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Optical Materials Express

Optical Materials Express

  • Editor: David J. Hagan
  • Vol. 1, Iss. 3 — Jul. 1, 2011
  • pp: 413–427
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Highly bismuth-substituted, record-performance magneto-optic garnet materials with low coercivity for applications in integrated optics, photonic crystals, imaging and sensing

Mohammad Nur-E-Alam, Mikhail Vasiliev, Viacheslav A. Kotov, and Kamal Alameh  »View Author Affiliations


Optical Materials Express, Vol. 1, Issue 3, pp. 413-427 (2011)
http://dx.doi.org/10.1364/OME.1.000413


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Abstract

We report on the fabrication of radio frequency (RF) sputtered Bi-substituted lutetium iron garnet films doped with aluminum and the results of adjusting the properties of these films by means of co-sputtering deposition using an additional bismuth oxide target. Very attractive optical, magnetic and magneto-optical properties are achieved in these new magneto-optic materials. The high-performance magnetically-soft thin-film engineered materials synthesized have a wide range of potential applications in next-generation integrated optics, magneto-photonics and magnetic field sensors.

© 2011 OSA

1. Introduction

The methods for the calculation of the expected crystal lattice parameters of doped iron-garnet materials containing various rare-earth and metal-ion substitutions have been described in detail in [21

21. A. H. Eschenfelder, Magnetic Bubble Technology (Springer-Verlag, New York, ISBN 3–540–09822–4), 1980.

]. For example, the cubic lattice parameter a of a garnet layer of composition type described by the formula (BiLu)3(FeAl)5O12 can be predicted from the layer stoichiometry by using the following Eq. (1).
a(A)=12.376+0.0828Bi[f.u.]0.031Lu[f.u.]0.0741Al[f.u.]
(1)
where f.u. (formula units) is the number of atoms of each corresponding element substituted into the garnet lattice (the calculation is based on evaluating the effects of substituting each of the atom types shown into the yttrium-iron garnet lattice of parameter 12.376 Å). We found, using Eq. (1), that a garnet material with a composition described by the formula Bi1.8Lu1.2Fe3.6Al1.4O12 is expected to have a lattice parameter of 12.384 Å and would therefore represent a material engineered for almost-perfect lattice-matching with gadolinium gallium garnet (GGG) substrates, which have a lattice parameter of 12.383 Å. High-crystalline-quality iron-garnet materials with high Bi substitutions typically possess crystal lattice parameters exceeding that of GGG significantly and have been deposited so far mostly onto specialized and somewhat rare large-parameter substrate types, like GSGG. In addition, it is rather difficult to obtain garnet-phase layers with Bi substitutions being as large as 1.8 f.u. using LPE processes, however RF sputtering of such materials from oxide-mix-based targets has been demonstrated successfully [13

13. M. Vasiliev, M. N. Alam, V. A. Kotov, K. Alameh, V. I. Belotelov, V. I. Burkov, and A. K. Zvezdin, “RF magnetron sputtered (BiDy)3(FeGa)5O12:Bi2O3 composite garnet-oxide materials possessing record magneto-optic quality in the visible spectral region,” Opt. Express 17(22), 19519–19535 (2009). [CrossRef] [PubMed]

]. This has opened the way for the development of closely substrate-matched and highly-Bi-substituted garnet layers exhibiting very strong specific Faraday rotation and strong in-plane magnetization component (weak uniaxial magnetic anisotropy) simultaneously.

The goal of this work is to investigate and compare the properties and the practicality of these lattice-engineered garnet films sputtered onto GGG (111) and also the glass substrates (Corning Eagle XG). To the best of our knowledge, no characterization data on the sputter-deposited garnet material of this particular composition could be found in the literature published to date. We report the results of optimizing the oven-annealing regimes as well as on the optical, magnetic and magneto-optical properties of Bi1.8Lu1.2Fe3.6Al1.4O12 films, which are found to be very attractive for various optical and magneto-optical applications in non-reciprocal integrated optics, magneto-photonic crystals and waveguides, magnetic field imaging and sensing devices. Experimental results confirm our hypothesis which states that the co-sputtering approach (using an additional bismuth oxide target) will lead to improving the MO quality of garnet films for this material type similarly to the results reported in [13

13. M. Vasiliev, M. N. Alam, V. A. Kotov, K. Alameh, V. I. Belotelov, V. I. Burkov, and A. K. Zvezdin, “RF magnetron sputtered (BiDy)3(FeGa)5O12:Bi2O3 composite garnet-oxide materials possessing record magneto-optic quality in the visible spectral region,” Opt. Express 17(22), 19519–19535 (2009). [CrossRef] [PubMed]

,23

23. M. Vasiliev, M. Nur-E-Alam, K. Alameh, P. Premchander, Y. T. Lee, V. A. Kotov, and Y. P. Lee, Annealing behaviour and crystal structure of RF-sputtered Bi-substituted dysprosium iron-garnet films having excess co-sputtered Bi-oxide content,” J. Phys. D Appl. Phys. 44(7), 075002 (2011). [CrossRef]

].

2. Materials Synthesis and Characterization Techniques

During the sputtering processes, we used low-pressure pure-argon (Ar) plasma; the details of sputtering process conditions used are summarized in Table 1

Table 1. Sputtering Parameters and Process Conditions Used for the Deposition of Magneto-Optic Bi1.8Lu1.2Fe3.6Al1.4O12 Garnet Layers and Garnet-Bismuth Oxide Nanocomposite Derivatives

table-icon
View This Table
. The targets were always pre-sputtered for 10-20 minutes before depositing the films onto the substrates to achieve stable process conditions. The film thicknesses were monitored during the deposition processes using in situ laser reflectometry. The film thicknesses were also re-measured after the deposition using their transmission spectra obtained with a UV/visible spectrophotometer and our thickness-fitting software [13

13. M. Vasiliev, M. N. Alam, V. A. Kotov, K. Alameh, V. I. Belotelov, V. I. Burkov, and A. K. Zvezdin, “RF magnetron sputtered (BiDy)3(FeGa)5O12:Bi2O3 composite garnet-oxide materials possessing record magneto-optic quality in the visible spectral region,” Opt. Express 17(22), 19519–19535 (2009). [CrossRef] [PubMed]

].

A conventional box-furnace-type oven system was used to run the annealing processes for our as-deposited (amorphous) garnet and garnet-oxide thin films. We also performed the annealing heat treatment at a range of different temperatures for one particular batch of garnet-oxide composite thin films and evaluated the annealing effects on the optical and MO properties of our garnet-oxide nanocomposite materials. The optical and MO performance of thin film garnet materials was found to be critically dependent on the annealing temperature and also the process duration used. The annealing processes were run for Bi1.8Lu1.2Fe3.6Al1.4O12 garnet thin films in between a range of temperatures 620-700°C, with 3-5 °C/min temperature ramp-up and ramp-down rates, for a number of different annealing durations. The 3°C/min temperature-ramp rate resulted in micro-crack-free film surfaces observed in films sputtered onto both substrate types. Bi1.8Lu1.2Fe3.6Al1.4O12: Bi2O3 composite films having different vol. % of extra bismuth oxide were subjected to annealing using a range of temperatures in between 610 and 680 °C for different annealing process durations. The annealed thin films were characterized optically, magnetically and magneto-optically by deriving their absorption coefficient spectra and measuring the specific Faraday rotation at several wavelengths. The Faraday rotation hysteresis loops were also measured to characterize the magnetic switching properties. The specific Faraday rotation measurements of films were performed using a Thorlabs PAX polarimeter system and an electromagnet, by recording the azimuth directions of the polarization plane of polarized laser light transmitted through samples. A transmission-mode polarization microscope (Leitz Orthoplan) was used to observe the magnetic domain patterns of garnet films generated by the component of the layers’ magnetization existing in the direction perpendicular to the film plane. Unlike the (BiDy)3(FeGa)5O12 films studied by us previously in detail [13

13. M. Vasiliev, M. N. Alam, V. A. Kotov, K. Alameh, V. I. Belotelov, V. I. Burkov, and A. K. Zvezdin, “RF magnetron sputtered (BiDy)3(FeGa)5O12:Bi2O3 composite garnet-oxide materials possessing record magneto-optic quality in the visible spectral region,” Opt. Express 17(22), 19519–19535 (2009). [CrossRef] [PubMed]

], the films of composition type (BiLu)3(FeAl)5O12 were magnetically-soft, yet showed the high-contrast domain patterns even after a brief contact with a strong permanent magnet (the materials possessed a low remnant magnetization and did not remain in the monodomain state after being subjected to the saturating field).

3. Results and Discussion

3.1 Properties of Sputtered Bi1.8Lu1.2Fe3.6Al1.4O12 Garnet Layers on Glass and GGG Substrates

Bi1.8Lu1.2Fe3.6Al1.4O12 garnet layers of (1000 ± 20) nm thickness were deposited onto glass and GGG substrates. The annealed high-quality thin garnet films were achieved after running the optimized annealing treatments (1 hour at 650 °C for films deposited onto GGG substrates and 3 hours at 630 °C for films on glass substrates). The materials demonstrated an attractive combination of rather high specific Faraday rotation (confirming high Bi substitution levels achieved) and low optical absorption across large parts of the visible spectral range. Very good transparency was observed across the near-infrared range. We derived the absorption coefficient spectrum of the material according to the technique reported in Ref. [16

16. M. J. Steel, M. Levy, and R. M. Osgood, “High Transmission Enhanced Faraday Rotation in One-Dimensional Photonic Crystals with Defects,” IEEE Photon. Technol. Lett. 12(9), 1171–1173 (2000). [CrossRef]

]. Figure 1
Fig. 1 Derived absorption coefficient spectrum showing the upper (red color) and lower limits (brown color) of Bi1.8Lu1.2Fe3.6Al1.4O12 garnet films deposited onto GGG (111) substrates and annealed at 650 °C for 1 h according to the methodology described in Section II. The data points for the MO figure of merit measured using 532 nm, 635 nm and 660 nm light with associated error bars are shown in the inset.
shows the typical absorption spectrum of crystallized Bi1.8Lu1.2Fe3.6Al1.4O12 layers deposited onto GGG (111) substrates, with the upper and lower limits for the absorption coefficients shown. Similar spectra of absorption coefficient were observed on the samples sputtered onto glass (Corning Eagle XG) substrate also. The maximum (measured in optimally-annealed films on GGG substrates) values of Faraday rotation per film thickness of this garnet material type were around 5.9 deg/µm at 532 nm, 1.6 deg/µm at 635 nm and 1.07 deg/µm at 660 nm, and the films also had relatively low absorption, which led to high MO figures of merit.

These properties, together with their magnetically-soft behavior, make sputtered films of composition Bi1.8Lu1.2Fe3.6Al1.4O12 very attractive for use in different magneto-optic applications and in novel photonic components, for example in garnet waveguides [25

25. T. Mizumoto, S. Mashimo, T. Ida, and Y. Naito, “In-plane Magnetized Rare Earth Iron Garnet for a Waveguide Optical Isolator Employing Nonreciprocal Phase Shift,” IEEE Trans. Magn. 29(6), 3417–3419 (1993). [CrossRef]

]. We measured the MO quality factors (2θF/α) of Bi1.8Lu1.2Fe3.6Al1.4O12 garnet layers deposited onto GGG (111) substrates and obtained values of 13.9° ( ± 1.6°) at 532 nm, 15.7° ( ± 2°) at 635 nm and 12.7° ( ± 0.7°) at 660 nm; these values were lower by about 15-20% in films deposited onto glass.

Figure 2
Fig. 2 Hysteresis loops of specific Faraday rotation measured at 532 nm in sputtered Bi1.8Lu1.2Fe3.6Al1.4O12 garnet films deposited at 250 °C onto (a) GGG substrate (annealed for 1 h at 650 °C), (b) glass substrate (annealed for 3 h at 630 °C). Insets show the measured coercive force, saturation field and the magnetic field sensitivity values at 532 and 635 nm within the linear ranges of magnetization, and (c) hysteresis loop of specific Faraday rotation measured at 532 nm in sputtered Bi1.8Lu1.2Fe3.6Al1.4O12 garnet films of 650 nm deposited onto GGG at 680 °C substrate temperature annealed for 3 h at 630 °C.
shows the hysteresis loops of specific Faraday rotation measured at 532 nm in films sputtered onto GGG (111) and also glass substrates using 250 °C substrate temperature (a, b) and also the same data for a film deposited onto GGG at 680 °C (c). The measured coercive force for the films sputtered at 250 °C on GGG substrates was about 45 Oe, while the coercivity of the films on glass substrates was near 100 Oe (Fig. 2 (a, b)). We observed a much lower coercive force value of below 20 Oe in films on GGG substrates prepared at a higher substrate temperature of 680 °C (Fig. 2 (c)). During hysteresis measurements, the external magnetic field was applied in the direction perpendicular to the film plane, and parallel to the light propagation direction. The almost-linear character of magnetization curves observed below saturation indicates that a significant component of the film’s magnetization lies in the film plane. However, the magnetization vectors of the films on both substrate types also had a perpendicular component, which resulted in the observations of maze-type magnetic domain patterns by polarization microscopy and also using magnetic force microscopy (NT-MDT Nova Scanning Probe Nanolaboratory).Within the linear magnetization range, a rather high Faraday-effect magnetic field sensitivity (the ratio of increments of Faraday rotation to magnetic field) of up to 42.8 °/(cm·Oe) was measured at 635 nm, which even exceeds the previously-reported value of 13 °/(cm·Oe) measured in epitaxial (BiLu)3(FeGa)5O12 films obtained by LPE [22

22. N. Adachi, K. Obata, T. Okuda, T. Machi, and N. Koshizuka, “Synthesis of Bi-Lu-substituted Iron Garnet Films for Visualization of Magnetic Flux in High-Tc Superconductors,” Jpn. J. Appl. Phys. 41 (Part1, 10), 5986–5990 (2002).

]. The domain structures observed in our garnet and garnet-oxide composite thin films in the absence of externally applied magnetic fields is shown in Fig. 3
Fig. 3 Regular maze-type domains were observed in sputtered typical Bi1.8Lu1.2Fe3.6Al1.4O12 garnet films onto GGG deposited onto GGG substrate at (a) 250 °C T(sub) (annealed for 1 h @ 650 °C, (b) 680 °C T(sub) (annealed for 3 h @ 630 °C) and (c) Bi1.8Lu1.2Fe3.6Al1.4O12: Bi2O3 (4.5 vol. %) composite garnet-oxide films (annealed for 10 hrs @ 610 °C) using the transmission-mode polarization microscope (Leitz Orthoplan) at high magnification (630 X).
. An average domain width of about 1 micron was observed in films of 1 µm thickness.

The attractive properties of Bi1.8Lu1.2Fe3.6Al1.4O12 garnet material with magnetically-soft behavior show great promise for the future development of different emerging types of reconfigurable nano-photonic devices. Especially important is the possibility of obtaining garnet films with in-plane magnetization, linear magnetization response and good magnetic and MO properties on non-garnet substrates and without resorting to the use of complex crystal growth technologies.

3.2. Properties of Co-sputtered Bi1.8Lu1.2Fe3.6Al1.4O12: Bi2O3 Nanocomposite Layers on Glass and GGG Substrates

Bi1.8Lu1.2Fe3.6Al1.4O12: Bi2O3 nanocomposite layers having different volumetric fractions of extra Bi2O3 (4.5-20 vol. %) were produced and then crystallized using a high temperature annealing system. The optical and MO properties of all composite films were characterized. Figure 4
Fig. 4 Transmission spectra of several 1050nm-thick Bi1.8Lu1.2Fe3.6Al1.4O12: Bi2O3 (4.5 vol. %) composite garnet-oxide layers (samples from the same deposition batch) sputtered onto monocrystalline GGG (111) and also onto glass (Corning Eagle XG) substrates and post-deposition annealed for 5 h at 610°C and at 615°C; the inset shows a schematic diagram of the power transmission spectrum measurement using a UV/VIS spectrophotometer. The measured percentage of the incident optical power transmitted through the substrate/film system is plotted (no additional normalization with respect to the blank substrate transmission was applied).
shows the transmission spectra of several annealed garnet-oxide composite films of 1050 nm thickness sputtered onto both glass and garnet substrates measured using a UV/VIS spectrophotometer (Beckman Coulter D 640 B). Non-uniformity effects were not observed after the co-sputter deposition of amorphous oxide-mixed films or after running the annealing heat treatment processes inside the oven. Significantly, lower absorption coefficients were obtained in garnet-oxide composite films across the visible spectral region compared to Bi1.8Lu1.2Fe3.6Al1.4O12 garnet layers as shown in Fig. 5
Fig. 5 Derived absorption spectra of Bi1.8Lu1.2Fe3.6Al1.4O12 and several Bi1.8Lu1.2Fe3.6Al1.4O12: Bi2O3 composite films sputtered onto GGG (111) substrates; the excess content of Bi2O3 and the annealing regimes for the typical garnet and the co-sputtered composite films are mentioned.
. The addition of extra bismuth oxide didn’t have much impact on the Faraday rotation of the films but it did improve the optical quality noticeably, consequently improving the magneto-optic quality in terms of MO figure of merit up to more than 50° at 635 nm.

The optical and MO properties of garnet materials were critically dependent on the optimization of annealing process parameters, and the optimization of all annealing process parameters for each garnet composition type was a time-consuming process since the annealing behavior of films is strongly composition-dependent [13

13. M. Vasiliev, M. N. Alam, V. A. Kotov, K. Alameh, V. I. Belotelov, V. I. Burkov, and A. K. Zvezdin, “RF magnetron sputtered (BiDy)3(FeGa)5O12:Bi2O3 composite garnet-oxide materials possessing record magneto-optic quality in the visible spectral region,” Opt. Express 17(22), 19519–19535 (2009). [CrossRef] [PubMed]

]. Bi1.8Lu1.2Fe3.6Al1.4O12: Bi2O3 (4.5 vol. % excess bismuth oxide) composite films were annealed using many possible approaches to thermal treatment, and it was found that the optimized annealing temperatures were between 610 and 620 °C and the optimized time durations varied between 3 and 20 hours. Significant effects of the annealing temperature variation on both the optical and MO properties were observed in this material type. The optimized absorption coefficient spectra achieved in Bi1.8Lu1.2Fe3.6Al1.4O12: Bi2O3 (4.5 vol. % of excess Bi2O3) garnet-oxide composite films sputtered onto GGG (111) substrates and annealed at 610-620 °C for different annealing time durations are shown in Fig. 6
Fig. 6 Derived absorption spectra of Bi1.8Lu1.2Fe3.6Al1.4O12: Bi2O3 (4.5 vol. % of excess Bi2O3) garnet-oxide composite films sputtered onto GGG (111) substrates and annealed at 610-620 °C for different annealing time durations as specified.
.

Figure 7
Fig. 7 The data points showing the summary of optimization of annealing temperature and annealing processes duration used to crystallize the typical Bi1.8Lu1.2Fe3.6Al1.4O12 garnet layer deposited at 250 °C and 680 °C substrates’ temperature and several composite Bi1.8Lu1.2Fe3.6Al1.4O12: Bi2O3 films of having excess Bi2O3 onto GGG (111) substrate.
shows the summary of the optimization results for the annealing regimes used to crystallize the garnet and garnet-oxide amorphous layers and also the values of best-achieved MO figures of merit (data points measured using a 635 nm plane-polarized laser source). These experimental results provide a reliable source of data for further studies of this interesting material, which has been synthesized for the first time. The best-achieved (so far) MO performance characteristics of our garnet and garnet-oxide composite films for two important wavelengths in the visible spectral region are shown in Fig. 8
Fig. 8 Measured quality factor in terms of figure of merit of typical Bi1.8Lu1.2Fe3.6Al1.4O12 garnet layer deposited at 250 °C and 680 °C substrates’ temperature and several best annealed composite Bi1.8Lu1.2Fe3.6Al1.4O12: Bi2O3 films of having 4.5 vol. % excess Bi2O3 onto GGG (111) substrate.
.

The effects of adding bismuth oxide on the coercivity of the films sputtered onto both GGG and glass substrates were observed, and the results are presented in Figs. 9
Fig. 9 Hysteresis loops of specific Faraday rotation measured at 532 nm in sputtered typical Bi1.8Lu1.2Fe3.6Al1.4O12 layer on GGG (annealed for 1 h at 650 °C) and Bi1.8Lu1.2Fe3.6Al1.4O12: Bi2O3 (4.5 vol. %) composite garnet films deposited onto GGG substrate (annealed at 620 °C for 3 h). Insets show the measured coercive force, and saturation field values within the linear ranges of magnetization.
and 10
Fig. 10 Hysteresis loops of specific Faraday rotation measured at 532 nm in sputtered Bi1.8Lu1.2Fe3.6Al1.4O12 garnet films on glass substrate (annealed for 3 h at 630 °C) and Bi1.8Lu1.2Fe3.6Al1.4O12: Bi2O3 (12.5 vol. %) composite garnet films deposited onto glass substrate (annealed at 560 °C for 5 h). Insets show the measured coercive force and saturation field within the linear ranges of magnetization.
. Comparatively, lower coercive force values were measured in composite films sputtered onto both types of substrates. We believe that better crystalline quality, lower coercive force values and even higher magnetic field sensitivity can be achieved in our films sputtered onto GGG substrates, if high-substrate-temperature deposition regime is optimized to achieve the conditions suitable for epitaxial-quality layer growth (sputter epitaxy).

Note that two experimental setups were used to confirm the calibration accuracy of the Thorlabs PAX polarimeter that was used for Faraday rotation measurements, namely (i) the direct measurements of optical power transmitted through the sample and the use of an analyzer rotated 45 degrees with respect to the polarisation direction of the incident laser light, under various magnetization conditions, and (ii) a well-calibrated measurement setup based on the detection of polarisation components. The measured Faraday rotations for both setups were in excellent agreement. The Thorlabs PAX polarimeter had a high dynamic range of 70 dB, a broad wavelength range, and an accuracy of ± 0.2°.

The surface morphology as well as surface magnetic field distribution topography of Bi1.8Lu1.2Fe3.6Al1.4O12: Bi2O3 composite films having 4.5 vol. % and 12.5 vol. % of excess bismuth oxide sputtered onto GGG substrates have been characterized using atomic force microscopy (AFM) and magnetic force microscopy (MFM). Figure 11
Fig. 11 Scanning-probe (AFM/MFM) images of garnet-oxide composite thin films having 4.5 vol. % and 12.5 vol. % extra bismuth oxide sputtered onto GGG (111) substrates. (a-b) 3D images showing the topography (5 × 5 µm sample area) of a 1050 nm thick Bi1.8Lu1.2Fe3.6Al1.4O12:Bi2O3 (4.5 vol. %) composite film annealed for 5 h at 615 °C and its surface magnetism features measured across a 25 × 25 µm sample area; (c-d) 2D AFM topography (c) and (d) an AC magnetic force magnitude map (processed feedback phase image) obtained from a 1.2 × 1.2 µm sample area of a Bi1.8Lu1.2Fe3.6Al1.4O12:Bi2O3 (12.5 vol. %) nanocomposite film annealed for 5 h at 580 °C. The black-white color palette of image (d) represents the measured RMS strength of the AC magnetic interaction force between the tip and surface, and the color map shown was obtained using a halved algebraic sum of the phase image data map obtained and its inverted phase image data map, so that only the magnitude of the magnetic interaction force is represented. The white-colored pixels correspond to the minima locations of the magnetic interaction force.
shows the scanning probe microscopy inspection results for garnet samples of composition Bi1.8Lu1.2Fe3.6Al1.4O12: Bi2O3 (4.5 vol. %) presented as 3D images of the surface features and surface magnetic field distribution (Fig. 11 (a and b)), and also shows the results for a Bi1.8Lu1.2Fe3.6Al1.4O12: Bi2O3 (12.5 vol. %) film presented as 2D images (Fig. 11(c, d)). The garnet samples were scanned using semi-contact mode of probe-interaction to obtain the feedback-phase and also the surface topography data simultaneously from the same scan area. The MFM cantilever tip used was cobalt-coated to enable the magnetic-force interaction representation through the phase of the cantilever feedback signal. Nano-crystalline surface microstructure and its associated surface roughness features of the garnet films were observed from the obtained high-contrast images extracted from the measured feedback-phase images and topography data. The magnetic domains structure and the map of magnetic interaction force between the cantilever tip and sample surface were also imaged.

It is important to notice that Figs. 11(a, b) reveal that the addition of extra bismuth oxide results in bismuth-rich MO garnet-phase grains surrounded by transparent non-magnetic bismuth oxide regions. While the measured overall Faraday rotation of the composite film was not improved, the measured overall optical transmission was considerably increased, leading to significant increase in MO figure of merit.

To the best of our knowledge, this is the first report on the properties of this advanced MO material type (garnet-oxide nanocomposites of class Bi1.8Lu1.2Fe3.6Al1.4O12:Bi2O3) appearing in the literature published to date. Our work is ongoing and further results, especially on the crystal structure and microstructural details of Bi1.8Lu1.2Fe3.6Al1.4O12 garnet layers and their co-sputtered nanocomposite derivatives will be reported elsewhere.

4. Conclusion

We have studied the RF sputtering deposition and oven annealing processes required for the manufacture of high-performance magneto-optic films of composition types Bi1.8Lu1.2Fe3.6Al1.4O12 and (BiLu)3(FeAl)5O12:Bi2O3 on garnet and glass substrates. The optical, magnetic and magneto-optical properties of a range of highly Bi-substituted lutetium iron-aluminum garnet layers have been characterized in detail and reported for the first time. Significantly improved magneto-optical figures of merit have been achieved using the co-sputtering bismuth oxide-mixing approach, and the results confirm that this synthesis method is suitable for a wide range of Bi-substituted MO garnet materials. The developed garnet and garnet-oxide thin film materials possess a combination of properties which are highly promising in regard to the future development of garnet waveguides, non-reciprocal integrated-optics components as well as magnetic field imaging and sensing devices.

Acknowledgment

This research is supported by the Faculty of Computing, Health and Science, Edith Cowan University. We also acknowledge the support provided by the Department of Nanobio Materials and Electronics, Gwangju Institute of Science and Technology (South Korea).

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M. Vasiliev, M. N. Alam, V. A. Kotov, K. Alameh, V. I. Belotelov, V. I. Burkov, and A. K. Zvezdin, “RF magnetron sputtered (BiDy)3(FeGa)5O12:Bi2O3 composite garnet-oxide materials possessing record magneto-optic quality in the visible spectral region,” Opt. Express 17(22), 19519–19535 (2009). [CrossRef] [PubMed]

14.

I. L. Lyubchanskii, N. N. Dadoenkova, M. I. Lyubchanskii, E. A. Shapovalov, and Th. Rasing, “Magnetic photonic crystals,” J. Phys. D Appl. Phys. 36(18), R277–R287 (2003). [CrossRef]

15.

M. Vasiliev, K. Alameh, V. Belotelov, V. A. Kotov, and A. K. Zvezdin, ““Magnetic Photonic Crystals: 1-D Optimization and Applications for the Integrated Optics Devices,” IEEE/OSA,” J. Lightwave Technol. 24(5), 2156–2162 (2006). [CrossRef]

16.

M. J. Steel, M. Levy, and R. M. Osgood, “High Transmission Enhanced Faraday Rotation in One-Dimensional Photonic Crystals with Defects,” IEEE Photon. Technol. Lett. 12(9), 1171–1173 (2000). [CrossRef]

17.

M. Vasiliev, V. A. Kotov, K. E. Alameh, V. I. Belotelov, and A. K. Zvezdin, “Novel Magnetic Photonic Crystal Structures for Magnetic Field Sensors and Visualizers,” IEEE Trans. Magn. 44(3), 323–328 (2008). [CrossRef]

18.

M. Nur-E-Alam, M. Vasiliev, and K. Alameh, Nano-structured magnetic photonic crystals for magneto-optic polarization controllers at the communication-band wavelengths,” Opt. Quantum Electron. 41(9), 661–669 (2009). [CrossRef]

19.

P. Tierno, F. Sagués, T. H. Johansen, and T. M. Fischer, “Colloidal transport on magnetic garnet films,” Phys. Chem. Chem. Phys. 11(42), 9615–9625 (2009). [CrossRef] [PubMed]

20.

A. Abdelrahman, M. Vasiliev, K. Alameh, and P. Hannaford, “Asymmetrical two-dimensional magnetic lattices for ultracold atoms,” Phys. Rev. A 82(1), 012320 (2010). [CrossRef]

21.

A. H. Eschenfelder, Magnetic Bubble Technology (Springer-Verlag, New York, ISBN 3–540–09822–4), 1980.

22.

N. Adachi, K. Obata, T. Okuda, T. Machi, and N. Koshizuka, “Synthesis of Bi-Lu-substituted Iron Garnet Films for Visualization of Magnetic Flux in High-Tc Superconductors,” Jpn. J. Appl. Phys. 41 (Part1, 10), 5986–5990 (2002).

23.

M. Vasiliev, M. Nur-E-Alam, K. Alameh, P. Premchander, Y. T. Lee, V. A. Kotov, and Y. P. Lee, Annealing behaviour and crystal structure of RF-sputtered Bi-substituted dysprosium iron-garnet films having excess co-sputtered Bi-oxide content,” J. Phys. D Appl. Phys. 44(7), 075002 (2011). [CrossRef]

24.

J. P. Krumme, V. Doormann, B. Strocka, and P. Willich, “Selected-area sputter epitaxy of iron-garnet films,” J. Appl. Phys. 60(6), 2065–2068 (1986). [CrossRef]

25.

T. Mizumoto, S. Mashimo, T. Ida, and Y. Naito, “In-plane Magnetized Rare Earth Iron Garnet for a Waveguide Optical Isolator Employing Nonreciprocal Phase Shift,” IEEE Trans. Magn. 29(6), 3417–3419 (1993). [CrossRef]

OCIS Codes
(130.3130) Integrated optics : Integrated optics materials
(160.3820) Materials : Magneto-optical materials
(310.3840) Thin films : Materials and process characterization

ToC Category:
Thin Films

History
Original Manuscript: May 13, 2011
Revised Manuscript: June 8, 2011
Manuscript Accepted: June 12, 2011
Published: June 17, 2011

Citation
Mohammad Nur-E-Alam, Mikhail Vasiliev, Viacheslav A. Kotov, and Kamal Alameh, "Highly bismuth-substituted, record-performance magneto-optic garnet materials with low coercivity for applications in integrated optics, photonic crystals, imaging and sensing," Opt. Mater. Express 1, 413-427 (2011)
http://www.opticsinfobase.org/ome/abstract.cfm?URI=ome-1-3-413


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References

  1. A. K. Zvezdin and V. A. Kotov, in Modern Magnetooptics and Magnetooptical Materials (Bristol, Institute of Physics Publishing, and Philadelphia), ISBN 075030362X, 1997.
  2. C. F. Buhrer, “Faraday Rotation and Dichroism of Bismuth Calcium Vanadium Iron Garnet,” J. Appl. Phys. 40(11), 4500–4502 (1969). [CrossRef]
  3. G. B. Scott and D. E. Lacklison, “Magnetooptic Properties and Applications of Bismuth Substituted Iron Garnets,” IEEE Trans. Magn. 12(4), 292–311 (1976). [CrossRef]
  4. T. Hibiya, Y. Morishige, and J. Nakashima, “Growth and Characterization of Liquid-Phase Epitaxial Bi-Substituted Iron Garnet Films for Magneto-Optic Application,” Jpn. J. Appl. Phys. 24, 1316–1319 (1985). [CrossRef]
  5. T. Okuda, N. Koshizuka, K. Hayashi, T. Takahashi, H. Kotani, and H. Yamamoto, “Epitaxial growth of Bi-substituted yttrium iron garnet films by ion beam sputtering,” Advances in Magneto-Optics, Proc. Int. Symp. Magneto-Optics, J. Magn. Soc. Jpn. 11, Supplement S1, 179–182 (1987).
  6. Y. H. Kim, J. S. Kim, S. I. Kim, and M. Levy, “Epitaxial Growth and Properties of Bi-Substituted Yttrium-Iron-Garnet Films Grown on (111) Gadolinium-Gallium-Garnet Substrates by Using rf Magnetron Sputtering,” J. Korean Phys. Soc. 43(3), 400–405 (2003).
  7. Y. Okamura, T. Kawakami, and S. Yamamoto, “Sputter epitaxy of cerium yttrium iron garnet films on neodymium gallium garnet substrates,” J. Appl. Phys. 81(8), 5653–5655 (1997). [CrossRef]
  8. M. Gomi, T. Tanida, and M. Abe, “RF Sputtering of Highly Bi-substituted Garnet Films on Glass Substrates for Magneto-Optic Memory,” J. Appl. Phys. 57(8), 3888–3890 (1985). [CrossRef]
  9. S. Kang, S. Yin, V. Adyam, Q. Li, and Y. Zhu, “Bi3Fe4Ga1O12 Garnet Properties and Its Application to Ultrafast Switching in the Visible Spectrum,” IEEE Trans. Magn. 43(9), 3656–3660 (2007). [CrossRef]
  10. S. Kahl, A. M. Grishin, S. I. Khartsev, K. Kawano, and J. S. Abell, “Bi3Fe5O12 Thin Film Visualizer,” IEEE Trans. Magn. 37(4), 2457–2459 (2001). [CrossRef]
  11. M. Vasiliev, P. C. Wo, K. Alameh, P. Munroe, Z. Xie, V. A. Kotov, and V. I. Burkov, “Microstructural characterization of sputtered garnet materials and all-garnet magnetic heterostructures: establishing the technology for magnetic photonic crystal fabrication,” J. Phys. D Appl. Phys. 42(13), 135003 (2009). [CrossRef]
  12. A. K. Bandyopadhyay, S. E. Rios, S. Fritz, J. Garcia, J. Contreras, and C. J. Gutierrez, “Ion Beam Sputter-Fabrication of Bi-YIG Films for Magnetic Photonic Applications,” IEEE Trans. Magn. 40(4), 2805–2807 (2004). [CrossRef]
  13. M. Vasiliev, M. N. Alam, V. A. Kotov, K. Alameh, V. I. Belotelov, V. I. Burkov, and A. K. Zvezdin, “RF magnetron sputtered (BiDy)3(FeGa)5O12:Bi2O3 composite garnet-oxide materials possessing record magneto-optic quality in the visible spectral region,” Opt. Express 17(22), 19519–19535 (2009). [CrossRef] [PubMed]
  14. I. L. Lyubchanskii, N. N. Dadoenkova, M. I. Lyubchanskii, E. A. Shapovalov, and Th. Rasing, “Magnetic photonic crystals,” J. Phys. D Appl. Phys. 36(18), R277–R287 (2003). [CrossRef]
  15. M. Vasiliev, K. Alameh, V. Belotelov, V. A. Kotov, and A. K. Zvezdin, ““Magnetic Photonic Crystals: 1-D Optimization and Applications for the Integrated Optics Devices,” IEEE/OSA,” J. Lightwave Technol. 24(5), 2156–2162 (2006). [CrossRef]
  16. M. J. Steel, M. Levy, and R. M. Osgood, “High Transmission Enhanced Faraday Rotation in One-Dimensional Photonic Crystals with Defects,” IEEE Photon. Technol. Lett. 12(9), 1171–1173 (2000). [CrossRef]
  17. M. Vasiliev, V. A. Kotov, K. E. Alameh, V. I. Belotelov, and A. K. Zvezdin, “Novel Magnetic Photonic Crystal Structures for Magnetic Field Sensors and Visualizers,” IEEE Trans. Magn. 44(3), 323–328 (2008). [CrossRef]
  18. M. Nur-E-Alam, M. Vasiliev, and K. Alameh, Nano-structured magnetic photonic crystals for magneto-optic polarization controllers at the communication-band wavelengths,” Opt. Quantum Electron. 41(9), 661–669 (2009). [CrossRef]
  19. P. Tierno, F. Sagués, T. H. Johansen, and T. M. Fischer, “Colloidal transport on magnetic garnet films,” Phys. Chem. Chem. Phys. 11(42), 9615–9625 (2009). [CrossRef] [PubMed]
  20. A. Abdelrahman, M. Vasiliev, K. Alameh, and P. Hannaford, “Asymmetrical two-dimensional magnetic lattices for ultracold atoms,” Phys. Rev. A 82(1), 012320 (2010). [CrossRef]
  21. A. H. Eschenfelder, Magnetic Bubble Technology (Springer-Verlag, New York, ISBN 3–540–09822–4), 1980.
  22. N. Adachi, K. Obata, T. Okuda, T. Machi, and N. Koshizuka, “Synthesis of Bi-Lu-substituted Iron Garnet Films for Visualization of Magnetic Flux in High-Tc Superconductors,” Jpn. J. Appl. Phys. 41 (Part1, 10), 5986–5990 (2002).
  23. M. Vasiliev, M. Nur-E-Alam, K. Alameh, P. Premchander, Y. T. Lee, V. A. Kotov, and Y. P. Lee, Annealing behaviour and crystal structure of RF-sputtered Bi-substituted dysprosium iron-garnet films having excess co-sputtered Bi-oxide content,” J. Phys. D Appl. Phys. 44(7), 075002 (2011). [CrossRef]
  24. J. P. Krumme, V. Doormann, B. Strocka, and P. Willich, “Selected-area sputter epitaxy of iron-garnet films,” J. Appl. Phys. 60(6), 2065–2068 (1986). [CrossRef]
  25. T. Mizumoto, S. Mashimo, T. Ida, and Y. Naito, “In-plane Magnetized Rare Earth Iron Garnet for a Waveguide Optical Isolator Employing Nonreciprocal Phase Shift,” IEEE Trans. Magn. 29(6), 3417–3419 (1993). [CrossRef]

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