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Introductory nuclear physics new krane (2)

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Introductory nuclear physics new krane (2)

INTRODUCTORY NUCLEAR PHYSICSKenneth s. KraneOregon State UniversityJOHN WILEY & SONSNew York • Chichester • Brisbane • Toronto • SingaporeCopyright ©

Introductory nuclear physics new krane (2) 1988, by John Wiley & Sons. Inc.All rights reserved. Published simultaneously in Canada.Reproduction or translation OÍ any part of this work beyond t

hat permitted by Sections 107 and 108 of the 1976 United States Copyright Act without the permission of the copyright owner is unlawful. Requests for Introductory nuclear physics new krane (2)

permission or further information should he addressed to the Permissions Department. John Wiley & SonsLibrary of Congress Cataloging in Publication Da

Introductory nuclear physics new krane (2)

ta:Kranc. Kenneth s.Introductory nuclear physics.Rev. ed. of Introductory nuclear physics/David Halliday. 2nd. cd. 1955.1. Nuclear physics. I. Hallida

INTRODUCTORY NUCLEAR PHYSICSKenneth s. KraneOregon State UniversityJOHN WILEY & SONSNew York • Chichester • Brisbane • Toronto • SingaporeCopyright ©

Introductory nuclear physics new krane (2) 6 5 4 3 2PREFACEThis work began as a collaborative attempt with David Halliday to revise and update the second edition of his classic text Introducto

ry’ Nuclear Physics (New York: Wiley. 1955). As the project evolved, it became clear that, owing to other commitments. Professor Halliday would be abl Introductory nuclear physics new krane (2)

e to devote only limited time to the project and he therefore volunteered to remove himself from active participation, a proposal to which I reluctant

Introductory nuclear physics new krane (2)

ly and regretfully agreed. He was kind enough to sign over to me the rights to use the material from the previous edition.I first encountered Halliday

INTRODUCTORY NUCLEAR PHYSICSKenneth s. KraneOregon State UniversityJOHN WILEY & SONSNew York • Chichester • Brisbane • Toronto • SingaporeCopyright ©

Introductory nuclear physics new krane (2) nd its readability, and in preparing this new version, 1 have tried to preserve these elements, which are among the strengths of the previous work.Aud

ience This text is written primarily for an undergraduate audience, but could be used in introductory graduate surveys of nuclear physics as well. It Introductory nuclear physics new krane (2)

can be used specifically for physics majors as part of a survey of modern physics, but could (with an appropriate selection of material) serve as an i

Introductory nuclear physics new krane (2)

ntroductory course for other areas of nuclear science and technology, including nuclear chemistry, nuclear engineering, radiation biology, and nuclear

INTRODUCTORY NUCLEAR PHYSICSKenneth s. KraneOregon State UniversityJOHN WILEY & SONSNew York • Chichester • Brisbane • Toronto • SingaporeCopyright ©

Introductory nuclear physics new krane (2) s text Modern Physics (New York: Wiley, 1983)] or at a more advanced, but still undergraduate level. (A brief summary of the needed quantum background

is given in Chapter 2.) The text is therefore designed in a “two-track” mode, so that the material that requires the advanced work in quantum mechani Introductory nuclear physics new krane (2)

cs, for instance, transition probabilities or matrix elements, can be separated from the rest of the text by skipping those sections that require such

Introductory nuclear physics new krane (2)

a background. This can be done without interrupting the logical flow' of the discussion.Mathematical background at the level of differential equation

INTRODUCTORY NUCLEAR PHYSICSKenneth s. KraneOregon State UniversityJOHN WILEY & SONSNew York • Chichester • Brisbane • Toronto • SingaporeCopyright ©

Introductory nuclear physics new krane (2) The presentation of a broad selection of material permits the instructor to tailor a curriculum to meet the needs of any particularVvlPREFACEStudent a

udience. The complete text is somewhat short for a full-year course, but too long for a course of quarter or semester length. The instructor is theref Introductory nuclear physics new krane (2)

ore able to select material that will provide students with the broadest possible introduction to the field of nuclear physics, consistent with the ti

Introductory nuclear physics new krane (2)

me available for the course.The second feature is the unabashedly experimental and phenomenological emphasis and orientation of the presentation. The

INTRODUCTORY NUCLEAR PHYSICSKenneth s. KraneOregon State UniversityJOHN WILEY & SONSNew York • Chichester • Brisbane • Toronto • SingaporeCopyright ©

Introductory nuclear physics new krane (2) lly selected following searches for papers that present data in the clearest possible manner and that relate most directly to the matter under discuss

ion. These original experiments are discussed, often with accompanying diagrams of apparatus, and results with uncertainties are given, all in the att Introductory nuclear physics new krane (2)

empt to convince students that progress in nuclear physics sprang not exclusively from the forehead of Fermi, but instead has been painstakingly won i

Introductory nuclear physics new krane (2)

n the laboratory. At the same time, the rationale and motivation for the experiments arc discussed, and their contributions to the theory are emphasiz

INTRODUCTORY NUCLEAR PHYSICSKenneth s. KraneOregon State UniversityJOHN WILEY & SONSNew York • Chichester • Brisbane • Toronto • SingaporeCopyright ©

Introductory nuclear physics new krane (2) pplications. The first unit presents background material on nuclear sizes and shapes, discusses the two-nucleon problem, and presents an introduction

to nuclear models. These latter two topics can be skipped without loss of continuity in an abbreviated course. The second unit on decay and radioactiv Introductory nuclear physics new krane (2)

ity presents the traditional topics, with new material included to bring nuclear decay nearly into the current era (the recently discovered “heavy” de

Introductory nuclear physics new krane (2)

cay modes, such as 14c, double decay, jB-dclayed nucleon emission, Mdssbaucr elTecl, and so on). The third unit surveys nuclear reactions, including f

INTRODUCTORY NUCLEAR PHYSICSKenneth s. KraneOregon State UniversityJOHN WILEY & SONSNew York • Chichester • Brisbane • Toronto • SingaporeCopyright ©

Introductory nuclear physics new krane (2) hyperfine interactions, particle physics, nuclear astrophysics, and general applications including nuclear medicine. The emphasis here is on the overl

ap with other physics and nonphysics specialties, including atomic physics, high-energy physics, cosmology, chemistry, and medicine. Much of this mate Introductory nuclear physics new krane (2)

rial, particularly in Chapters 18 and 19, represents accomplishments of the last couple of years and therefore, as in all such volatile areas, may be

Introductory nuclear physics new krane (2)

outdated before the book is published. Even if this should occur, however, the instructor is presented with a golden opportunity to make important poi

INTRODUCTORY NUCLEAR PHYSICSKenneth s. KraneOregon State UniversityJOHN WILEY & SONSNew York • Chichester • Brisbane • Toronto • SingaporeCopyright ©

Introductory nuclear physics new krane (2) unit builds to a considerable degree on the previous material; it would be very unwise, for example, to attempt the material on meson physics or parti

cle physics without a firm grounding in nuclear reactions.Sequence Chapters or sections that can be omitted without loss of continuity in an abbreviat Introductory nuclear physics new krane (2)

ed reading are indicated with asterisks (*) in the table of contents. An introductory short course in nuclear physics could be based on Chapters 1, 2,

Introductory nuclear physics new krane (2)

3, 6, 8, 9, 10, and 11, which cover the fundamental aspects of nuclear decay and reactions, but little of nuclear structure. Fission and fusion can b

INTRODUCTORY NUCLEAR PHYSICSKenneth s. KraneOregon State UniversityJOHN WILEY & SONSNew York • Chichester • Brisbane • Toronto • SingaporeCopyright ©

Introductory nuclear physics new krane (2) ters 16 to 20) deals with applications and does not necessarily follow Chapter 15 in sequence. In fact, most of this material could be incorporated at

any time after Chapter 11 (Nuclear Reactions). Chapter 16, covering spins and moments, could even be moved into the first unit after Chapter 3. Chapt Introductory nuclear physics new krane (2)

er 19 (Nuclear Astrophysics) requires background material on fission and fusion from Chapters 13 and 14.

INTRODUCTORY NUCLEAR PHYSICSKenneth s. KraneOregon State UniversityJOHN WILEY & SONSNew York • Chichester • Brisbane • Toronto • SingaporeCopyright ©

INTRODUCTORY NUCLEAR PHYSICSKenneth s. KraneOregon State UniversityJOHN WILEY & SONSNew York • Chichester • Brisbane • Toronto • SingaporeCopyright ©

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