Study of Different Magneto-Optic Materials for Current Sensing Applications

Study of Different Magneto-Optic Materials for Current Sensing Applications

J. Sens. Sens. Syst., 7, 421–431, 2018 https://doi.org/10.5194/jsss-7-421-2018 © Author(s) 2018. This work is distributed under the Creative Commons Attribution 4.0 License. Study of different magneto-optic materials for current sensing applications Sarita Kumari and Sarbani Chakraborty Electrical and Electronics Engineering Department, Birla Institute of Technology, Mesra, Ranchi – 835215, Jharkhand, India Correspondence: Sarita Kumari ([email protected]) Received: 14 August 2017 – Revised: 20 December 2017 – Accepted: 15 May 2018 – Published: 13 June 2018 Abstract. This article discusses the properties of different diamagnetic and paramagnetic materials for a basic current/magnetic field sensor system set up with different relative orientations of analyzers and polarizers. The paper analyzes linearity ranges of different materials and their sensitivity for different wavelengths. Terbium doped glass (TDG), terbium gallium garnet (TGG), doped TGG and dense flint glass materials are used for analysis based on Faraday’s rotation principle. TGG shows high Faraday rotation, temperature stability and high optical quality. Three ranges of the magnetic field have been chosen for performance analysis. The study reveals that doping of praseodymium (Pr3C) on TGG exhibits a better response at 532 nm as well as 1064 nm wavelengths than TGG. At 632.8 nm wavelength, cerium (Ce3C) doped terbium aluminum garnet (TAG) ceramic exhibits better resolution than others. The study has been done for performance analysis of different MO sensors applicable for measurement of various process parameters like current, displacement, and magnetic field. 1 Introduction rial changes the plane of polarization of a linearly polarized light when placed in a magnetic field. This property can be This article is based on analysis of linearity and sensitivity of utilized in designing various sensors if the change in mag- different magneto-optic (MO) materials. The applications of netic field can be associated with any physical variable. It of- magnetic materials are gaining importance in wide fields like fers non-contact sensing techniques for measurement of any industry, defense, astronomy and materials. More research parameter like current, displacement, and magnetic field. It is being carried out in developing new material. Magnetic has gained so much popularity because of many advantages materials are important media for data handling like data over traditional sensing techniques like its immunity to elec- processing, saving and retrieving. Smart card and magnetic tromagnetic interference, stray capacitance as well as envi- strip scanning systems are the most commonly and vastly ronmental effect. The sensor is highly reliable with a quick used applications of the MO effect in our day-to-day life. response. Transmitting and receiving optical data have min- Various magnetic materials are available, such as diamag- imum loss and are least affected by noise compared to other netic, paramagnetic, ferromagnetic and ferrimagnetic. Mag- means of measurement. The Faraday effect can be used for netic materials can be made optically sensitive by doping solid, liquid as well as gaseous media. MO materials must them with rare earth ions. There are 17 types of rare earth ele- have high Verdet constants and high optical transparency for ments available on earth, but the most commonly used are yt- effective performance. The magneto-optical sensor provides trium (Y), neodymium (Nd), gadolinium (Gd), terbium (Tb) a new perspective in sensor designing and testing. and dysprosium (Dy). Chen et al. (2016a, b), Villaverde et The material used to design the sensor is called Faraday al. (1978), and Booth and White (1984) have used rare earth active material or magneto-optic material and the rotation garnets for their study. of the polarization plane is called Faraday rotation (Hecht, In 1845, Faraday found that if a glass block is kept un- 1987; Jenkins and White, 1976; Shurcliff, 1962). Faraday der a strong magnetic field, it becomes optically active (as rotation (θ) is proportional to change in magnetic flux den- reported in Jenkins and White, 1976). Optically active mate- Published by Copernicus Publications on behalf of the AMA Association for Sensor Technology. 422 S. Kumari and S. Chakraborty: Study of different magneto-optic materials for current sensing applications sity B and total optical path length L. Vverdet is the propor- tionality constant and is called a Verdet constant. Materials which have paramagnetic ions show a high Verdet constant, whereas it usually is very small for most of the materials. One example of material consisting of paramagnetic ions is terbium, which includes terbium doped glass (TDG) and ter- bium gallium garnet (TGG) as MO materials. The Faraday rotation changes with variation in wavelength of any MO ma- Figure 1. Schematic diagram of the basic magneto-optic measure- terial. ment system. Many scientists have reported various properties of MO materials such as change in Verdet constant with wavelength, temperature dependency and size scalability. Verdet con- effect (MOKE) microscopy assisted with magneto-optical in- stants of various diamagnetic materials such as fused sil- dicator film (MOIF) (Qiu et al., 2017). Kalska et al. (2008) ica (Dynasil 1001), borosilicate (BK-7) glass and undoped found a shift in the magneto-optic hysteresis curves due to yttrium aluminum garnet (YAG) crystal were calculated by exchange bias in the temperature-dependent magneto-optic Munin et al. (1992) for different wavelengths in the visible hysteresis curve of “quasi-two-dimensional” arrays. Deeter region. It was found that YAG shows a higher Verdet con- et al. (1990, 1994), Deeter (1995) and Wolfe et al. (1992) stant than BK-7 and Dynasil at 632.8 nm wavelength. Us- designed a YIG-based magnetic field sensor. ing the Czochralski (Cz) method, Chen et al. (2016a, b) have Based on a literature survey it is found that MO sen- 3C 3C fabricated Dy doped TGG material and Tm doped TGG sors are being used in many industrial applications, such as material. The Verdet constant and magneto-optical character- measurement of displacement (Bera and Chakraborty, 2011), istics of the materials can be enhanced remarkably by adding magnetic field (Wolfe et al., 1992; Chakraborty and Ku- 3C 3C 3C 3C rare earth ions. The doped (Ce , Pr , Dy and Nd dop- mari, 2015), current (Chakraborty and Bera, 2008; Zubia et ing) TGG shows a 20–30 % higher Verdet constant value than al., 2013), temperature, and vibration. Several studies are pure TGG. Different techniques have been used to measure a reporting on MO material development and its properties Verdet constant of MO materials like pulsed magnetic fields (Munin et al., 1992; Chen et al., 2016a, b; Booth and White, for TGG by Villaverde et al. (1978), the Faraday effect in dia- 1984; Chakraborty and Bera, 2008; Chakraborty and Ku- magnetic glass by Thamaphat et al. (2006), and the ellipsom- mari, 2015). etry technique in different media such as flint glass and water In this context, analysis of sensitivity can be regarded as by Suchat et al. (2011). Faraday rotation of rare earth garnet one of the important performance criteria in sensor design. material is usually inversely proportional to the wavelength It shows how the material behaves with the change in partic- of light, except for yttrium iron garnet (YIG), where the ular parameters. Since terbium doped materials exhibit very Verdet constant increases above 1300 nm wavelength (Booth high rotation, these are very popular and widely used in sen- and White, 1984). Analysis (Chen et al., 2016a, b) shows sor designing. In this paper we are focusing on various MO that YIG has a poor transparency below 1100 nm. For visible materials at different wavelengths and analyzing the sensi- and near-infra-red wavelengths rare earth garnets are imple- tivity of a basic magneto-optic setup under different relative mented for better performance. In 800–1700 nm wavelength, orientations of polarizer and analyzer. Zhao (2001) found higher rotation and low temperature de- pendency of YbBi:YIG material. It exhibits higher linearity, sensitivity and accuracy than pure YIG. At 1550 nm wave- 2 Theory length, Huang and Zhang (2002) doped yttrium (Y3C) and ytterbium (Yb3C) ions in bismuth substituted iron garnet to Figure 1 shows the basic block diagram of a magneto-optic achieve large rotation and high temperature stability. Koerdt measurement setup. For analysis, the basic current measure- et al. (2003) found the Faraday effect in photonic crystals ment setup has been used (Chakraborty and Bera, 2008; filled with transparent liquid at 573 nm. Characterization of Bera and Chakraborty, 2011). It consists of a laser source, MO properties of various MO materials is explained by Do- polarizer, Faraday rotator, analyzer, and photo-detector to nati et al. (1988) for a wide range of Vis-NIR wavelengths. detect the change in plane of polarization. An unpolarized In the visible region, Chakraborty and Bera (2008) devel- monochromatic light beam coming from the laser source be- oped a current sensor based on a null detection technique comes polarized after passing through the polarizer. A lin- and Chakraborty and Kumari (2015) designed a magnetic early polarized monochromatic light beam passes through field sensor using a TDG crystal as an MO sensor. A low- the magneto-optic material under the influence of a strong cost optical current sensor was designed and demonstrated magnetic field, and after passing through the analyzer, the by Zubia et al. (2013). The characterization of applied ten- beam is received by the photo-detector. sile stress is studied with in situ magnetic domain imaging The polarization devices can be expressed in many forms, and their dynamic behaviors by using magneto-optical Kerr such as the Mueller matrix, Jones matrix and state of po- J. Sens. Sens. Syst., 7, 421–431, 2018 www.j-sens-sens-syst.net/7/421/2018/ S. Kumari and S. Chakraborty: Study of different magneto-optic materials for current sensing applications 423 Figure 2.

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