiNbO3 single crystals,” J. Phys.: Condens. Matter 11, 4723–4730 (1999). [CrossRef]

14.

D. J. Keeble, M. Loyo-Menoyo, Y. Furukawa, and K. Kitamura, “Electron paramagnetic resonance of Fe3+ in LiNbO3 ,” Phys. Rev. B 71, 224111 (2005). [CrossRef]

15.

K. Buse, “Light-induced charge transport processes in photorefractive crystals I: Models and experimental methods,” Appl. Phys. B 64, 391–407 (1997). [CrossRef]

16.

O. Schirmer, O. Thiemann, and M. Wöehlecke, “Defects in LiNbO3. I. experimental aspects,” J. Phys. Chem. Solids 52, 185–200 (1991). [CrossRef]

17.

D. Rytz, B. A. Wechsler, M. H. Garrett, C. C. Nelson, and R. N. Schwartz, “Photorefractive properties of BaTiO3:Co,” J. Opt. Soc. Am. B 7, 2245–2254 (1990). [CrossRef]

18.

M. H. Garrett, J. Y. Chang, H. P. Jenssen, and C. Warde, “High beam-coupling gain and deep- and shallow-trap effects in cobalt-doped barium titanate, BaTiO3:Co,” J. Opt. Soc. Am. B 9, 1407–1415 (1992). [CrossRef]

19.

Y. P. Yang, D. Psaltis, M. Luennemann, D. Berben, U. Hartwig, and K. Buse, “Photorefractive properties of lithium niobate crystals doped with manganese,” J. Opt. Soc. Am. B 20, 1491–1502 (2003). [CrossRef]

OCIS Codes
(130.3730) Integrated optics : Lithium niobate
(190.5330) Nonlinear optics : Photorefractive optics
(300.1030) Spectroscopy : Absorption

ToC Category:
Materials

History
Original Manuscript: September 10, 2007
Revised Manuscript: November 11, 2007
Manuscript Accepted: November 11, 2007
Published: December 5, 2007

Citation
Wenbo Yan, Yangxian Li, Lihong Shi, Hongjian Chen, Shiguo Liu, Ling Zhang, Ziheng Huang, Shaolin Chen, and Yongfa Kong, "Photochromic effect in LiNbO3: Fe :Co," Opt. Express 15, 17010-17018 (2007)
http://www.opticsinfobase.org/oe/abstract.cfm?URI=oe-15-25-17010


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References

  1. P. Günter and J. P. Huignard, Photorefractive Materials and Their Applications, Vols. I and II, (Springer-Verlag, Heidelberg, 1989).
  2. K. Buse, "Light-induced charge transport processes in photorefractive crystals II: Materials," Appl. Phys. B 64, 391-407 (1997). [CrossRef]
  3. K. Buse, A. Adibi, and D. Psaltis, "Non-volatile holographic storage in doubly doped lithium niobate crystals," Nature 393, 665-668 (1998). [CrossRef]
  4. L. Y Ren, L. R. Liu, D. A. Liu, Ch. H. Zhou, and G. G. Li, "Experimental and theoretical study of non-volatile photorefractive holograms in doubly doped LiNbO3:Fe:Cu," Opt. Mater. 23, 261-267 (2003). [CrossRef]
  5. W. Phillips, J. J. Amodei, and D. L. Staebler, "Optical and holographic storage properties of transition metal doped lithium niobate," RCA Rev. 33, 94-109 (1972).
  6. D. K. McMillen, T. D. Hudson, J. Wagner, and J. Singleton, "Holographic recording in specially doped lithium niobate crystals," Opt. Express 12, 491-502 (1998). [CrossRef]
  7. H. Fujita, M. Inoue, and W. Phillips, "Optical properties of Cobalt-doped lithium niobate," Jpn. J. Appl. Phys. 44, 1909-1917 (1978).
  8. M. Lee, S. Takekawa, Y. Furukawa, Y. Uchida, K. Kitamura, H. Hatano, and S. Tanaka, "Photochromic effect in near-stoichiometric LiNbO3 and two-color holographic recording," J. Appl. Phys. 88, 4476-4485 (2000). [CrossRef]
  9. M. Lee, I. G. Kim, S. Takekawa, Y. Furukawa, Y. Uchida, K. Kitamura, and H. Hatano, "Electron paramagnetic resonance investigation of the photochromic effect in near-stoichiometric LiNbO3 with applications to holographic storage," J. Appl. Phys. 89, 5311-5317 (2001). [CrossRef]
  10. A. Adibi, K. Buse, and D. Psaltis, "Two-center holographic recording," J. Opt. Soc. Am. B 18, 584-601 (2001). [CrossRef]
  11. A. Adibi, K. Buse, and D. Psaltis, "System measure for persistence in holographic recording and application to singly-doped and doubly-doped lithium niobate," Appl. Opt. 40, 5175-5182 (2001). [CrossRef]
  12. H. Kurz, E. Krätzig, W. Keune, H. Engelmann, U. Gonser, B. Dischler, and A. Räuber, "Photorefractive centers in LiNbO3, studied by optical-, Mössbauer- and EPR-methods," Appl. Phys. 12, 355-368 (1977). [CrossRef]
  13. Y. N. Choi, I. W. Park, S. S. Kim, S. S. Park, and S. H. Choh, "Electron paramagnetic resonance studies of Co2+ ions in congruent and nearly stoichiometric LiNbO3 single crystals," J. Phys.: Condens. Matter 11, 4723-4730 (1999). [CrossRef]
  14. D. J. Keeble, M. Loyo-Menoyo, Y. Furukawa, and K. Kitamura, "Electron paramagnetic resonance of Fe3+ in LiNbO3," Phys. Rev. B 71, 224111 (2005). [CrossRef]
  15. K. Buse, "Light-induced charge transport processes in photorefractive crystals I: Models and experimental methods," Appl. Phys. B 64, 391-407 (1997). [CrossRef]
  16. O. Schirmer, O. Thiemann, and M. Wöehlecke, "Defects in LiNbO3. I. experimental aspects," J. Phys. Chem. Solids 52, 185-200 (1991). [CrossRef]
  17. D. Rytz, B. A. Wechsler, M. H. Garrett, C. C. Nelson, and R. N. Schwartz, "Photorefractive properties of BaTiO3:Co," J. Opt. Soc. Am. B 7, 2245-2254 (1990). [CrossRef]
  18. M. H. Garrett, J. Y. Chang, H. P. Jenssen, and C. Warde, "High beam-coupling gain and deep- and shallow-trap effects in cobalt-doped barium titanate, BaTiO3:Co," J. Opt. Soc. Am. B 9, 1407-1415 (1992). [CrossRef]
  19. Y. P. Yang, D. Psaltis, M. Luennemann, D. Berben, U. Hartwig, and K. Buse, "Photorefractive properties of lithium niobate crystals doped with manganese," J. Opt. Soc. Am. B 20, 1491-1502 (2003). [CrossRef]

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