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Third Day Poster Session, 17 June 2010 - NanoTR-VI

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P and<br />

<strong>Poster</strong> <strong>Session</strong>, Thursday, <strong>June</strong> <strong>17</strong><br />

Theme F686 - N1123<br />

Magneto-Optical and Optical Properties of Cerium Substituted Yttrium Iron Garnet Thin Films<br />

Prepared by Sol-Gel Process<br />

1<br />

2<br />

2<br />

1<br />

1<br />

UYavuz ÖztürkUP P*, Mustafa ErolP P, Erdal CelikP P, Ömer MermerP brahim AvgnP<br />

PEge University Electrical and Electronics Department, 35100 Bornova, Izmir-TURKEY.<br />

PDokuz Eylul University, Department of Metallurgical and Materials Engineering, Tınaztepe Kampüsü, 35160 Buca, Izmir-TURKEY.<br />

2<br />

1<br />

Abstract- Cerium doped yttrium iron garnet (CeRxRYR3-xRFeR5ROR12R; Ce-YIG) magneto-optical thin films were fabricated on Si (100) and fused<br />

silica substrates by using sol-gel method for magneto-optical applications. Ce doped YIG films with nano size regions fabricated with dip<br />

and spin coating from two different solutions prepared from Ce, Y and Fe-based precursors, solvent and chelating agent at low temperature<br />

o<br />

using a sol-gel technique. Coated thin films annealed at the temperature range of 800 and 1000 P PC for 2 h in air. Optical, morphological,<br />

structural and magnetic properties were investigated by scanning electron microscopy (SEM), spectraphotometer, magneto-optical<br />

measurement set up and vibrating sample magnetometer (VSM).<br />

Ce doped yttrium iron garnet (CeRxRYR3-xRFeR5ROR12R; Ce-YIG)<br />

is a promising material for magneto-optical applications<br />

because of its large specific Faraday rotation and low<br />

propagation loss [1,2]. The available Ce-YIG material<br />

research has mainly on a single crystals and thin films [1-<br />

4]. Polycrystalline Ce-YIG and its optical and magnetooptical<br />

properties has rarely been investigated. In this<br />

study, we have investigated optical properties of garnet<br />

films synthesized by using sol-gel method. Sol-gel<br />

processing offers considerable advantages such as better<br />

mixing of the starting materials, excellent chemical<br />

homogeneity in the final product and coating large areas<br />

without expensive devices [5].<br />

We applied sol-gel process with following order. Ce, Y<br />

and Fe based precursor materials dissolved in methanol<br />

and glacial acetic acid (GAA) were used as a solvent for<br />

the synthesis of materials. Si(100) and fused silica were<br />

used as substrates. Ce-YIG gel solutions with completely<br />

solved (Sol A) and unsolved cerium content (Sol B) were<br />

dip-coated and spin coated on the substrates at room<br />

temperature. This process was followed by heat treatment<br />

o<br />

by annealing films between 800-1000 P PC for 2 hours in<br />

air.<br />

Figure1.a shows the SEM results of Ce:YIG annealed at<br />

1000 °C. There are two kinds of region observed. Darker<br />

regions have less Si content compared to the lighter<br />

regions according to the EDS results. So as can be seen<br />

Fig. 2.a there are interaction between substrate and garnet<br />

phase which leads to nucleation. Fig. 1.b shows SEM<br />

result of Ce-YIG prepared with Sol B annealed at 800°C.<br />

magnetization value of Ce-YIG (43 emu/cc) is lower than<br />

that of bulk YIG (136 emu/cc) [6]. The magneto-optical<br />

measurement set up was build up according to previously<br />

published paper [7]. By using this set up faraday and kerr<br />

effects of the Ce doped YIG films were measured. The<br />

optical constant of these films were determined using<br />

transmittance and reflectance spectra.<br />

(a)<br />

Figure 2. VSM and magneto-optical result of Ce-YIG prepared<br />

(a) on fused silica with Sol A at 1000 °C and (b) on Si(00) with<br />

Sol B at 800 °C<br />

As conclusion, cerium-doped YR3RFeR5ROR12R garnet films<br />

were prepared on Si(100) and fused silica by two different<br />

sol-gel method. Ce:YIG thin films were obtained with<br />

cubic YIG phase and good the surface quality. We<br />

measured transmittance and absorption spectra and also<br />

showed the agreement between magnetisation and<br />

magneto-optical measurements.<br />

This work has been supported by The Scientific and<br />

Technological Research Council of Turkey (TUBITAK).<br />

(b)<br />

* Corresponding author: yavuz.ozturk@ege.edu.tr<br />

(a)<br />

[1] O. Kamada, T. Nakaya, S. Higuchi, Sensors and Actuators A<br />

119 (2005) 345–348<br />

[2] M. Huang, S-Y. Zhang, Appl. Phys. A 74 (2002) <strong>17</strong>7–180<br />

[3] N. Inoue, K. Yamasawa: Elect. Eng. In Jpn. 1<strong>17</strong> (1996) 1<br />

[4] X. Zhou, W. Cheng, F. Lin, X. Ma, W. Shi, Applied Surface<br />

Science 253 (2006) 2108–2112<br />

[5] L.L Hench, J.K. West, Principles of Electronic Ceramics.<br />

John Wiley & Sons, New York (1990)<br />

[6] B. Lax, K.J. Buton, Microwave Ferrites and Ferrimagnetics,<br />

McGraw-Hill, NY, (1962)<br />

[7] S. Polisetty, J. Scheffler, S. Sahoo, Yi Wang, T. Mukherjee,<br />

Xi He, and Ch. Binek, Review Of Scientific Instruments 79<br />

(2008) 055107 _<br />

(b)<br />

Figure 1. SEM result of Ce:YIG prepared at 1000 °C (a) with Sol<br />

A and 800 °C (b) Sol B<br />

The magnetization curve of Ce-YIG phase observed<br />

with VSM at room temperature. The measured saturation<br />

6th Nanoscience and Nanotechnology Conference, zmir, <strong>2010</strong> 632

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