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Oxide Electronics and Functional Properties of Transition Metal Oxides PDF

258 Pages·2014·8.835 MB·English
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CHEMISTRY RESEARCH AND APPLICATIONS O E F XIDE LECTRONICS AND UNCTIONAL P T ROPERTIES OF RANSITION METAL OXIDES No part of this digital document may be reproduced, stored in a retrieval system or transmitted in any form or by any means. The publisher has taken reasonable care in the preparation of this digital document, but makes no expressed or implied warranty of any kind and assumes no responsibility for any errors or omissions. No liability is assumed for incidental or consequential damages in connection with or arising out of information contained herein. This digital document is sold with the clear understanding that the publisher is not engaged in rendering legal, medical or any other professional services. C R A HEMISTRY ESEARCH AND PPLICATIONS Additional books in this series can be found on Nova‘s website under the Series tab. Additional e-books in this series can be found on Nova‘s website under the e-book tab. CHEMISTRY RESEARCH AND APPLICATIONS O E F XIDE LECTRONICS AND UNCTIONAL P T ROPERTIES OF RANSITION METAL OXIDES ALEXANDER PERGAMENT EDITOR New York Copyright © 2014 by Nova Science Publishers, Inc. All rights reserved. No part of this book may be reproduced, stored in a retrieval system or transmitted in any form or by any means: electronic, electrostatic, magnetic, tape, mechanical photocopying, recording or otherwise without the written permission of the Publisher. For permission to use material from this book please contact us: Telephone 631-231-7269; Fax 631-231-8175 Web Site: http://www.novapublishers.com NOTICE TO THE READER The Publisher has taken reasonable care in the preparation of this book, but makes no expressed or implied warranty of any kind and assumes no responsibility for any errors or omissions. No liability is assumed for incidental or consequential damages in connection with or arising out of information contained in this book. The Publisher shall not be liable for any special, consequential, or exemplary damages resulting, in whole or in part, from the readers‘ use of, or reliance upon, this material. Any parts of this book based on government reports are so indicated and copyright is claimed for those parts to the extent applicable to compilations of such works. Independent verification should be sought for any data, advice or recommendations contained in this book. In addition, no responsibility is assumed by the publisher for any injury and/or damage to persons or property arising from any methods, products, instructions, ideas or otherwise contained in this publication. This publication is designed to provide accurate and authoritative information with regard to the subject matter covered herein. It is sold with the clear understanding that the Publisher is not engaged in rendering legal or any other professional services. If legal or any other expert assistance is required, the services of a competent person should be sought. FROM A DECLARATION OF PARTICIPANTS JOINTLY ADOPTED BY A COMMITTEE OF THE AMERICAN BAR ASSOCIATION AND A COMMITTEE OF PUBLISHERS. Additional color graphics may be available in the e-book version of this book. Library of Congress Cataloging-in-Publication Data Oxide electronics and functional properties of transition metal oxides / editor, Alexander Pergament (Petrozavodsk State University, Russia). pages cm. -- (Chemistry research and applications) Includes index. ISBN: (cid:28)(cid:26)(cid:27)(cid:16)(cid:20)(cid:16)(cid:25)(cid:22)(cid:22)(cid:21)(cid:20)(cid:16)(cid:24)(cid:22)(cid:23)(cid:16)(cid:23) (eBook) 1. Transition metal oxides. 2. Oxides--Electric properties. I. Pergament, Alexander, editor. QD172.T6O95 2014 621.381--dc23 2014026239 Published by Nova Science Publishers, Inc. † New York CONTENTS Oxide Electronics: An Introduction vii Alexander Pergament Chapter 1 Unipolar Resistive Switching Effect 1 Tatiana V. Kundozerova and Genrickh B. Stefanovich Chapter 2 Some Fundamental Points of Technology of Lithium Niobate and Lithium Tantalate Single Crystals 31 M. N. Palatnikov and N. V. Sidorov Chapter 3 Sputter Deposited Nanolaminates Containing Group IVB (Ti, Zr, Hf)-Oxides: Phase Structure and Near Band Gap Optical Absorption Behavior 169 Carolyn Rubin Aita Chapter 4 Optical and Electrical Switching of Thermochromic VO Smart Coatings 211 2 Mohammed Soltani Editor Contact Information 231 Index 233 OXIDE ELECTRONICS: AN INTRODUCTION Alexander Pergament1 Petrozavodsk State University, Petrozavodsk, Russia ABSTRACT MOSFETs (Metal-Oxide-Semiconductor Field-Effect Transistors) have for a long time been the workhorse of modern electronics industry. For the purpose of a permanent integration enhancement, the size of a MOSFET has been decreasing exponentially for over decades in compliance with the Moore‘s Law, but nowadays, owing to the intrinsic restrictions, the further scaling of MOSFET devices either encounters fundamental (e.g. quantum-mechanical) limits or demands for more and more sophisticated and expensive engineering solutions. Alternative approaches and device concepts are currently designed both in order to sustain an increase of the integration degree, and to improve the functionality and performance of electronic devices. Oxide electronics is one of such promising approaches which could enable and accelerate the development of information and computing technology. The behavior of d-electrons in transition metal oxides (TMOs) is responsible for the unique properties of these materials, causing strong electron-electron correlations, which play an important role in the mechanism of metal- insulator transition. The Mott transition in vanadium dioxide is specifically the effect that researchers consider as one of the most promising phenomena for oxide electronics, particularly, in its special direction known as a Mott-transition field-effect transistor (MTFET). Therefore, VO -based MTFET is one of the fields of oxide electronics. Also, 2 oxide ReRAM is another rapidly growing field of oxide electronics. Finally, many other functional properties of TMOs, including, for example, optical and electrical switching of thermochromic VO smart coatings, optical properties (especially Raman spectra) of 2 single crystalline lithium niobate and tantalate (LiNbO and LiTaO ), as well as optical 3 3 properties (near band gap optical absorption) of TMO-based nanolaminates, like e.g. ZrO -Al O , HfO -Al O , TiO -Al O , ZrO -TiO , and HfO -TiO , are extremely 2 2 3 2 2 3 2 2 3 2 2 2 2 important to understand and estimate potential ability of different TMOs and TMO-based structures in diverse fields of oxide electronics. Keywords: Oxide electronics, Transition metal oxides, Oxide ReRAM, Lithium Niobate and Tantalate, Vanadium dioxide, Oxide nanolaminates 1 E-mail: [email protected]. viii Alexander Pergament The term ―oxide electronics‖ have emerged not so long ago in the everyday-life of scientific literature, but already firmly taken its place. The point is that the modern IT revolution is based on technological progress which enables an exponentially growing enhancement of the performance of electronic devices. During all the history of the development of electronic components, from a vacuum diode to modern highly integrated ICs with nanometer scale of individual elements, the question of the physical limitations on the further progress in this area arose repeatedly. After the invention of an IC by J. Kilby and R. Noyce in 1958 [1], the number of transistors on a chip roughly doubles every two years, and afterwards the processing speed and storage capacity increase correspondingly (Moore‘s Law). Such a dynamics is typical of all other key parameters of the ICs, the most important of which is a characteristic size of the active region d [2], for example, the FET effective m channel length. In recent years, the issue of constraints for standard Si-based electronics has been widely discussed in the scientific literature, which is primarily associated with the possibility of further scaling toward nano-size. In this regard, in the 2007 edition of The International Technology Roadmap for Semiconductors (ITRS, http://www.itrs.net), a new section has appeared, namely ―Emergent Research Device Materials‖, which indicates the need to develop a new generation of devices based on new physical principles [3]. Dimensional constraints of the conventional CMOS technology will not allow, apparently, overcoming the limit of d far beyond 10 nm, and this can be called as a m ―Moore‘s Law violation‖ [4] (or, so to say, ―More than Moore‖, – the pun which seems to originate from the ITRS authors). Note, however, that the ITRS program still optimistically claims that a theoretical limit of scaling for Si is not seen, and by 2026 it is planned to achieve the level of d = 6 nm (and according to the Intel‘s road map – 10 nm by 2015, the so called m ―P1274 process‖ [5]). Recently, a laboratory prototype of a SOI-based FET with a 3 nm channel length has been reported [6]. Last years, technologies with characteristic topological dimensions of 45, 22 and 10 nm are being actively developed, and the main directions here are as follows: high-k gate dielectrics, multigate structures, the use of such materials as Ge, A3B5 and graphene, Si-Ge alloys in the source and drain regions and strained silicon, and finally, «tri-gate» FET configuration [5] (some of these directions have also been presented in the recent review «Technology Evolution for Silicon Nanoelectronics: Postscaling Technology» [7]). Simultaneously, new technical solutions for architecture optimization (such as, e.g., multi-core processors and the Blue Gene project), system integration and innovative design are developed (see, e.g., a corresponding discussion in the review [4]). Alternative approaches are based on another mechanism (as compared to the field effect in Si CMOS FETs) or even on a drastic change in computational paradigm or architecture (quantum computers, neuroprocessors). Amongst the approaches utilizing new physical mechanisms, one can list, for example, spintronics, superconducting electronics, single- electronics, molecular electronics, as well as one more quite recent direction, so-called ―soletronics‖ (single atom electronics) [8]. One of such novel directions, oxide electronics, is based on the idea of application of unique properties and physical phenomena in strongly correlated transition metal oxides (TMO). Metal-insulator transition (MIT) [9] belongs to the class of the aforementioned phenomena, and many TMOs, e.g. vanadium dioxide, undergo MITs as functions of temperature or electric field [4, 9, 10]. Complex strongly correlated TMOs, such as HTSC cuprates, CMR manganites or some interfaces (such as, for instance, LaAlO /SrTiO ), had first been considered as candidate 3 3 materials for oxide electronics [3], and the list of devices proposed had included, for example,

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