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Advances in Chemical Physics: Molecular Beams, Volume 10 PDF

418 Pages·1966·15.317 MB·English
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Preview Advances in Chemical Physics: Molecular Beams, Volume 10

MOLECULAR BEAMS ADVANCES IN CHEMICAL PHYSICS VOLUME X ADVANCES IN CHEMICAL PHYSICS EDITOR: I. Prigogine Facultk des Sciences, Universitk Libre de Bruxelles, Brussels, Belgium EDITORIAL BOARD THORA . BAK,U niversitetets Fysik Kemiske Institut, Copenhagen, Denmark J. DUCHESNUEni,v ersity of Lihge, Li&ge, Belgium H. C. LONGUEIT-HIGGINTSh,e University Chemical Laboratory, Cambridge, England M. MANDELU, niversity of Leiden, Leiden, Holland V. MATHOTU, niversite Libre de Bruxelles, Brussels, Belgium P. MAZURI, nstitut Lorentz, Leiden, Holland A. MONSTERL, aboratoire de Chimie Physique, Universite de Paris, Paris, France S. ONO,I nstitute of Physics, College of General Education, Tokyo, Japan B. PULLMANL,a boratoire de Chimie Theorique, Universitk de Paris, Paris, France S. RICE,I nstitute for the Study of Metals, University of Chicago, Chicago, Illinois J. W. STOUTI,n stitute for the Study of Metals, University of Chicago, Chicago, Illinois G. SZASZG, eneral Electric Company, Zurich, Switzerland M. VOLKENSTEIINn,s titute of Macromolecular Chemistry, Leningrad, V. U.S.S.R. B. H. ZIMMS, chool of Science and Engineering, University of California at San Diego, La Jolla, California MOLECULAR BEAMS Edited by JOHN ROSS Brown University, Providence, lulode Island INTERSCIENCE PUBLISHERS a division of John Wiley & Sons, New York - London - Sydney COPYRIGH0T 1966 JOHN WILEY& SONS, INC. BY ALL RIGHTS RESERVED LIBRARY CONGRESS CATALOCGA RDN UMBE58R-9 935 OF PRINTED IN THE UNITED STATES OF AMERICA AUTHORS I. AMDURD,e partment of Chemistry, Massachusetts Institute of Technology, Cambridge, Massachusetts JAMES B. ANDERSONM,e chanical Engineering Department, Princeton Univer- sity, Princeton, New Jersey RONALDP. ANDRESM, echanical Engineering Department, Princeton Univer- sity, Princeton, New Jersey BENJAMIBNE DERSONPh, ysics Department, New York University, New York, New York RICHARD B. BERNSTEINT, heoretical Chemistry Institute and Chemistry Department, University of Wisconsin, Madison, Wisconsin JOHNB . FENNM, echanical Engineering Department, Princeton University, Princeton, New Jersey CLAYTONG ~ESED,e partment of Physics, The University of Chicago, Chicago, Illinois E. F. GREENEM, etcalf Chemical Laboratories, Brown University, Providence, Rhode Island DUDLEYH ERSCHBACHD,e partment of Chemistry, University of California, Berkeley, California J. E. JORDADNe,p artment of Chemistry, Massachusetts Institute of Technol- ogy, Cambridge, Massachusetts A. L. MOURSUNDM, etcalf Chemical Laboratories, Brown University, Providence, Rhode Island E. E. MUSCHLITZJ,r ., Department of Chemistry, University of Florida, Gainesville, Florida EDWARDJ. ROBINSONPh, ysics Department, New York University, New York, New York JOHNR oss, Department of Chemistry, Brown University, Providence, Rhode Island R. F. STEBBINGSG, eneral Atomic Division of General Dynamics Corpora- tion, San Diego, California PREFACE Studies of molecules in nearly collision-free and unidirectional motion, that is, in molecular beams, have been made for over fifty years. The technique has long been recognized as particularly suitable for the determination of the interaction of a single molecule with another molecule, with a photon, with external fields, or with surfaces. (See the Appendix for some general references.) In principle. at least, molecular beam experiments provide the means for direct measure- ments of molecular properties. Of course, the properties of macroscopic systems are related to those of their molecular constituents by the theories of statistical mechanics. These relations are always some statistical average of molecular properties, an average which obscures the dependence of the macroscopic measurement on the molecular properties. In practice the removal of all statistical averages even in molecular beam experiments presents extreme problems. The articles in this volume are reviews of some of the current molecu- lar beam research in the general area of chemical physics. Interest in such experiments has increased sharply in the last ten years, especially among chemical kineticists. The predominant, common theme through- out the volume is molecular interactions. Elastic scattering is discussed in two articles, one reviewing high- energy scattering and repulsive forces, the other low-energy scattering and a number of quantum-mechanical effects for which both attractive and repulsive forms are of importance. Reactive scattering is the topic of four articles, two on neutral reactions and two on ionic reactions. Information on chemical reactions may be obtained by molecular beam measurements on the scattered chemical product or from the study of elastic scattering in reactive systems. Both methods are reviewed. Ion-molecule and charge-transfer reactions are also discussed in sep- arate articles. The remaining sections of the volume are devoted to inelastic scattering of metastable atoms, the determination of atomic polarizabilities, and the technique of hypersonic beams. The articles are representative of current molecular beam research in chemical physics, but the selection is by no means complete. For vii viii PREFACE instance, reviews on nonreactive inelastic scattering, on the use of beams as a technique for molecular resonance spectroscopy, and on the inter- actions of molecules with surfaces are among the omissions. I wish to thank my colleague Professor F. Greene for much help E. and advice in editing this volume and Dr. G. P. Flynn for compiling the subject index. JOHN Ross CONTENTS 1. Beam Measurements of Atomic Polarizabilities . By Benjamin Bederson and Edward J. Robinson 1 2. Elastic Scattering of High-Energy Beams: Repulsive Forces . By I. Amdur and J. E. Jordan 29 3. Quantum Effects in Elastic Molecular Scattering By Richard B. Bernstein . . 75 4. Elastic Scattering in Chemically Reactive Systems . By E. F. Greene, A. L. Moursund, and J. Ross 135 5. Collisions of Electronically Excited Atoms and Molecules By E. E. Muschlitz, Jr. . . 171 6. Charge Transfer By R. F. Stebbings . . 195 7. Ion-Neutral Reactions By C. F. Giese . . 247 8. Supersonic Nozzle Beams . . . By J. B. Anderson, R. P. Andres, and J. B. Fenn 275 9. Reactive Scattering in Molecular Beams . By D. R. Herschbach . 319 . . Appendix. Selected References on Molecular Beam Research 395 . . Author Index 397 Subject Index . . 411 Advance in Chemical Physics, VolunzeX Edited by John Ross Copyright © 1966 by John Wiley & Sons. Inc. 1. BEAM MEASUREMENTS OF ATOMIC POLARIZABILITIES" BENJAMIN BEDERSON and EDWARD J. ROBINSON Physics Department, New York University, New York CONTENTS I. Introduction .................................. ................. 1 11. Theory ....................................... ................. 2 111. Methods of Calculating Polarizabilities ............ ................ 6 IV. Atomic Beam Experiments ..................... ................. 9 A. Alkali Measurements ....................... ................. 9 B. Measurements of Metastable 3 PA~r gon ....... ................ 20 V. Conclusion ................................... .................. 25 References ......................................... ................. 26 I. INTRODUCTION Polarizability is a seemingly ubiquitous atomic property which appears as a parameter in the description of many important atomic processes. The calculation of the van der Waals interaction, the des- cription of charge transfer and other ion-atom and electron-atom collision processes, of optical lifetimes, and of optical dispersion all directly involve or are related to the static polarizabilities of ground and excited states of neutral atoms and molecules. In a general sense one can expect that the atomic polarizability will be a useful para- meter when dealing with any atomic process in which the outer part of the electronic wave function plays an important role. Direct experi- mental determinations of atomic polarizabilities provide a very sensitive check on the accuracy of electronic wave functions, where these are * Some of the work described in this article was supported by the Advanced Research Projects Agency, through the Office of Naval Research, Washington, D.C., under Contract No. NONR-285(60), and by the Defense Atonlic Support Agency, through the Army Research Office, Durham, N.C., under Contract No. DA-ARO-D-3 1-12 4G530. 1 2 BENJAMIN BEDERSON AND EDWARD J. ROBINSON available. In addition, since the approximation methods used in calculating quadrupole shielding factors can also be used to calculate polarizabilities,’ comparison of such calculations with experiment provides an independent check on these methods, and is therefore helpful in providing more reliable values of nuclear quadrupole moments. Atomic beam methods would appear to be eminently suited to measuring polarizabilities, because of the absence of particleparticle interactions. Yet, there have been only a few such experiments in recent years, notably the deflection experiments of Chamberlain and Zorn’ at Yale, and the balance experiment^^-^ by the N.Y.U. group. (The earlier work of Scheffers and Stark5 is primarily of historic interest.) Our purpose in this article is to discuss these experiments in some detail, and also to briefly describe some of the principal methods by which atomic polarizabilities have been calculated in recent years. THEORY II. The energy of an atom in an external field is readily calculable from perturbation theory, provided one has means of estimating the relevant matrix elements. Let an unperturbed atom have a Hamiltonian Ho with energy go. In the presence of an electric field E, the Hamiltonian + becomes So 2’T.h e perturbation 2’= -p;E, where the electric dipole operator pe= - C eri i with ri the position vector of the ith electron. The first-order pertur- bation energy is B1 = (Ol&”lO) = (0Jp;EJO) (1) where 10) is the unperturbed state vector. Since 2’is an operator of odd parity, the matrix element in Eq. (1) will vanish if (0) has a definite parity. That is, states of definite parity have zero permanent dipole moments. The second-order perturbation energy g2 is given by a summation containing matrix elements of p, between 10) and other states Ik) of the form c,=- c <Ol Pe’El k)< k Ipe*ElO) (2) - k#O da, 80

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