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Featured researches published by Jovan Jevtic.


IEEE Transactions on Circuits and Systems | 2015

A Generic Model of Memristors With Parasitic Components

Maheshwar Pd. Sah; Changju Yang; Hyongsuk Kim; Bharathwaj Muthuswamy; Jovan Jevtic; Leon O. Chua

In this paper, a generic model of memristive systems, which can emulate the behavior of real memristive devices is proposed. Non-ideal pinched hysteresis loops are sometimes observed in real memristive devices. For example, the hysteresis loops may deviate from the origin over a broad range of amplitude A and frequency f of the input signal. This deviation from the ideal case is often caused by parasitic circuit elements exhibited by real memristive devices. In this paper, we propose a generic memristive circuit model by adding four parasitic circuit elements, namely, a small capacitance, a small inductance, a small DC current source, and a small DC voltage source, to the memristive device. The adequacy of this model is verified experimentally and numerically with two thermistors (NTC and PTC) memristors.


Journal of Analytical Atomic Spectrometry | 2016

New inductively coupled plasma for atomic spectrometry: the microwave-sustained, inductively coupled, atmospheric-pressure plasma (MICAP)

Andrew J. Schwartz; Yan Cheung; Jovan Jevtic; Velibor Pikelja; Ashok Menon; Steven J. Ray; Gary M. Hieftje

A novel inductively coupled plasma (ICP), termed the microwave-sustained, inductively coupled, atmospheric-pressure plasma (MICAP), has been developed that operates at microwave frequency (2.45 GHz). To sustain the new plasma, a dielectric resonator ring (fabricated from an advanced technical ceramic) is coupled with a 2.45 GHz microwave field generated from a microwave-oven magnetron. The microwave field induces polarization currents (small shifts in the equilibrium positions of bound electrons) in the resonator that generate an orthogonal magnetic field, analogous to that produced by electrical current within a traditional ICP load coil. This magnetic field is capable of sustaining an annular plasma in either air or nitrogen that can readily accept solution samples in the form of a wet aerosol produced from a conventional nebulizer and a spray chamber. An initial analytical evaluation of the MICAP with radially viewed optical emission spectrometry (OES) revealed that limits of detection ranged from 0.03–70 ppb with relative standard deviations from 0.7–2.0%. In addition, the new plasma exhibited good tolerance to solvent loading, and was found to be capable of accepting a wide variety of organic solvents directly and salt solutions up to 3% w/w concentration. Combined, the results suggest that the MICAP could be a competitive, simpler alternative to traditional, radiofrequency argon ICP-OES.


international conference on plasma science | 2014

Dielectric resonator antenna for high power RF plasma applications

Jovan Jevtic; Ashok Menon; Velibor Pikelja

Summary form only given. Some of the numerous applications of the inductively coupled plasma, at both atmospheric and low pressure, include plasma manufacturing, optical and mass spectroscopy, gasification and plasma reforming, semiconductor fabrication, in-space propulsion, gas lasers, ion sources, and fusion. A coil of copper or silver-plated tubing is typically used to couple the radio-frequency power into the plasma. Although this technology has been used extensively for many decades, an RF coil suffers from limitations which negatively affect the quality of the generated plasma and increase the complexity of the plasma source. These limitations include high ohmic losses in the antenna conductor which necessitate fluid cooling, high levels of capacitive coupling which necessitate RF shielding, high inter-turn voltage which limits the maximum power due to electric breakdown, external tuning capacitors which add to the size and cost, material properties of copper which demand a vacuum or thermal barrier between the coil and the plasma, etc.We will present a remarkable alternative to an RF coil which addresses all of the limitations mentioned above. It increases the maximum power limit by an order of magnitude while operating at a very high efficiency and producing high quality uniform plasma, without the need for RF shielding, and is fully compatible with high vacuum, high purity, and high temperature environment. This is possible due to the outstanding electrical, thermal, and mechanical properties of the advanced technical ceramics. We have used such ceramic materials to construct ring shaped dielectric resonators whose dielectric polarization currents replace the conduction currents of a copper coil. Polarization currents offer many advantages over conduction currents in plasma applications. One of the most outstanding properties of a dielectric resonator is that it completely eliminates capacitive coupling as the resonator maintains exactly zero RF potential even under full power. We will describe the construction and optical plasma diagnostics of prototype plasma sources for both atmospheric pressure thermal plasma at 2.45GHz in air and Nitrogen1 and low pressure cold plasma at 430MHz in Argon at power levels up to 1kW. In addition, we will show conceptual solutions for the implementation of dielectric resonator antennas in many of the inductively coupled plasma applications.


Archive | 2003

Modular local coil set for magnetic resonance imaging

Ashok Menon; Derek Seeber; Jovan Jevtic


Archive | 2005

Phased array MRI coil with controllable coupled ring resonator

Jovan Jevtic; Velibor Pikelja


Archive | 2002

Floating radio frequency trap for shield currents

Derek Seeber; Ashok Menon; Jovan Jevtic


Archive | 2003

Knee-foot coil with improved homogeneity

Jovan Jevtic; Derek Seeber; Ashok Menon


Archive | 2002

Retracting mri head coil

Jovan Jevtic; Ashok Menon; Derek Seeber; Matthew J. Mercier; Steven M. Zwolinski; Matthias Gyori


Archive | 2014

Plasma generator using dielectric resonator

Jovan Jevtic; Ashok Menon; Velibor Pikelja


Archive | 2003

Loop MRI coil with improved homogeneity

Jovan Jevtic; Derek Seeber; Ashok Menon

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Andrew J. Schwartz

Indiana University Bloomington

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Bharathwaj Muthuswamy

Milwaukee School of Engineering

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Gary M. Hieftje

Indiana University Bloomington

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Leon O. Chua

University of California

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Changju Yang

Chonbuk National University

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Hyongsuk Kim

Chonbuk National University

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