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THE EFFECTS OF RELATIVITY IN ATOMS, MOLECULES, AND THE SOLID STATE THE EFFECTS OF RELATIVITY IN ATOMS, MOLECULES, AND THE SOLID STATE Edited by S. Wilson Rutherford Appleton Laboratory Oxfordshire, United Kingdum 1. P. Grant Uniuersity of Oxford Oxford, Uniled Kingdom aud B. L. Gyorffy Universily of Brislol Brislo/, United Kingdom SPRINGER SCIENCE+BUSINESS MEDIA, llC Llbrarv of Congress Catalog lng-ln-Publ leat Ion Data The Effects of relatlvity 1n atoms, oolecules, and the solid state I edlted by S. WIIson, I.P. Grant, and B.L. Gyorffy. p. c •. "Proceedlngs of a .eetlng on the effects of relatlvity In atoms, molecules, and the solid state, held March 30-Aprll 1, 1990, In Ab lngdon, Oxfordsh 1r e, Un I ted K 1n gdom "--T. p. verso. Inc I udes b I b li ograph 1cal references and Index. ISBN 978-1-4613-6646-1 ISBN 978-1-4615-3702-1 (eBook) DOI 10.1007/978-1-4615-3702-1 1. Atomic structure--Congresses, 2. Molecular structure -Congresses. 3. Solid state physlcs--Congresses. 4. Solid state chemlstry--Congresses. 5. Reiativity (PhYSics)--Congresses. 1. WIIson, S, (Stephen), 1950- II. Grant, 1. P. III. GyiirffY, B. L. QC172.E34 1991 539'.1--dc20 91-11449 CIP Proceedings of a meeting on the Effects of Relativity in Atoms, Molecules, and the Solid State, held March 30-ApriI 1, 1990, in Abingdon, Oxfordshire, United Kingdom ISBN 978-1-4613-6646-1 © 1991 Springer Science+Business Media New York Originally published by Plenum Press, New York in 1991 Softcover reprint of the hardcover 1st edition 1991 AII 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, mechanical, photocopying, microfilming, recording, or otherwise, without written permission from the Publisher Preface Recent years have seen a growing interest in the effects of relativity in atoms, molecules and solids. On the one hand, this can be seen as result of the growing awareness of the importance of relativity in describing the properties of heavy atoms and systems containing them. This has been fueled by the inadequacy of physical models which either neglect relativity or which treat it as a small perturbation. On the other hand, it is dependent upon the technological developments which have resulted in computers powerful enough to make calculations on heavy atoms and on systems containing heavy atoms meaningful. Vector processing and, more recently, parallel processing techniques are playing an increasingly vital role in rendering the algorithms which arise in relativistic studies tractable. This has been exemplified in atomic structure theory, where the dominant role of the central nuclear charge simplifies the problem enough to permit some prediction to be made with high precision, especially for the highly ionized atoms of importance in plasma physics and in laser confinement studies. Today's sophisticated physical models of the atom derived from quantum electrodynamics would be intractable without recourse to modern computational machinery. Relativistic atomic structure calculations have a history dating from the early attempts of Swirles in the mid 1930's but continue to provide one of the primary test beds of modern theoretical physics. In. non-relativistic molecular structure calculations the use of basis set expansion techniques is almost mandatory. Although it has been known since the work of Kim in the late 1960's that there are problems associated with the use of basis set expansion techniques in relativistic electronic structure calculations, these difficulties have only recently been resolved. By affording a firm foundation for the ab initio treatment of molecules containing heavy atoms and the interactions between them these developments open up new horizons for modern theoretical chemistry. Relativistic quantum chemistry has a vast range of potential applications in both the academic and the commercial sectors in fields as diverse as catalysis and pharmacology, molecular electronics and molecular biology. However, relativistic electronic structure calculations for molecules will remain demanding for some time to come both in the requirement for more efficient and reliable numerical methods and algorithms, and for the computer resources which these methods require. Relativistic solid-state calculations will be just as demanding. In. solid-state theory the emphasis has until now been more on deriving physically intuitive approximation schemes which seem tractable. The consensus which has enabled atomic and molecular physicists and theoretical chemists to build general purpose models has, so far, not existed amongst solid-state theorists. This volume records the proceedings of a meeting on "The Effects of Relativity in Atoms, Molecules and the Solid State" held under the auspices of three of the Science and Engineering Research Council's Collaborative Computational Projects : Project 1 - v Electron correlation in molecules, Project 2 -Continuum states of atoms and molecules, and Project 9 -The electronic structure of solids. The meeting was held at The Coseners House, Abingdon, Oxfordshire, over the weekend 30th March - 1st April, 1990. s. July 1990 Wilson I.P. Grant B.L. Gyorffy vi Contents Relativistic Effects on Periodic Trends P.Pyykko ATOMS Relativistic Atomic Structure and Electron-Atom Collisions 17 I.P. Grant On the Accuracy of Oscillator Strengths 45 B.c. Fawcett Atomic Structure Calculations in Breit-Pauli Approximation 55 W. Eissner Relativistic Calculations of Parity Non-Conserving Effects in Atoms 67 A.c. Hartley and P.G.H. Sandars High Precision Relativistic Atomic Structure Calculations Using the Finite Basis Set Approximation 83 H.M. Quiney Relativistic Calculations of Electron Impact Ionisation Cross-Sections of Highly Charged Ions 125 D.L. Moores MOLECULES Nonsingular Relativistic Perturbation Theory and Relativistic Changes of Molecular Structure 135 W.H.E. Schwarz, A. Rutkowski and G. Collignon Basis Set Expansion Dirac-Fock SCF Calculations and MBPT Refinement 149 Y. Ishikawa Comments 163 Polyatomic Molecular Dirac-Hartree-Fock Calculations with Gaussian Basis Sets 167 K.G. Dyall, K. Fregri, Jr. and P.R. Taylor vii Open Shell Relativistic Molecular Dirac-Hartree-Fock SCF-Program 185 O. Visser, PJ.c. Aerts and L. Visscher General Contraction in Four-Component Relativistic Hartree-Fock Calculations 197 L. Visscher, P.J.c. Aerts and O. Visser Accurate Relativistic Dirac-Fock and MBPT Calculations on Argon with Basis Sets of Contracted Gaussian Functions 207 Y. Ishikawa and R.C. Binning, Jr. Comments 215 Relativistic Many-Body Perturbation Theory of Atomic and Molecular Electronic Structure 217 S. Wilson SOLID STATE Relativistic Density-Functional Theory for Electrons in Solids 255 B.L. Gyorffy, J.B. Staunton, H. Ebert, P. Strange and B. Ginatempo Influence of Relativistic Effects on the Magnetic Moments and Hyperfine Fields of 5d-Impurity Atoms Dissolved in Ferromagnetic Fe 275 H. Ebert, B. Drittler, R. Zeller and P.H. Dederichs Relativistic Spin-Polarized Density-Functional Theory: Simplified Method for Fully Relativistic Calculations 285 P. Cortona Theory of Magnetocrystalline Anisotropy 295 J. Staunton, P. Strange, B.L. Gyorffy, M. Matsumoto, J. Poulter, H. Ebert and N.P. Archibald The Spin Polarized Photoemission from Non-Magnetic Metals 319 B. Ginatempo and B.L. Gyorffy Theory of Magnetic X-Ray Dichroism 333 H. Ebert, B. Drittler, P. Strange, R. Zeller and B.L. GyorffY Participants 349 Index 351 viii RELATIVISTIC EFFECTS ON PERIODIC TRENDS Pekka Pyykko Department of Chemistry, University of Helsinki Et. Hesperiankatu 4, 00100 Helsinki, Finland 1. INTRODUCTION Whether we work on atoms, molecules or solids, we have in common the Periodic System. At least seven different trends can be found in it, see Figure 1. The last three of them are of relativistic origin. Some of their particular consequences on chemical and physical properties of elements are shown in Figure 2. A few recent examples are quoted below. 2. A REVIEW OF REVIEWS Grant (1970) reviewed the relativistic calculations on atoms and Pyykko (1978) the ones on molecules, including a chapter on "Relativity and the Periodic Table". These effects were brought to the attention of many chemists by Pitzer (1979) or Pyykko and Desclaux (1979), and have now entered the inorganic chemistry textbooks by Cotton and Wilkinson (1988) or Mackay and Mackay (1989). The book by Pyykko (1986) includes 3119 references (and seems to miss about 1% of the relevant material). Some later reviews are mentioned in Table 1. 3. SOME RECENT RESULTS IN CHEMISTRY The valencies of gold. It was suggested already by Pyykko (1978) that the relativistic destabilization of the 5d shell would explain the well-known valency increase from Ag(I) to Au(III). Schwerdtfeger (1989) has now compared the calculated stabilities of the (free) halides AUX2- and AUX4-, and expli citly demonstrated that the preference for the higher oxida tion state, III instead of I, indeed is of relativistic ori gin. The "gold maximum". The relativistic contraction and stabili zation of the ns valence shell (n = 4 to 6) suffers a local maximum at the coinage metals, group 11. Schwarz et al. (1989) analysed the origins of this trend. The Effects of Relativity on Atoms, Molecules, and the Solid State Edited by S. Wilson et al., Plenum Press, New York, 1991 "Relativistic compounds". A number of novel organometallic compounds have recently been synthesized and characterized, in which a weak attraction, roughly of 10 kcal/mole or half of an 00 eV, much like in a good hydrogen bond, seems exist between formally closed-shell Au{I) atoms saving a 5d1 configuration. MoSe generally, bonds between 5d1 , 6s2 or the configuration 5d are found. without explicit proof, these bonds are pre sumed to have strong relativistic contributions. In any case, this "relativistic encouragement" has been a source of inspi ration for the syntheticians, as evidenced by some of the titles of Balch et ale (1987), Nagle et ale (1988), Raptis et ale (1989), Scherbaum et ale (1988), and Wang et ale (1988). A particularly striking example is the octahedral, six coordinate carbon complex ({Ph3PAU)6C}2+ of Scherbaum et ale (1988). The carb~n elgctron octet could then form, in 0h symmetry, an (a1) (t1u) "8-electron-7-centre bond". In addi tion, the Au-Au attractions would help. The only available calculation on it is that by Rosch et ale (1989). Both the Au Au and the C-Au interactions are found to contribute to the bonding. pert~rba~ive Hartree-Fock-Slater studies on the bonding in the 5d -6s molecule TI Pt(CN) by Ziegler et ale (1989a) suggest that the interaction between thallium and the tetra cyanoplatinate has both strong ionic and covalent components. AU~+. A clean example on the 5d10_5d10 attraction would be the gas-phase Au22+, claimed by Saunders (1989). The theoretical situation is summarized in Table 2. The pseudopotential HF or CI calculations and the semiempirical tight-binding calcula tions give a repulsive ground state. The non-relativistic DVM calculations by Li et ale (1990) are seen to considerably overbind for AU2+ and thus lack credibility. Therefore the observation, if true, must come from an excited electronic state (Mukherjee et ale 1990). Both their TB calculations and the present PP-HF ones indeed find such a m~n~mum in the states promoting one 5da antibonding electron to the 6sa bonding MO. The ground-state PP-CI curve of Ermler (private communica tion) can be divided to three domains: a) R > 6 a.u : A large-R domain with superposed +l/R repUlsion and an _~/R4 charge-po1arisabi1ity-type attraction. The coef ficient of the latter gives an Au+ polarisability,~, of about 14.2 a.u. b) About 5 < R < 6: Some extra bonding (about 0.065 eV) but no minimum. c) R < 5: Extra, Pauli repulsion. Trends along triads. The bond strength trend CU > Ag < Au was explained quite early as a relativistic effect (see Ziegler et ale (1989b) and, for later literature, Balasubramanian (1989a).) A similar trend is seen in various organometallic compounds of groups 6 (Cr > Mo < W), 8 (Fe> Ru < Os), 9 (Co> Rh < Ir), 10 (Ni > Pd < Pt), and the strengthening has also been shown to be a relativistic effect (Ziegler et ale 1989b). For the same trend among the group 6 dimers, see Ziegler (1987). A recent experimental example on this D trend are the diatomic molecules CuIn > AgIn < AuIn (Balduccieet ale 1989). 2 Trends in Periodic System(s) l.Main vertical trend: First shell of each I ano malously small (1s, 2p, 3d, 4f). Due to 'primo genic repulsion', larger <r> for larger n. 2.Main horizontal trend: Smaller <r> for larger Z. 3.Main periodicity: Filled shells particularly stable. Half-filled non-relativistic shells also. 4.Partial screening effects: d-shell contraction, lanthanold contraction. 5.Relativistic contraction and stabilization (s, p). 6.Relativlstic expansion and destabilization (d, f) 7.Spin-orbit splitting. No deep group-theoretical principle. Ie) Pekka Pyykko. March 21, 1990. Fig. 1. 3

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