magnetic anisotropies in nanostructured matter, 2009, p.303

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magnetic anisotropies in nanostructured matter, 2009, p.303

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[...]... in two dimension tiously in parentheses since although such clusters appear as distinct features in Scanning Tunnelling Microscopy (STM) pictures, see Fig 1.5, in the case of magnetic atoms forming these clusters they are connected to each other, e.g., by long range magnetic interactions It was already said that a classication of nanosystems can be made only in a kind of semi-qualitative manner using... Preliminary considerations In preliminary considerations basic denitions concerning frequently used colloquial terminologies are introduced In particular the "geometrical" origin of terms like parallel and antiparallel or collinear and non-collinear and the dierence between "spin" viewed as a classical vector or as a spinor are emphasized Also introduced is an explicit formulation for the spin orbit interaction... written without indoctrinations by others Denitely Simon Altmann (Oxford) and Walter Kohn (S Barbara) did (and still do) have a substantial share in this kind of intellectual "pushing" xiii â 2009 by Taylor & Francis Group, LLC 1 Introduction In here the key words in the title of the book, namely nanostructured matter and magnetic anisotropies, are critically examined and dened Nanosystems and nanostructured. .. [1] In Eq (2.12) Rij = Ri Rj , and J, and refer in turn to the exchange interaction parameter, the magnetic dipoledipole parameter and the spin-orbit interaction parameter Quite clearly by the terms "collinear" or "non-collinear spins" transformation properties of classical vectors are implied, however, in a very particular manner Consider an arbitrary pair of spins, si and sj In principle, since... the direction cosines of this axis, and is the rotation angle in a right-hand screw sense about n, 0 , then U (R) is given [1] by U (R) = U (n, ) , C in3 S (n2 + in1 )S U (n, ) = (n2 in1 )S C + in3 S S = sin(/2) , (3.27) , C = cos(/2) (3.28) (3.29) U (R) is a transformation in spin space only, i.e., U (R) SU 2 Returning now to (3.24) and using the invariance condition in (3.19), á à 0 ả... beginning of a book dealing with nanostructured matter: nanosystems are not interesting per se, but only because of their exceptional physical properties, some of which will be discussed in here The other key words in the title of the book, namely magnetic anisotropies, also need clarication Per denition anisotropic physical properties are direction dependent quantities, i.e., are coupled to an intrinsic... Eq (3.20) applies Quaternions are not really avoided here, since (n, ) is a quaternion, namely an object containing a vector n and a scalar [2] â 2009 by Taylor & Francis Group, LLC 22 3.4.2 Magnetic Anisotropies in Nanostructured Matter Local spin density functional approaches It was already mentioned in Sect 2.3.2 that in using a local spin density functional (LS-DFT) approach the exchange eld is... LLC 2 Magnetic Anisotropies in Nanostructured Matter order to dene nanosystems somehow satisfactorily the concept of functional units or functional parts of a solid system has to be introduced Functional in this context means that particular physical properties of the total system are mostly determined by such a unit or part In principle two kinds of nanosystems can be dened, namely solid systems in which... consider the magnetic moments in bulk Fe and for Fe(100) In the bulk case (innite system) in each unit cell the same magnetic moment pertains, while in the semi-innite system Fe(100) the moment in surface near layers is dierent from the one deep inside the â 2009 by Taylor & Francis Group, LLC 12 Magnetic Anisotropies in Nanostructured Matter system As is well known, sizeable oscillations of the moment with... scales in one or two dimensions There are of course cases in which the usual scales seemingly dont apply Quantum corrals for example, see Fig 1.5, can have diameters exceeding the usual connement length of 2d-nanosystems Another, very prominent case is that of magnetic domain walls, which usually in bulk systems have a thickness of several hundred nanometers However, since in nanowires domain walls . Data Weinberger, P. (Peter) Magnetic anisotropies in nanostructured matter / Peter Weinberger. p. cm. (Series in condensed matter physics ; 2) Includes bibliographical references and index. ISBN. hereafter invented, including photocopying, microfilming, and recording, or in any information storage or retrieval system, without written permission from the publishers. For permission to photocopy. & Francis Group, an informa business Boca Raton London New York Magnetic Anisotropies in Nanostructured Matter © 2009 by Taylor & Francis Group, LLC Chapman & Hall/CRC Taylor &

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Mục lục

  • Cover Page

  • Title Page

    • Magnetic Anisotropies in Nanostructured Matter

      • Contents

      • Biography

      • Acknowledgments

      • Afterword

      • Introduction

        • Table of Contents

        • Chapter 1: Introduction

        • Afterword

        • Preliminary considerations

          • Table of Contents

          • Chapter 2: Preliminary considerations

            • 2.1 Parallel, antiparallel, collinear & non-collinear

            • 2.2 Characteristic volumina

            • 2.3 "Classical" spin vectors and spinors

              • 2.3.1 "Classical vectors" and Heisenberg models

              • 2.3.2 Spinors and Kohn-Sham Hamiltonians

              • 2.4 The famous spin-orbit interaction

                • 2.4.1 The central field formulation

                • Afterword

                • Symmetry considerations

                  • Table of Contents

                  • Chapter 3: Symmetry considerations

                    • 3.1 Translational invariance

                    • 3.2 Rotational invariance

                    • 3.3 Colloquial or parent lattices

                    • 3.4 Tensorial products of spin and configuration

                      • 3.4.1 Rotational properties

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