19B3 Nuclear States from Charged Particle Reactions

Landolt-Börnstein Numerical Data and Functional Relationships in Science and Technology New Series / Editor in Chief: W...

Author: Z.N. Soroko | S. Sukhoruchkin

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Landolt-Börnstein Numerical Data and Functional Relationships in Science and Technology New Series / Editor in Chief: W. Martienssen

Group I: Elementary Particles, Nuclei and Atoms Volume 19

Nuclear States from Charged Particle Reactions Subvolume B Tables of Excitations from Reactions with Charged Particles Part 3 Z = 63 - 99 S.I. Sukhoruchkin Z.N. Soroko Edited by H. Schopper

ISSN 1615-1844 (Elementary Particles, Nuclei and Atoms) ISBN 978-3-540-48697-8 Springer Berlin Heidelberg New York Library of Congress Cataloging in Publication Data Zahlenwerte und Funktionen aus Naturwissenschaften und Technik, Neue Serie Editor in Chief: W. Martienssen Vol. I/19B3: Editor: H. Schopper At head of title: Landolt-Börnstein. Added t.p.: Numerical data and functional relationships in science and technology. Tables chiefly in English. Intended to supersede the Physikalisch-chemische Tabellen by H. Landolt and R. Börnstein of which the 6th ed. began publication in 1950 under title: Zahlenwerte und Funktionen aus Physik, Chemie, Astronomie, Geophysik und Technik. Vols. published after v. 1 of group I have imprint: Berlin, New York, Springer-Verlag Includes bibliographies. 1. Physics--Tables. 2. Chemistry--Tables. 3. Engineering--Tables. I. Börnstein, R. (Richard), 1852-1913. II. Landolt, H. (Hans), 1831-1910. III. Physikalisch-chemische Tabellen. IV. Title: Numerical data and functional relationships in science and technology. QC61.23 502'.12 62-53136 This work is subject to copyright. All rights are reserved, whether the whole or part of the material is concerned, specifically the rights of translation, reprinting, reuse of illustrations, recitation, broadcasting, reproduction on microfilm or in other ways, and storage in data banks. Duplication of this publication or parts thereof is permitted only under the provisions of the German Copyright Law of September 9, 1965, in its current version, and permission for use must always be obtained from Springer-Verlag. Violations are liable for prosecution act under German Copyright Law. Springer is a part of Springer Science+Business Media springeronline.com © Springer-Verlag Berlin Heidelberg 2007 Printed in Germany The use of general descriptive names, registered names, trademarks, etc. in this publication does not imply, even in the absence of a specific statement, that such names are exempt from the relevant protective laws and regulations and therefore free for general use. Product Liability: The data and other information in this handbook have been carefully extracted and evaluated by experts from the original literature. Furthermore, they have been checked for correctness by authors and the editorial staff before printing. Nevertheless, the publisher can give no guarantee for the correctness of the data and information provided. In any individual case of application, the respective user must check the correctness by consulting other relevant sources of information. Cover layout: Erich Kirchner, Heidelberg Typesetting: Authors and Redaktion Landolt-Börnstein, Darmstadt Printing and Binding: AZ Druck, Kempten SPIN: 1167 2159

63/3020 - 5 4 3 2 1 0 – Printed on acid-free paper

Editor H. Schopper CERN, CH-1211 Geneva 23, Switzerland e-mail: [email protected]

Contributors S.I. Sukhoruchkin Z.N. Soroko Petersburg Nuclear Physics Institute 188300 Gatchina, Leningrad District, Russia e-mail: [email protected]

Landolt-Börnstein Editorial Office Gagernstr. 8, D-64283 Darmstadt, Germany fax: +49 (6151) 171760 e-mail: [email protected] Internet http://www.landolt-boernstein.com

Preface

Nuclear level schemes and resonance parameters are of great interest for nuclear spectroscopy, for astrophysical models, thermonuclear calculations and for other applications. Parameters for nuclear levels of stable nuclei have been published in the Volumes I/16B, I/18A, B, C, and in I/19A1, A2. In the Volumes I/19A, B further data obtained from transfer reactions are presented. Volume I/19C contains the data of unstable nuclei far from the stability region which have been deduced from reactions other than transfer reactions (e.g. beta decay, spallation reactions, or inverse reactions). The data in these volumes should be considered as the most complete data collection for nuclear levels. The contents of the various volumes can be characterized in the following way: Data for unbound states (resonances) I/16B, C I/19A

Low lying levels, neutron-induced resonances (I/16A contains general information on neutron physics) Highly excited levels above the low lying states, unbound states from charged-particle reactions (Z = 2 to 18 in I/19A1, Z = 19 to 83 in I/19A2)

Data for bound states (stable nuclei) I/18A, B, C Low lying levels (Z = 2 to 36 in I/18A, Z = 37 to 62 in I/18B, Z = 63 to 100 in I/18C) In I/18A the theoretical methods of treating nuclei are summarized, in particular those for deformed nuclei. I/19B Excited levels from charged-particle reactions (Z = 3 to 36 in I/19B1, Z = 37 to 62 in I/19B2, Z = 63 to 99 in I/19B3) For the two Volumes I/18 and I/19B the distributions of the Z values to the respective subvolumes are the same. However, Volume I/19B contains data for many more isotopes than Volume I/18. In addition for some of the isotopes listed in Volume I/18 new data became available since its publishing and these have also been included in Volume I/19B, however, duplication of data was avoided. Table 1 in Volume I/19B provides the number of levels registered for each isotope of the various volumes. This should make it easy for the user to find the data of the isotope he or she is looking for. Data for unstable nuclei far from the stability line I/19C

Excited levels for proton-rich and neutron-rich nuclei derived from reactions other than transfer reactions, e.g. beta-decay, spallation reactions or inverse reactions.

In agreement with the Publisher's general effort to make the data available to users by modern methods each subvolume is delivered with a CD ROM which contains all the data of the printed volume but in view of the large amount of data some of the information is given on the CD ROM only.

Preface

VII

The compilation was as usual prepared by eminent experts in the fields. One of the characteristics of Landolt-Börnstein is that data are evaluated before they are accepted for the compilation. The idea is to present 'best values' which can be used with confidence by non-experts. Preparing such best values also implied making corrections necessary because of different energy calibrations in various publications. I would like to thank the authors for their careful work and their flexibility to comply with the wishes of the editor and publisher. Thanks are also due to the members of the Landolt-Börnstein editorial staff who have made major contributions to the successful production of this volume.

Geneva, November 2006

The Editor

Contents

1 1.1 1.2 1.3 1.4 1.5 1.6

Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . General remarks. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . List of notations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . Data presentation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . Interpretation of data of nuclear excitations . . . . . . . . . . . . . . . . . . . . . . . . . . Conclusions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . Acknowledgments . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .

1 1 19 22 23 25 25

2

Tables .

26

63-Europium Eu-145 . . . Eu-146 . . . Eu-147 . . . Eu-148 . . . Eu-149 . . . Eu-150 . . . Eu-151 . . . Eu-152 . . . Eu-153 . . . Eu-154 . . . Eu-155 . . . Eu-156 . . . Eu-157 . . . Eu-159 . . . Eu-160 . . . 64-Gadolinium Gd-146 . . . Gd-147 . . . Gd-148 . . . Gd-149 . . . Gd-150 . . . Gd-151 . . . Gd-152 . . . Gd-153 . . . Gd-154 . . . Gd-155 . . . Gd-156 . . . Gd-157 . . . Gd-158 . . . Gd-159 . . . Gd-160 . . . Gd-161 . . . Gd-162 . . .

............................................

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26 26 27 27 28 29 29 31 34 36 38 39 40 40 40 41 42 42 42 43 43 44 45 47 48 52 55 59 60 65 66 66

65-Terbium Tb-149 . Tb-150 . Tb-151 . Tb-152 . Tb-153 . Tb-154 . Tb-155 . Tb-156 . Tb-157 . Tb-158 . Tb-159 . Tb-160 . Tb-161 . Tb-162 . Tb-163 .

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67 67 67 68 68 69 69 71 71 72 74 76 78 80 80

66-Dysprosium Dy-154 . . . Dy-155 . . . Dy-156 . . . Dy-157 . . . Dy-158 . . . Dy-159 . . . Dy-160 . . . Dy-161 . . . Dy-162 . . . Dy-163 . . . Dy-164 . . . Dy-165 . . . Dy-166 . . .

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81 81 82 84 85 86 87 88 91 96 101 104 106

67-Holmium Ho-157 . Ho-158 . Ho-159 . Ho-160 . Ho-161 . Ho-162 . Ho-163 . Ho-164 . Ho-165 . Ho-166 . Ho-167 . Ho-168 . Ho-169 . Ho-170 .

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107 108 108 110 110 111 112 114 115 117 120 121 122 122

68-Erbium Er-161 Er-162 Er-163 Er-164 Er-165 Er-166 Er-167 Er-168 Er-169 Er-170 Er-171 Er-172

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123 123 124 125 128 130 134 136 146 149 151 152

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Contents 69-Thulium Tm-165 . Tm-166 . Tm-167 . Tm-168 . Tm-169 . Tm-170 . Tm-171 . Tm-172 . Tm-173 . Tm-174 . Tm-175 .

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153 153 154 154 156 157 160 161 161 162 162

70-Ytterbium Yb-166 . . Yb-167 . . Yb-168 . . Yb-169 . . Yb-170 . . Yb-171 . . Yb-172 . . Yb-173 . . Yb-174 . . Yb-175 . . Yb-176 . . Yb-177 . . Yb-178 . .

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163 163 164 166 168 170 173 178 180 184 185 187 188

71-Lutetium Lu-171 . Lu-172 . Lu-173 . Lu-174 . Lu-175 . Lu-176 . Lu-177 . Lu-178 . Lu-179 . Lu-180 .

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189 189 190 191 194 196 197 199 200 200

72-Hafnium Hf-173 . Hf-174 . Hf-175 . Hf-176 . Hf-177 . Hf-178 . Hf-179 . Hf-180 . Hf-181 . Hf-182 . Hf-183 .

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201 201 201 202 203 204 207 210 214 217 217

IX

73-Tantalum Ta-179 . Ta-180 . Ta-181 . Ta-182 . Ta-183 . Ta-184 . Ta-185 .

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218 219 220 221 221 222 222

74-Tungsten W-178 . W-179 . W-180 . W-181 . W-182 . W-183 . W-184 . W-185 . W-186 . W-187 . W-188 .

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223 223 224 224 225 228 231 233 238 240 242

75-Rhenium Re-181 . Re-182 . Re-183 . Re-184 . Re-185 . Re-186 . Re-187 . Re-188 . Re-189 . Re-190 . Re-191 .

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243 244 244 246 246 248 248 250 251 251 251

76-Osmium Os-184 . Os-185 . Os-186 . Os-187 . Os-188 . Os-189 . Os-190 . Os-191 . Os-192 . Os-193 . Os-194 .

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252 252 255 255 257 258 260 262 264 266 266

77-Iridium Ir-183 . Ir-184 . Ir-185 . Ir-186 . Ir-187 . Ir-188 . Ir-189 . Ir-190 . Ir-191 . Ir-192 . Ir-193 . Ir-194 . Ir-195 .

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267 267 267 268 268 268 269 269 272 273 275 276 278

78-Platinum Pt-180 . Pt-181 . Pt-182 . Pt-183 . Pt-184 . Pt-185 . Pt-186 . Pt-187 . Pt-188 . Pt-189 . Pt-190 . Pt-191 . Pt-192 . Pt-193 . Pt-194 . Pt-195 . Pt-196 . Pt-197 . Pt-198 . Pt-199 . Pt-200 .

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279 279 280 281 281 282 284 284 284 285 285 286 288 290 292 294 296 299 301 302 303

79-Gold Au-186 . Au-187 . Au-188 . Au-189 . Au-190 . Au-191 . Au-192 . Au-193 . Au-194 . Au-195 . Au-196 . Au-197 . Au-198 . Au-199 .

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304 304 304 305 305 306 306 306 307 307 308 310 312 315

X

Contents

80-Mercury Hg-184 . Hg-185 . Hg-186 . Hg-187 . Hg-188 . Hg-189 . Hg-190 . Hg-191 . Hg-192 . Hg-193 . Hg-194 . Hg-195 . Hg-196 . Hg-197 . Hg-198 . Hg-199 . Hg-200 . Hg-201 . Hg-202 . Hg-203 . Hg-204 . Hg-205 . Hg-206 .

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317 317 318 318 318 319 319 319 320 320 320 321 321 322 323 324 325 326 328 329 330 330 331

81-Thallium Tl-195 . Tl-196 . Tl-197 . Tl-198 . Tl-199 . Tl-200 . Tl-201 . Tl-202 . Tl-203 . Tl-204 . Tl-205 . Tl-206 . Tl-207 . Tl-208 . Tl-209 .

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332 332 332 333 333 333 333 334 334 336 338 341 342 343 343

82-Lead Pb-196 Pb-197 Pb-198 Pb-199 Pb-200 Pb-201 Pb-202 Pb-203 Pb-204 Pb-205 Pb-206 Pb-207 Pb-208 Pb-209 Pb-210 Pb-211 Pb-212 Pb-214

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344 344 344 345 345 345 346 347 347 350 352 355 359 365 368 369 370 370

83-Bismuth Bi-201 . Bi-202 . Bi-203 . Bi-204 . Bi-205 . Bi-206 . Bi-207 . Bi-208 . Bi-209 . Bi-210 . Bi-211 . Bi-212 . Bi-213 . Bi-214 . Bi-215 .

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371 371 371 372 372 373 375 376 379 382 384 385 386 386 386

84-Polonium Po-196 . Po-197 . Po-198 . Po-199 . Po-200 . Po-201 . Po-202 . Po-203 . Po-204 . Po-205 . Po-206 . Po-207 . Po-208 . Po-209 . Po-210 . Po-211 . Po-212 . Po-213 . Po-214 . Po-215 . Po-216 .

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387 387 387 387 388 388 388 388 389 389 389 389 390 390 391 392 393 394 394 394 394

85-Astatine At-203 . At-204 . At-205 . At-206 . At-207 . At-208 . At-209 .

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395 395 395 395 396 396 396

86-Radon Rn-208 Rn-209 Rn-210 Rn-211 Rn-212 Rn-213 Rn-214 Rn-215 Rn-216 Rn-217 Rn-218 Rn-219 Rn-220 Rn-222

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397 397 397 398 398 398 398 399 399 399 399 400 400 400

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Contents 87-Francium Fr-213 . Fr-214 . Fr-215 . Fr-216 . Fr-217 . Fr-218 . Fr-219 . Fr-220 . Fr-221 . Fr-222 . Fr-223 . Fr-225 .

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401 401 401 401 402 402 402 403 403 404 404 405

88-Radium Ra-212 . Ra-213 . Ra-214 . Ra-215 . Ra-216 . Ra-217 . Ra-218 . Ra-219 . Ra-220 . Ra-221 . Ra-222 . Ra-223 . Ra-224 . Ra-225 . Ra-226 . Ra-227 . Ra-228 .

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406 406 406 406 407 407 407 408 409 409 409 410 410 411 412 413 415

89-Actinium Ac-219 . Ac-220 . Ac-221 . Ac-222 . Ac-223 . Ac-224 . Ac-225 . Ac-226 . Ac-227 . Ac-228 . Ac-229 . Ac-230 . Ac-231 . Ac-232 .

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416 416 416 416 417 417 417 417 418 419 419 420 420 420

90-Thorium Th-217 . Th-218 . Th-220 . Th-221 . Th-222 . Th-223 . Th-224 . Th-225 . Th-226 . Th-227 . Th-228 . Th-229 . Th-230 . Th-231 . Th-232 . Th-233 . Th-234 .

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XI

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421 421 421 421 422 422 422 422 423 423 423 424 425 427 429 430 431

91-Protactinium Pa-229 . . . Pa-230 . . . Pa-231 . . . Pa-232 . . . Pa-233 . . . Pa-234 . . . Pa-235 . . . Pa-236 . . . Pa-237 . . .

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432 434 434 435 435 436 437 437 437

92-Uranium U-230 . U-231 . U-232 . U-233 . U-234 . U-235 . U-236 . U-237 . U-238 . U-239 . U-240 .

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438 438 438 439 440 443 447 449 451 452 453

93-Neptunium Np-233 . . Np-234 . . Np-235 . . Np-236 . . Np-237 . . Np-238 . . Np-239 . . Np-240 . . Np-242 . .

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454 454 454 455 455 456 457 458 458

94-Plutonium Pu-235 . . Pu-236 . . Pu-237 . . Pu-238 . . Pu-239 . . Pu-240 . . Pu-241 . . Pu-242 . . Pu-243 . . Pu-244 . . Pu-245 . . Pu-246 . .

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459 459 459 460 461 463 464 466 467 469 469 469

95-Americium Am-239. . Am-240. . Am-241. . Am-242. . Am-243. . Am-244. . Am-245. .

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470 470 471 471 472 473 473

96-Curium Cm-242 . Cm-243 . Cm-244 . Cm-245 . Cm-246 . Cm-247 . Cm-248 . Cm-249 . Cm-250 .

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474 474 474 475 475 476 477 478 478

97-Berkelium Bk-247 . . Bk-248 . . Bk-249 . . Bk-250 . . Bk-251 . .

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479 479 479 480 480

98-Californium Cf-246 . . . Cf-247 . . . Cf-248 . . . Cf-249 . . . Cf-250 . . . Cf-251 . . . Cf-252 . . . Cf-253 . . .

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481 481 481 481 482 482 482 482

99-Einsteinium Es-251 . . . Es-252 . . . Es-253 . . . Es-254 . . .

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483 483 483 483 3 References . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 484 Supplement (complete sets of data) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . CD-ROM

Excitations from reactions with charged particles

1

Introduction

1.1

General remarks

1

This report is the third part, Volume I/19B3, of the compilation of parameters of nuclear bound states excited in reactions with charged particles – Volume I/19B (consisting of 3 subvolums covering different ranges of Z). The data were collected in a Combined charged particle Reaction File (CRF), which contains also data on very unstable nuclei (in volume I/19C). Properties of low-lying levels of many nuclei were considered in LB volumes I/18A [01Sc0A], I/18B [02Sc0A], I/18C [03Sc0A]. Data on unbound states derived from neutron and charged particle resonances were published in LB volumes I/16 [98Sc0A, 04BrZU] and I/19A [04Sc0B, 05Sc0A]. Existing high-quality information on excited bound states situated above the low-lying levels but below the states seen as resonances is essential for understanding of general properties of nuclei and is important for many applications. The compilation Vol. I/19B contains information on parameters of bound excited states which were obtained in high-resolution measurements with charged particle spectrometers. Frequently these data are combined with data obtained in measurements of γ-ray spectra after neutron capture, in β-decay study, etc. We have collected existing information on parameters of nucleon transfer reactions: total and differential cross sections, spectroscopic factors, parameters of few-nucleon transfer, etc. These parameters were not considered (with very few exceptions) in the recent compilation LB I/18ABC. We include also data for many neighbour nuclei not presented in LB I/18ABC. As a result, information on all nuclei with exception of proton-rich and neutron-rich nuclei situated very far from the valley of stability (for which data will be published in LB I/19C) is presented in both compilations I/18ABC and I/19B. Data on nuclear excitations are contained in four Volumes, respectively: for nuclei with Z ≤ 36, 37 ≤ Z ≤ 62, Z ≥ 63, and for very unstable nuclei (LB I/19C). These regions of Z are the same as in the compilations LB I/18ABC, where theoretical parametertization of properties of nuclear low-lying levels are presented. We give data for the broader range of nuclei and pay attention to the parameters of nucleon transfer reactions. To avoid duplication with the material in compilations LB I/18, LB I/16 and LB I/19A (resonance parameters) we present in the book data obtained mainly from transfer reactions with charged particles. Other information, branching ratios of radiative transitions from bound excited states, is given mainly in the Supplement (on CD). Numbers of excited states in Volume 19B (in the book and in the Supplement) are given in Tables 1.1, 1.2 and 1.3 (for the three Volumes 19B3, 19B1 and 19B2, respectively) as a ”ratio” in the first column. The asterisk marks the number of levels in very unstable isotopes which are considered in volume I/19C. These Tables also contain the numbers of excited states presented in all the LB-compilations I/18ABC, I/19A, I/16BC, I/19BC mentioned above. We have collected the original data on different reactions with charged-particles from papers published during the last 25-35 years. Data on energies of excited states and T1/2 were taken from publications in Nuclear Data Sheets (NDS) [04Nu0A]. We give references on NDS in the headings of isotope-tables, usually before other references. Data in NDS evaluations (ENSDF – Evaluated Nuclear Structure Data File) were used to facilitate the presentation of the experimental material on cross sections and spectroscopic factors of reactions with charged particles. All data were grouped according to the common Z and A of the compound nuclei formed in different reactions. The international Nuclear Science Reference system (NSR) was widely used during the collection of data. Modern PC-capacities and the NSR-file permitted to collect and represent in a common format all data scattered in the literature. We have selected data from the original works mentioned in NSR and used the corresponding identification number of each paper in NSR. In some cases we have tried to find so-called ”best values” from the most recent original works, in other cases we give several sets of data from different original works for comparison.

Landolt-B¨ ornstein New Series I/19B3


2

Table 1.1. Numbers of bound states in compound nuclei A Z with 63 ≤ Z ≤ 99 contained in the third part of this compilation (I/19B3). The ratio shows the number of states in Volume I/19B3 and its Supplement. Asterisks mark isotopes included in volume I/19C. The number of bound states in the compilation LB I/18C, the number of resonances in reactions with charged particles in the compilation LB I/19A2 and the number of neutron resonances in the compilation LB I/16C are given in the same line for comparison. A

Z Eu 137 Eu 138 Eu 139 Eu 140 Eu 141 Eu 144 Eu 143 Eu 144 Eu 145 Eu 146 Eu 147 Eu 148 Eu 149 Eu 150 Eu 151 Eu 152 Eu 153 Eu 154 Eu 155 Eu 156 Eu 157 Eu 159 Eu 138 Gd 139 Gd 140 Gd 141 Gd 142 Gd 143 Gd 144 Gd 145 Gd 146 Gd 147 Gd 148 Gd 149 Gd 150 Gd 151 Gd 152 Gd 153 Gd 154 Gd 155 Gd 156 Gd 157 Gd 136

19B3 1* 7* 49* 62* 28* 61* 127* 202* 144* 14/204 4/35 17/157 3/104 48/130 3/84 78/176 91/195 85/167 113/159 59/80 6/32 3/40 22/31 34* 57* 23* 65* 111* 105* 158* 151* 60/196 3/199 19/304 2/393 5/393 27/107 19/158 89/221 53/227 175/217 148/272 185/325

18C 19A 16C

A

Z Gd 159 Gd 160 Gd 161 Gd 162 Gd 141 Tb 142 Tb 143 Tb 144 Tb 145 Tb 146 Tb 147 Tb 148 Tb 149 Tb 150 Tb 151 Tb 152 Tb 153 Tb 154 Tb 155 Tb 156 Tb 157 Tb 158 Tb 159 Tb 160 Tb 161 Tb 162 Tb 163 Tb 140 Dy 142 Dy 143 Dy 144 Dy 145 Dy 146 Dy 147 Dy 148 Dy 149 Dy 150 Dy 151 Dy 152 Dy 153 Dy 154 Dy 155 Dy 158

19

2 16 38 12 42 19

2 106 22 77 19 7

43 43

18 45 40 24 27 26 22

131 9 162 95 87

19B3 53/217 228/298 46/103 33/51 15/20 5* 12* 103* 31* 19* 46* 94* 82* 9/178 2/115 2/266 2/100 32/138 4/37 47/86 21/68 38/152 96/96 100/116 86/174 52/69 8/8 34/36 5* 6* 79* 14* 12* 21* 20* 56* 58* 85* 130* 249* 132* 19/145 30/171

18C 19A 16C 25 88 12 96 24 58

26 36 13 18 15 14 8

39

2 443 3

A

Z Dy 157 Dy 158 Dy 159 Dy 160 Dy 161 Dy 162 Dy 163 Dy 164 Dy 165 Dy 166 Dy 167 Dy 168 Dy 141 Ho 145 Ho 147 Ho 148 Ho 149 Ho 150 Ho 151 Ho 152 Ho 153 Ho 154 Ho 155 Ho 156 Ho 157 Ho 158 Ho 159 Ho 160 Ho 161 Ho 162 Ho 163 Ho 164 Ho 165 Ho 166 Ho 167 Ho 168 Ho 169 Ho 170 Ho 145 Er 147 Er 148 Er 149 Er 156

19B3 40/314 87/113 16/96 61/124 33/245 109/141 196/246 267/292 115/167 105/178 29/31 3* 4* 15* 4* 5* 16* 81* 16* 65* 31* 105* 37* 67* 150* 64/247 2/117 62/125 2/71 56/109 5/16 70/78 32/34 140/276 162/330 29/31 2/5 32/32 1/1 4* 1* 8* 14*

18C 16C 62 20 40 32 7 44 39 114 31 256 44 142 25 131 8 117

18 12 19 9

374 3



3

Table 1.1. (continued) Numbers of bound states in compound nuclei A Z with 63 ≤ Z ≤ 99 contained in the third part of this compilation (I/19B3). The ratio shows the number of states in Volume I/19B3 and its Supplement. Asterisks mark isotopes included in volume I/19C. The number of bound states in the compilation LB I/18C, the number of resonances in reactions with charged particles in the compilation LB I/19A2 and the number of neutron resonances in the compilation LB I/16C are given in the same line for comparison. A

Z Er 151 Er 152 Er 153 Er 154 Er 155 Er 156 Er 157 Er 158 Er 159 Er 160 Er 161 Er 162 Er 163 Er 164 Er 165 Er 166 Er 167 Er 168 Er 169 Er 170 Er 171 Er 172 Er 145 Tm 146 Tm 147 Tm 150 Tm 151 Tm 152 Tm 153 Tm 154 Tm 155 Tm 156 Tm 157 Tm 158 Tm 159 Tm 160 Tm 161 Tm 162 Tm 163 Tm 164 Tm 165 Tm 166 Tm 150

19B3 28* 57* 53* 41* 83* 97* 113* 114* 129* 186* 116* 26/122 13/110 74/383 23/204 99/105 144/172 77/200 423/427 118/143 89/161 55/73 26/41 5* 2* 12* 5* 19* 19* 63* 2* 6* 14* 72* 44* 73* 68* 95* 212* 97* 175* 23/201 1/1

18C 16C

A

Z Tm 168 Tm 169 Tm 170 Tm 171 Tm 172 Tm 173 Tm 174 Tm 175 Tm 151 Yb 152 Yb 153 Yb 154 Yb 155 Yb 156 Yb 157 Yb 158 Yb 159 Yb 160 Yb 161 Yb 162 Yb 163 Yb 164 Yb 165 Yb 166 Yb 167 Yb 168 Yb 169 Yb 170 Yb 171 Yb 172 Yb 173 Yb 174 Yb 175 Yb 176 Yb 177 Yb 178 Yb 153 Lu 154 Lu 155 Lu 156 Lu 157 Lu 159 Lu 167

23 32 41 28 26 27 17 55 5 12

18 19 174 276 130 125

22

19B3 18/137 76/142 26/151 116/258 19/49 4/13 5/33 2/4 21/31 10* 6* 14* 28* 5* 20* 2* 55* 45* 88* 74* 72* 62* 134* 97* 16/114 21/176 59/164 76/173 95/198 100/176 204/308 96/112 157/375 60/183 40/69 47/156 25/31 9* 15* 14* 16* 1* 32*

18C 19A 16C 12 1 12 11

22 25 14 31 51 17 41 18 23 8 6

1 432 13 4

7 22 24 170 101 167 79 69

A

Z Lu 161 Lu 162 Lu 163 Lu 164 Lu 165 Lu 166 Lu 167 Lu 168 Lu 169 Lu 170 Lu 171 Lu 172 Lu 173 Lu 174 Lu 175 Lu 176 Lu 177 Lu 178 Lu 179 Lu 180 Lu 154 Hf 156 Hf 157 Hf 158 Hf 159 Hf 160 Hf 161 Hf 162 Hf 163 Hf 164 Hf 165 Hf 166 Hf 167 Hf 168 Hf 169 Hf 170 Hf 171 Hf 172 Hf 173 Hf 174 Hf 175 Hf 176 Hf 160

19B3 26* 73* 104* 219* 193* 152* 9* 169* 38* 56* 203* 25/202 23/39 38/81 143/168 105/125 9/166 135/203 23/41 14/34 2/12 6* 7* 24* 32* 15* 26* 16* 52* 21* 57* 75* 64* 83* 119* 39* 100* 154* 109* 2/129 7/189 10/117 56/217

18C 19A 16C

11

7

12

6

13 24 19

13

11 10 6 21

10

449 59

11



4


Z Hf 178 Hf 179 Hf 180 Hf 181 Hf 182 Hf 183 Hf 184 Hf 157 Ta 158 Ta 159 Ta 164 Ta 165 Ta 166 Ta 167 Ta 168 Ta 169 Ta 170 Ta 171 Ta 172 Ta 173 Ta 174 Ta 175 Ta 176 Ta 177 Ta 178 Ta 179 Ta 180 Ta 181 Ta 182 Ta 183 Ta 184 Ta 185 Ta 158 W 160 W 162 W 164 W 165 W 166 W 167 W 168 W 169 W 170 W 171 W 177

19B3 3/145 119/161 121/186 121/246 137/179 9/19 2/7 0/4 2* 1* 4* 1* 24* 4* 70* 29* 10* 52* 77* 57* 64* 127* 126* 128* 184* 20* 49/135 53/246 57/116 1/154 3/19 2/6 19/24 1* 12* 1* 15* 33* 41* 51* 67* 37* 66* 82*

18C 19A 16C 25 128 38 197 32 215 23 154 150

9 22 12

2 61 772 24

A

Z W 173 W 174 W 175 W 176 W 177 W 178 W 179 W 180 W 181 W 182 W 183 W 184 W 185 W 186 W 187 W 188 W 190 W 161 Re 162 Re 163 Re 165 Re 167 Re 168 Re 169 Re 170 Re 171 Re 172 Re 173 Re 174 Re 175 Re 176 Re 177 Re 178 Re 179 Re 180 Re 181 Re 182 Re 183 Re 184 Re 185 Re 186 Re 187 Re 188 Re 172

19B3 49* 41* 29* 43* 127* 157* 37/76 17/184 45/119 38/91 92/122 123/145 83/191 322/367 69/76 94/192 23/23 6* 5* 1* 1* 1* 2* 2* 1* 8* 95* 10* 74* 35* 113* 114* 251* 68* 103* 101* 120/162 4/48 170/181 29/113 54/66 39/167 47/78 48/81

18C 19A 16C

A

Z Re 190 Re 191 Re 193 Re 164 Os 166 Os 167 Os 168 Os 169 Os 170 Os 171 Os 172 Os 173 Os 174 Os 175 Os 176 Os 177 Os 178 Os 179 Os 180 Os 181 Os 182 Os 183 Os 184 Os 185 Os 186 Os 187 Os 188 Os 189 Os 190 Os 191 Os 192 Os 193 Os 194 Os 196 Os 165 Ir 166 Ir 167 Ir 172 Ir 173 Ir 174 Ir 175 Ir 176 Ir 177 Ir 189

17 23 27 21 32 9

6 1 250 313 197 7 175

18 6 8

503 3 399

19B3 11/22 1/4 15/39 2* 5* 12* 8* 23* 14* 28* 71* 78* 66* 70* 71* 56* 57* 59* 134* 143* 249* 148* 91* 16/49 172/191 29/164 45/65 53/125 53/90 95/145 64/77 82/106 13/262 17/18 2* 1* 1* 1* 3* 47* 1* 54* 128* 122*

18C 16C 4

17 23 17 15 12 13

129 177 101 22 24

14 20



5


Z Ir 179 Ir 180 Ir 181 Ir 182 Ir 183 Ir 184 Ir 185 Ir 186 Ir 187 Ir 188 Ir 189 Ir 190 Ir 191 Ir 192 Ir 193 Ir 194 Ir 195 Ir 196 Ir 197 Ir 199 Ir 168 Pt 170 Pt 171 Pt 172 Pt 173 Pt 174 Pt 175 Pt 176 Pt 177 Pt 178 Pt 179 Pt 180 Pt 181 Pt 182 Pt 183 Pt 184 Pt 185 Pt 186 Pt 187 Pt 188 Pt 189 Pt 190 Pt 178

19B3 2* 89* 84* 181* 41* 3/52 5/71 5/90 8/95 4/68 3/19 17/85 108/157 33/71 82/231 53/77 51/166 38/44 5* 23* 2* 3* 6* 6* 10* 8* 11* 17* 28* 51* 26* 59* 4/92 128/138 85/93 4/103 87/87 181/191 5/95 5/73 4/72 18/47 20/55

18C 19A 16C

A

Z Pt 192 Pt 193 Pt 194 Pt 195 Pt 196 Pt 197 Pt 198 Pt 199 Pt 200 Pt 170 Au 171 Au 173 Au 175 Au 176 Au 177 Au 179 Au 181 Au 182 Au 183 Au 184 Au 185 Au 186 Au 187 Au 188 Au 189 Au 190 Au 191 Au 192 Au 193 Au 194 Au 195 Au 196 Au 197 Au 198 Au 199 Au 200 Au 201 Au 203 Au 176 Hg 177 Hg 178 Hg 179 Hg 191

31 4 6 21 28 11 17 16

4 17 17

21

62 11 54

19B3 100/100 73/133 82/89 70/150 97/114 111/141 76/104 56/64 21/61 35/38 1* 1* 5* 12* 28* 34* 3* 69* 13* 70* 59* 92* 4/84 5/91 5/49 4/275 5/46 3/97 2/33 51/89 3/24 29/45 132/215 45/76 155/158 52/69 11* 20* 12* 7* 3* 6* 6*

18C 19A 16C 2 15 12 12 27 19 8 53 44 6 10 5

12

31

8 21 10 52 10

270

A

Z Hg 181 Hg 182 Hg 183 Hg 184 Hg 185 Hg 186 Hg 187 Hg 188 Hg 189 Hg 190 Hg 191 Hg 192 Hg 193 Hg 194 Hg 195 Hg 196 Hg 197 Hg 198 Hg 199 Hg 200 Hg 201 Hg 202 Hg 203 Hg 204 Hg 205 Hg 206 Hg 177 Tl 179 Tl 181 Tl 183 Tl 184 Tl 185 Tl 186 Tl 187 Tl 188 Tl 189 Tl 190 Tl 191 Tl 192 Tl 193 Tl 194 Tl 195 Tl 180

19B3 36* 35* 43* 55* 4/18 50/50 5/89 4/34 4/81 3/74 3/196 3/218 3/156 6/139 7/154 5/207 19/68 23/60 24/97 52/84 23/98 78/79 37/83 76/78 7/63 52/53 9/10 1* 1* 1* 12* 2* 24* 8* 52* 8* 78* 24* 84* 73* 95* 125* 6/88

18C 19A 16C

12 18

10 9 2 27 6 49 9 18

73 88 44 86 38

15 23

21



6


Z Tl 197 Tl 198 Tl 199 Tl 200 Tl 201 Tl 202 Tl 203 Tl 204 Tl 205 Tl 206 Tl 207 Tl 208 Tl 209 Tl 210 Tl 182 Pb 183 Pb 184 Pb 185 Pb 186 Pb 187 Pb 188 Pb 189 Pb 190 Pb 191 Pb 192 Pb 193 Pb 194 Pb 195 Pb 196 Pb 197 Pb 198 Pb 199 Pb 200 Pb 201 Pb 202 Pb 203 Pb 204 Pb 205 Pb 206 Pb 207 Pb 208 Pb 209 Pb 196

19B3 5/35 21/58 3/31 3/34 6/16 15/63 12/15 71/103 86/86 73/88 81/94 23/42 2/10 7/7 5* 6* 1* 5* 3* 17* 8* 22* 7* 32* 7* 109* 137* 217* 136* 5/149 2/184 2/199 4/152 5/69 4/69 40/61 22/63 81/156 152/183 151/335 160/205 247/605 174/226

18C 19A 16C 5 20 5 10 7 3 11 32 7 7

10

138 2 139

14

7 20 23 54 1 25 84 1 23 100 15

242 410 382 94

A

Z Pb 211 Pb 212 Pb 214 Pb 184 Bi 186 Bi 187 Bi 188 Bi 189 Bi 190 Bi 191 Bi 192 Bi 193 Bi 194 Bi 195 Bi 196 Bi 197 Bi 198 Bi 199 Bi 200 Bi 201 Bi 202 Bi 203 Bi 204 Bi 205 Bi 206 Bi 207 Bi 208 Bi 209 Bi 210 Bi 211 Bi 212 Bi 213 Bi 214 Bi 215 Bi 216 Bi 190 Po 191 Po 192 Po 193 Po 194 Po 195 Po 196 Po 210

19B3 60/65 19/24 18/18 1/1 1* 1* 6* 1* 9* 2* 3* 1* 43* 4* 16* 17* 41* 49* 33* 37* 8/58 6/37 7/46 5/41 39/74 36/45 28/62 116/199 119/204 104/107 41/62 8/12 4/4 9/11 1/3 1* 6* 1* 5* 7* 18* 5* 3/22

18C 19A 16C 6

12 25 14 31 15 20 11

1 3

13

1 4 44 8 178

A

Z Po 198 Po 199 Po 200 Po 201 Po 202 Po 203 Po 204 Po 205 Po 206 Po 207 Po 208 Po 209 Po 210 Po 211 Po 212 Po 213 Po 214 Po 215 Po 216 Po 217 Po 218 Po 193 At 195 At 197 At 198 At 199 At 200 At 201 At 202 At 203 At 204 At 205 At 206 At 207 At 208 At 209 At 210 At 211 At 212 At 213 At 214 At 215 At 197

19B3 5/5 3/55 3/25 3/44 3/23 3/42 8/54 3/70 7/54 2/98 7/63 6/52 15/51 41/76 38/97 5/30 2/9 3/81 2/14 4/10 3* 11* 2* 1* 3* 1* 5* 3* 8* 2* 3/20 1/1 2/32 11/31 5/34 2/40 1/62 124* 115* 66* 6* 23* 6*

18C 19A 16C

35 30 15 10 14 28 5 10 2 16

8 19 8 8 4 2



7


Z At 217 At 219 At 197 Rn 198 Rn 199 Rn 201 Rn 202 Rn 203 Rn 204 Rn 205 Rn 216 At 217 At 219 At 197 Rn 198 Rn 199 Rn 201 Rn 202 Rn 203 Rn 204 Rn 205 Rn 206 Rn 207 Rn 208 Rn 209 Rn 210 Rn 211 Rn 212 Rn 213 Rn 214 Rn 215 Rn 216 Rn 217 Rn 218 Rn 219 Rn 220 Rn 222 Rn 200 Fr 201 Fr 202 Fr 204 Fr 206 Fr 216

19B3 18* 15* 4* 1* 5* 1* 2* 14* 18* 51* 25* 18* 15* 4* 1* 5* 1* 2* 14* 18* 51* 25* 18* 20* 3/41 8/46 4/31 5/57 3/33 2/53 2/48 4/4 2/20 2/11 3/23 30/30 16/20 12/12 1* 1* 1* 2* 2*

18C 19A 16C

A

Z Fr 210 Fr 211 Fr 212 Fr 213 Fr 214 Fr 215 Fr 216 Fr 217 Fr 218 Fr 219 Fr 220 Fr 221 Fr 222 Fr 223 Fr 225 Fr 227 Fr 206 Ra 207 Ra 208 Ra 209 Ra 210 Ra 211 Ra 212 Ra 213 Ra 214 Ra 215 Ra 216 Ra 217 Ra 218 Ra 219 Ra 220 Ra 221 Ra 222 Ra 223 Ra 224 Ra 225 Ra 226 Ra 227 Ra 228 Ra 229 Ra 230 Ra 231 Ra 209

22 4 2 2 12

3 4

19B3 11* 16* 26* 43* 3/41 3/58 3/21 3/27 3/18 30/30 3/30 5/34 40/46 1/1 11/58 45/51 38* 4* 3* 6* 9* 11* 4* 3/13 4/5 3/50 2/32 3/21 26/35 50/50 52/52 31/31 3/10 3/24 3/65 24/52 70/70 31/61 78/84 15/39 32* 23* 30*

18C 19A 16C

A

Z Ac 208 Ac 212 Ac 214 Ac 215 Ac 216 Ac 217 Ac 218 Ac 219 Ac 220 Ac 221 Ac 222 Ac 223 Ac 224 Ac 225 Ac 226 Ac 227 Ac 228 Ac 229 Ac 230 Ac 231 Ac 232 Ac 216 Th 217 Th 218 Th 220 Th 221 Th 222 Th 223 Th 224 Th 225 Th 226 Th 227 Th 228 Th 229 Th 230 Th 231 Th 232 Th 233 Th 234 Th 222 Pa 223 Pa 229 Pa 206

17

8

5

3 32 12 17

7 18 11 12 25 11 11 11

41

19B3 3* 1* 2* 2* 5* 1* 10* 36* 3/44 3/61 1/1 3/3 3/10 3/39 3/16 3/17 56/63 3/4 27/32 18/18 21/25 3/3 8* 1/1 2/5 3/17 3/13 3/26 3/27 3/18 5/5 3/24 3/57 28/91 9/64 50/87 83/97 64/96 84/226 9/13 2* 1* 78/78

18C 19A 16C

22

11 12 30 4 13 12 12

11 10 16 10 11 7 50 23 28 54 32 46 11

3 31 30 714



8


Z Pa 231 Pa 232 Pa 233 Pa 234 Pa 235 Pa 236 Pa 237 Pa 226 U 228 U 229 U 230 U 231 U 232 U 233 U 234 U 235 U 236 U 237 U 238 U 239 U 240 U 232 Np 233 Np 234 Np 235 Np 236 Np 237 Np 238 Np 239 Np 240 Np 242 Np 243 Np 234 Pu 235 Pu 236 Pu 237 Pu 238 Pu 239 Pu 230

19B3 1/1 60/87 1/1 35/74 3/7 17/24 3/6 13/20 12* 1* 1* 3/15 7/7 14/40 73/87 98/150 138/213 93/120 52/270 61/152 50/108 21/21 0/1 2/14 1/1 43/47 4/4 45/105 21/129 41/63 2/10 2/7 22* 1* 1/1 6/10 56/58 25/46 63/96

18C 19A 16C

A

Z Pu 241 Pu 242 Pu 243 Pu 244 Pu 245 Pu 246 Pu 237 Am 238 Am 239 Am 240 Am 241 Am 242 Am 243 Am 244 Am 245 Am 246 Am 237 Cm 238 Cm 239 Cm 240 Cm 241 Cm 242 Cm 243 Cm 244 Cm 245 Cm 246 Cm 247 Cm 248 Cm 249 Cm 250 Cm 241 Bk 242 Bk 243 Bk 244 Bk 245 Bk 247 Bk 248 Bk 249 Bk 240

34 28

138 33 22

7 9

10 27 34 54 37 27 38 43 45

44 770 144 3184 297 36 1692

21 30 48 31

28 26 42

41 752 17

2 64

19B3 29/132 96/106 24/54 61/69 12/46 14/21 2/12 1* 1* 2/11 57/60 24/110 69/141 23/29 30/114 2/21 8* 1* 1* 1* 3* 7* 5/5 27/30 2/14 33/62 51/64 52/56 20/44 50/50 1/1 3* 3* 4* 4* 3* 20/24 5/21 33/51

18C 19A 16C 38 1040 41 430 21 243 33 255 14

11 21 17 51 15 55 14

10 29 38 15 12 24

22

35

195 106 240

13 105 68 91 17 44 50

A

Z Bk 251 Bk 243 Cf 244 Cf 245 Cf 246 Cf 247 Cf 248 Cf 249 Cf 250 Cf 251 Cf 252 Cf 253 Cf 243 Es 244 Es 245 Es 246 Es 247 Es 251 Es 252 Es 253 Es 254 Es 247 Fm 248 Fm 249 Fm 250 Fm 251 Fm 252 Fm 253 Fm 254 Fm 255 Fm 256 Fm 247 Md 251 No 252 No 253 No 254 No 250

19B3 2/40 2/11 3* 2* 2* 1/2 12/12 2/18 2/55 2/47 2/60 2/9 2/5 2* 2* 1* 2* 1* 2/24 2/7 2/7 2/9 2* 1* 4* 10* 9* 1* 2* 4* 7* 27* 0* 6* 10* 22* 8*

18C 19A 16C 37 40 11

12 16 38 36 32 9 5

63 4 4 37

19 7 9

8

4 22

32



9

Table 1.2. Numbers of bound states in compound nuclei A Z with Z ≤ 36 contained in the first part of this compilation (I/19B1). The ratio shows the number of states in this volume and in the Supplement. The number of bound states in the compilation LB I/18A, the number of resonances in reactions with charged particles in compilation LB I/19A and the number of neutron resonances in the compilation LB I/16C are given in the same line for comparison. Asterisks mark the number of states in nuclei with Z ≤ 36 situated far from the stability-line and included in volume I/19C. A

Z H 5 H 4 He 5 He 6 He 7 He 8 He 9 He 10 He 4 Li 5 Li 6 Li 7 Li 8 Li 9 Li 10 Li 11 Li 6 Be 7 Be 8 Be 9 Be 10 Be 11 Be 12 Be 14 Be 8 B 9 B 10 B 11 B 12 B 13 B 14 B 15 B 16 B 17 B 9 C 10 C 11 C 12 C 13 C 14 C 15 C 16 C 17 C 4

19B1 4* 1* 15* 11* 7* 2* 4* 2* 2* 3* 13* 12/13 7/9 6/10 5/7 11* 3* 4* 8* 25* 13/32 37/40 14/15 19* 1* 4/4 11/20 14/39 4/40 15/49 14/22 8/15 8* 2* 1* 1* 8* 13/36 27/55 13/72 24/45 16/30 17/20 3/3

18A 19A 16C

A

Z C 19 C 11 N 12 N 13 N 14 N 15 N 16 N 17 N 18 N 19 N 13 O 14 O 15 O 16 O 17 O 18 O 19 O 20 O 21 O 22 O 15 F 16 F 17 F 18 F 19 F 20 F 21 F 22 F 23 F 24 F 25 F 16 Ne 17 Ne 18 Ne 19 Ne 20 Ne 21 Ne 22 Ne 23 Ne 24 Ne 25 Ne 26 Ne 28 Ne 18

8 11

4 3

8

12 11

9 7 7

1 4 4

1 7 23 8 5

1 4 51 33 5

1 4 28 46 34

8 13

3 18 8

13 34

58 37 4

19B1 3* 1* 5* 30* 18/53 61/121 21/115 14/65 21/35 7* 5* 3* 17* 8/84 38/133 36/119 31/123 21/55 15/22 5* 5* 1* 27* 36/76 25/100 51/190 49/152 14/36 7/22 4/6 2* 2* 1* 12* 21* 70* 28/232 33/116 65/101 12/34 1/12 2/7 4* 3*

18A 19A 16C

A

Z Ne 18 Na 19 Na 20 Na 21 Na 22 Na 23 Na 24 Na 25 Na 26 Na 27 Na 28 Na 29 Na 30 Na 31 Na 21 Mg 22 Mg 23 Mg 24 Mg 25 Mg 26 Mg 27 Mg 28 Mg 29 Mg 30 Mg 31 Mg 32 Mg 33 Mg 34 Mg 22 Al 23 Al 24 Al 25 Al 26 Al 27 Al 28 Al 29 Al 30 Al 31 Al 32 Al 35 Al 24 Si 25 Si 26 Si 30

7

10 16

12 11 23

41 154 133 61 7 47

5 95 215 70 92 33 15 21

2

48

91 432 254 66

20 27 42

13 13 48 282 74 102 65 45 20

19B1 1* 4* 6* 6/24 14/64 36/214 73/172 78/119 13/42 20/24 18/18 10* 6* 1* 2* 12/21 18/60 66/78 77/245 56/131 48/204 23/55 3/24 13* 12* 11* 7* 4* 2* 2* 7* 46* 8/64 64/201 46/243 33/166 8/49 21* 15* 5* 1* 2* 12* 35*

18A 19A 16C

94

11 11 11 52 60 264 1 114

11 11

59 51 79

76

11 21 385 67 64 155 35 12

4 47 146 258 7 260

1 1 7 Landolt-B¨ ornstein New Series I/19B3


10

Table 1.2. (continued) Numbers of bound states in compound nuclei A Z with Z ≤ 36 contained in the first part of this compilation (I/19B1). The ratio shows the number of states in this volume and in the Supplement. The number of bound states in the compilation LB I/18A, the number of resonances in reactions with charged particles in compilation LB I/19A and the number of neutron resonances in the compilation LB I/16C are given in the same line for comparison. Asterisks mark the number of states in nuclei with Z ≤ 36 situated far from the stability-line and included in volume I/19C. A

Z Si 28 Si 29 Si 30 Si 31 Si 32 Si 33 Si 34 Si 35 Si 36 Si 37 Si 38 Si 27 P 28 P 29 P 30 P 31 P 32 P 33 P 34 P 35 P 36 P 37 P 39 P 30 S 31 S 32 S 33 S 34 S 35 S 36 S 37 S 38 S 39 S 40 S 41 S 42 S 43 S 44 S 31 Cl 32 Cl 33 Cl 34 Cl 27

19B1 37/85 74/294 25/129 31/135 42/74 37/58 4* 6* 3* 3* 1* 1* 6* 15/33 15/68 33/149 127/171 147/147 21/35 3/12 19* 5* 5* 3* 1/5 40/60 146/256 27/151 39/133 36/59 7/23 33/39 16* 1* 10* 2* 4* 2* 3* 19/24 8/47 1/84 33/120

18A 19A 16C 24 64 314 52 37 81 108 69 31 30

46

77 97 504 33

9 42 315 64 156 105 100 104 60 82 17 1

4 65 194

A

Z Cl 36 Cl 37 Cl 38 Cl 39 Cl 40 Cl 41 Cl 42 Cl 45 Cl 33 Ar 34 Ar 35 Ar 36 Ar 37 Ar 38 Ar 39 Ar 40 Ar 41 Ar 42 Ar 43 Ar 44 Ar 45 Ar 46 Ar 35 K 36 K 37 K 38 K 39 K 40 K 41 K 42 K 43 K 44 K 45 K 46 K 47 K 48 K 37 Ca 38 Ca 39 Ca 40 Ca 41 Ca 42 Ca 35

19B1 134/248 92/127 28/84 24/39 16/26 18* 4* 11* 1* 7* 20* 38* 10/186 39/105 79/219 39/75 108/198 57/126 29/64 3/14 6/12 3/3 6* 13* 15* 90* 23/86 34/93 45/100 123/205 56/171 27/65 10/18 15/26 11/15 27/27 4/4 1* 24* 58/85 109/580 204/271 105/544

18A 19A 16C 41 224 84 77 422 16 37

41

179

1 133 578 4 73

59 207

78 70

99

87

70 256 39 110

53

382

253 127 415 9

A

Z Ca 44 Ca 45 Ca 46 Ca 47 Ca 48 Ca 49 Ca 50 Ca 51 Ca 52 Ca 38 Sc 39 Sc 40 Sc 41 Sc 42 Sc 43 Sc 44 Sc 45 Sc 46 Sc 47 Sc 48 Sc 49 Sc 50 Sc 51 Sc 52 Sc 54 Sc 56 Sc 42 Ti 43 Ti 44 Ti 45 Ti 46 Ti 47 Ti 48 Ti 49 Ti 50 Ti 51 Ti 52 Ti 53 Ti 54 Ti 56 Ti 43 V 44 V 43

19B1 111/150 73/91 82/103 38/90 102/135 119/247 26/58 10/35 12/13 6/6 1* 2* 9/41 25/200 85/118 105/142 101/116 53/210 177/255 49/144 57/101 149/213 42/50 9/19 6* 8* 7* 16/31 12/15 43/114 39/43 120/248 95/212 118/289 98/108 117/259 22/33 4/24 11* 9* 4* 1* 1*

18A 19A 16C 64 95 45 55 65 6 1 44 39

31 21 22 36 14 25 18

21 12 44 36 78 34 15 10 10

182 112 315 4 1110 197 294 107

66 106 114 118 87 79 34



11


Z V 46 V 47 V 48 V 49 V 50 V 51 V 52 V 53 V 54 V 57 V 60 V 46 Cr 47 Cr 48 Cr 49 Cr 50 Cr 51 Cr 52 Cr 53 Cr 54 Cr 55 Cr 56 Cr 57 Cr 58 Cr 59 Cr 60 Cr 61 Cr 62 Cr 48 Mn 49 Mn 50 Mn 51 Mn 52 Mn 53 Mn 54 Mn 55 Mn 56 Mn 57 Mn 58 Mn 50 Fe 51 Fe 52 Fe 45

19B1 19* 17/76 48/144 56/81 94/254 150/180 117/213 79/131 9/55 10/27 6* 3* 1* 20/34 32/37 99/158 47/146 152/269 227/299 51/166 35/138 64/106 35/36 4/4 1/1 10* 1* 4* 1* 3/5 6/12 25/25 40/140 83/101 153/416 79/146 125/213 209/263 47/75 12/34 3/7 11/11 91/100

18A 19A 16C

A

Z Fe 54 Fe 55 Fe 56 Fe 57 Fe 58 Fe 59 Fe 60 Fe 61 Fe 62 Fe 67 Fe 52 Co 53 Co 54 Co 55 Co 56 Co 57 Co 58 Co 59 Co 60 Co 61 Co 62 Co 63 Co 64 Co 54 Ni 55 Ni 56 Ni 57 Ni 58 Ni 59 Ni 60 Ni 61 Ni 62 Ni 63 Ni 64 Ni 65 Ni 66 Ni 67 Ni 68 Ni 69 Ni 70 Ni 74 Ni 57 Cu 53

33 21 26 13 38 19

18 37 70 42 16 29 18

13 14 36 38 18 21

23

282 105 1213 98 322 18 153

382 32 341 124 111

406 973 281 374 175

19B1 51/76 108/235 83/183 114/271 136/180 54/184 24/77 32/49 4/6 5/14 2* 1* 2/2 26/95 119/467 102/111 105/219 152/181 20/165 138/286 94/120 12/41 49/56 16/16 2* 19/24 59/87 157/163 215/263 192/325 72/201 230/263 68/145 86/100 45/110 59/113 22/63 3/9 8/21 6/6 2/7 2* 3/8

18A 19A 16C 17 38 36 425 78 92 38 316 64 127 18 82 24

17 32 31 41 11 22

18 36 33 35 28 44 19 20 19

321 587 135 194 221 5

4 22

576 15 465 67 81 58

A

Z Cu 59 Cu 60 Cu 61 Cu 62 Cu 63 Cu 64 Cu 65 Cu 66 Cu 67 Cu 68 Cu 69 Cu 70 Cu 71 Cu 73 Cu 59 Zn 60 Zn 61 Zn 62 Zn 63 Zn 64 Zn 65 Zn 66 Zn 67 Zn 68 Zn 69 Zn 70 Zn 71 Zn 72 Zn 73 Zn 74 Zn 76 Zn 77 Zn 78 Zn 61 Ga 62 Ga 63 Ga 64 Ga 65 Ga 66 Ga 67 Ga 68 Ga 69 Ga 58

19B1 21/55 107/260 6/89 50/126 80/133 114/250 147/172 42/193 97/123 16/18 19/19 10/22 5/5 6/6 8* 8* 18/62 4/55 32/109 49/72 79/230 63/171 65/171 80/129 73/128 38/69 35/41 38/38 10/14 9* 21* 8* 1* 4* 4* 17* 15* 38/56 20/130 7/61 51/127 63/86 87/107

18A 19A 16C 359 27 18 33 9 8 16

19 31 26 29 26 32 21 16 22

592 369 291 88 197

2 2 402 22 400 504 292 167

220 12 32 15 23

156 23



12


Z Ga 71 Ga 72 Ga 73 Ga 74 Ga 75 Ga 76 Ga 77 Ga 78 Ga 79 Ga 80 Ga 61 Ge 64 Ge 65 Ge 66 Ge 67 Ge 68 Ge 69 Ge 70 Ge 71 Ge 72 Ge 73 Ge 74 Ge 75 Ge 76 Ge 77 Ge 78 Ge 79 Ge 80 Ge 81 Ge 82 Ge 65 As 66 As 67 As 68 As 69 As 70 As 71 As 70

19B1 91/97 54/79 53/110 30/30 11* 19/45 22* 34* 19* 19* 13* 5* 22* 9* 48* 34* 36/171 36/173 136/176 104/180 145/180 81/119 144/251 73/103 65/137 43/51 11/48 39* 31* 36* 6* 1* 7* 15* 42* 108* 40* 41/63

18A 19A 16C 12 109 22 15 26

33 31 65 40 58 22 66 34 24 10

22 17 85 11 10

52

A

Z As 73 As 74 As 75 As 76 As 77 As 78 As 79 As 80 As 81 As 82 As 83 As 68 Se 69 Se 70 Se 71 Se 72 Se 73 Se 74 Se 75 Se 76 Se 77 Se 78 Se 79 Se 80 Se 81 Se 82 Se 83 Se 84 Se 85 Se 86 Se 88 Se 69 Br 70 Br 71 Br 72 Br 73 Br 74 Br 72

19B1 8/66 48/144 38/77 56/118 122/156 55/98 21/32 36/37 11/22 22/43 12* 27* 20* 60* 63* 5/26 4/52 6/81 24/101 60/144 65/166 51/159 85/185 68/113 43/84 48/74 31/38 27/51 42/64 13/28 3* 1* 1* 32* 77* 77* 121* 93*

18A 19A 16C

A

Z Br 76 Br 77 Br 78 Br 79 Br 80 Br 81 Br 82 Br 83 Br 84 Br 85 Br 86 Br 87 Br 88 Br 72 Kr 73 Kr 74 Kr 75 Kr 76 Kr 77 Kr 78 Kr 79 Kr 80 Kr 81 Kr 82 Kr 83 Kr 84 Kr 85 Kr 86 Kr 87 Kr 88 Kr 89 Kr 90 Kr 91 Kr 92 Kr 93 Kr 94 Kr 75

9

36

18

23

12

10

247

21 28 27 22 18 28 76 35 11 16 14 15

16

9 17 22 58 14 15 16

19B1 4/102 2/68 41/110 51/69 36/140 60/119 27/112 23/67 38/73 2/2 9/25 8/9 8* 8* 30* 53* 80* 88* 12/58 6/66 6/97 13/98 12/49 27/101 13/71 25/77 5/69 26/76 40/63 17/169 23/73 44* 47* 20* 36* 8* 3*

18A 19A 16C 11 8 8 8 13

8

9

7

340 330 15

12 14 24 17 13 8 12 26 13 9

5 9 176 6 207 225



13

Table 1.3. Numbers of bound states in compound nuclei A Z with 37 ≤ Z ≤ 62 contained in the second part of this compilation (I/19B2). The ratio shows the number of states in Volume I/19B2 and its Supplement. Asterisks mark isotopes included in I/19C. The number of bound states in Volume LB I/18B, the number of resonances in reactions with charged particles in the compilation LB I/19A2 and the number of neutron resonances in the compilation LB I/16C are given in the same line for comparison. A

Z Rb 74 Rb 75 Rb 76 Rb 77 Rb 78 Rb 79 Rb 80 Rb 81 Rb 82 Rb 83 Rb 84 Rb 85 Rb 86 Rb 87 Rb 88 Rb 89 Rb 90 Rb 91 Rb 92 Rb 93 Rb 94 Rb 95 Rb 96 Rb 76 Sr 77 Sr 78 Sr 79 Sr 80 Sr 81 Sr 82 Sr 83 Sr 84 Sr 85 Sr 86 Sr 87 Sr 88 Sr 89 Sr 90 Sr 91 Sr 92 Sr 93 Sr 94 Sr 95 Sr 73

19B2 1* 28* 31* 77* 99* 70* 18/97 2/75 34/102 2/57 69/134 16/66 70/99 50/69 66/113 17/61 15/58 2/31 2/60 26* 55* 8* 0* 12* 1* 32* 27* 29* 3/129 2/149 8/95 14/114 5/59 39/106 56/75 139/202 152/244 110/134 80/101 2/50 26/35 4/97 3/72 57*

18B 16C

A

Z Sr 97 Sr 98 Sr 99 Sr 100 Sr 101 Sr 102 Sr 78 Y 79 Y 80 Y 81 Y 82 Y 83 Y 84 Y 85 Y 86 Y 87 Y 88 Y 89 Y 90 Y 91 Y 92 Y 93 Y 94 Y 95 Y 96 Y 97 Y 98 Y 99 Y 100 Y 101 Y 102 Y 80 Zr 81 Zr 82 Zr 83 Zr 84 Zr 85 Zr 86 Zr 87 Zr 88 Zr 89 Zr 90 Zr 91 Zr 96

5 2 12 11 18

348 99

44 28 20 17 22 35 25 10

11 75 115 443

19B2 58* 53* 43* 16* 9* 6* 1* 1* 11* 84* 114* 71* 138* 76* 38/92 22/29 78/147 36/85 70/190 135/188 45/55 15/15 17/48 9/25 6/36 5/7 24* 33* 33* 30* 34* 10* 5* 14* 55* 123* 5/85 2/29 5/113 3/62 17/81 95/132 99/273 121/157

18B 19A 16C

A

Z Zr 93 Zr 94 Zr 95 Zr 96 Zr 97 Zr 98 Zr 99 Zr 100 Zr 101 Zr 102 Zr 103 Zr 104 Zr 83 Nb 85 Nb 84 Nb 86 Nb 87 Nb 88 Nb 89 Nb 90 Nb 91 Nb 92 Nb 93 Nb 94 Nb 95 Nb 96 Nb 97 Nb 98 Nb 99 Nb 100 Nb 101 Nb 102 Nb 103 Nb 104 Nb 105 Nb 106 Nb 84 Mo 85 Mo 86 Mo 87 Mo 88 Mo 89 Mo 90 Mo 92

15 15 20 38 8

11 8 30 697

4

25 7 28 37 11

23 141

19B2 99/135 72/76 23/67 45/77 54/134 12/32 30/58 73* 48* 48* 30* 7* 4* 8* 7* 21* 79* 5/99 7/46 2/46 30/93 75/137 107/165 41/100 45/385 83/118 36/36 50/62 9/16 23/23 4/35 48* 10* 47* 9* 5* 2* 2* 18* 30* 27* 48* 5/34 18/85

18B 19A 16C 43 145 9 101 23 139 2 73 50 3 30

11 10 11

30 5 10

18

18

238 3

4



14

Table 1.3. (continued) Numbers of bound states in compound nuclei A Z with 37 ≤ Z ≤ 62 contained in the second part of this compilation (I/19B2). The ratio shows the number of states in Volume I/19B2 and its Supplement. Asterisks mark isotopes included in I/19C. The number of bound states in Volume LB I/18B, the number of resonances in reactions with charged particles in the compilation LB I/19A2 and the number of neutron resonances in the compilation LB I/16C are given in the same line for comparison. A

Z Mo 92 Mo 93 Mo 94 Mo 95 Mo 96 Mo 97 Mo 98 Mo 99 Mo 100 Mo 101 Mo 102 Mo 103 Mo 104 Mo 105 Mo 106 Mo 107 Mo 108 Mo 109 Mo 110 Mo 86 Tc 87 Tc 88 Tc 89 Tc 90 Tc 91 Tc 92 Tc 93 Tc 94 Tc 95 Tc 96 Tc 97 Tc 98 Tc 99 Tc 100 Tc 101 Tc 102 Tc 103 Tc 104 Tc 105 Tc 106 Tc 107 Tc 108 Tc 91

19B2 79/132 38/236 57/132 51/164 91/113 75/96 120/163 38/136 58/127 58/119 40/57 32/33 36* 49* 30* 64* 29* 16* 6* 5* 3* 2* 11* 52* 49* 68* 50* 58/130 10/112 88/110 5/111 45/161 69/93 51/123 28/69 17/98 7/24 22/32 19* 40* 16* 26* 27*

18B 19A 16C

A

Z Tc 110 Tc 111 Tc 88 Ru 89 Ru 90 Ru 91 Ru 92 Ru 93 Ru 94 Ru 95 Ru 96 Ru 97 Ru 98 Ru 99 Ru 100 Ru 101 Ru 102 Ru 103 Ru 104 Ru 105 Ru 106 Ru 107 Ru 108 Ru 109 Ru 110 Ru 111 Ru 112 Ru 113 Ru 92 Rh 93 Rh 94 Rh 95 Rh 96 Rh 97 Rh 98 Rh 99 Rh 100 Rh 101 Rh 102 Rh 103 Rh 104 Rh 105 Rh 109

33 14 25 15 40 29 12 30 18

77 23 57 107 75 107 159 125

240 33 58 24

9

25

6 691

19B2 20* 9* 14* 4* 13* 22* 32* 39* 41* 4/81 11/73 7/75 23/75 32/70 14/72 42/139 107/149 1/133 79/134 4/52 35/60 13/49 43* 34* 33* 24* 50* 23* 11* 19* 28* 39* 21* 48* 68* 4/43 5/77 3/42 34/79 7/61 167/189 187/187 73/127

18B 19A 16C

A

Z Rh 107 Rh 108 Rh 109 Rh 110 Rh 111 Rh 112 Rh 113 Rh 114 Rh 93 Pd 94 Pd 95 Pd 96 Pd 97 Pd 98 Pd 99 Pd 100 Pd 101 Pd 102 Pd 103 Pd 104 Pd 105 Pd 106 Pd 107 Pd 108 Pd 109 Pd 110 Pd 111 Pd 112 Pd 113 Pd 114 Pd 115 Pd 116 Pd 117 Pd 118 Pd 120 Pd 94 Ag 97 Ag 98 Ag 99 Ag 100 Ag 101 Ag 102 Ag 106

20 24 9 23 18 38 20 14 10

40 89 173 140 8 105

4

2 15

4

10 19

5 1 3

21

4

293

19B2 9/9 28/57 3/12 22/78 7* 54* 5* 58* 5* 14* 16* 36* 14* 171* 199* 3/49 4/50 16/66 4/89 39/115 80/124 36/105 62/132 83/104 35/61 112/134 20/193 33/46 6/54 51* 39* 30* 48* 13* 16* 2* 2* 12* 19* 14* 56* 77* 52*

18B 16C

6 39 21 53 11 71 38 22 44 39

4 327 319 320 133 243 232

2



15


Z Ag 104 Ag 105 Ag 106 Ag 107 Ag 108 Ag 109 Ag 110 Ag 111 Ag 112 Ag 113 Ag 114 Ag 115 Ag 116 Ag 117 Ag 118 Ag 119 Ag 120 Ag 98 Cd 100 Cd 101 Cd 102 Cd 103 Cd 104 Cd 105 Cd 106 Cd 107 Cd 108 Cd 109 Cd 110 Cd 111 Cd 112 Cd 113 Cd 114 Cd 115 Cd 116 Cd 117 Cd 118 Cd 119 Cd 120 Cd 121 Cd 122 Cd 123 Cd 124 Cd 103

19B2 96* 65* 80/147 84/117 80/141 65/168 60/85 76/76 94/123 1* 15* 4* 37* 7* 25* 14* 4* 5* 5* 28* 40* 39* 69* 90* 11/65 8/98 27/146 194/298 19/149 110/290 104/167 208/300 216/231 138/156 35/70 57/97 6/55 10/52 2/32 4/29 61* 6* 24* 20*

18B 19A 16C 2 31

19

21 35 14 4 36

11 434 4 438 11

28 58 68 11 44 62 8 40 156 45 40 9 26

65 103 157 121 443 86 48

A

Z Cd 126 Cd 128 Cd 130 Cd 100 In 101 In 102 In 103 In 104 In 105 In 106 In 107 In 108 In 109 In 110 In 111 In 112 In 113 In 114 In 115 In 116 In 117 In 118 In 119 In 120 In 121 In 122 In 123 In 124 In 125 In 126 In 127 In 128 In 129 In 130 In 131 In 132 In 102 Sn 103 Sn 104 Sn 105 Sn 106 Sn 107 Sn 108 Sn 125

19B2 1* 9* 2* 1* 1* 1* 36* 32* 46* 99* 55* 9/62 3/104 6/95 6/84 34/210 35/65 25/167 8/62 64/100 40/86 34/77 5/18 39/74 2/2 3/53 14/16 36/36 4/7 47* 7* 15* 5* 6* 4* 5* 8* 4* 4* 19* 30* 45* 25* 111*

18B 19A 16C

A

Z Sn 110 Sn 111 Sn 112 Sn 113 Sn 114 Sn 115 Sn 116 Sn 117 Sn 118 Sn 119 Sn 120 Sn 121 Sn 122 Sn 123 Sn 124 Sn 125 Sn 126 Sn 127 Sn 128 Sn 129 Sn 130 Sn 131 Sn 132 Sn 133 Sn 134 Sn 106 Sb 107 Sb 108 Sb 109 Sb 110 Sb 111 Sb 112 Sb 113 Sb 114 Sb 115 Sb 116 Sb 117 Sb 118 Sb 119 Sb 120 Sb 121 Sb 122 Sb 123 Sb 109

3 3 37 15 2 14

33 2 30 76 25 258 4

19B2 96* 44/84 73/142 30/122 66/148 42/271 80/190 185/288 138/151 124/150 127/154 111/137 130/140 80/92 81/111 173/218 63/73 50/85 26/49 2/41 31* 20* 32* 22* 5* 4* 4* 23* 59* 112* 69* 101* 43* 6/59 5/127 15/77 39/87 37/104 5/131 19/129 36/79 167/181 65/118 96/105

18B 16C

41 35 51 18 64 9 44 10 17 12 23 11 47 5 41

7 5 6

15 4 15 5 218 103 86 30 282 361 192

301



16


Z Sb 125 Sb 126 Sb 127 Sb 128 Sb 129 Sb 130 Sb 131 Sb 132 Sb 133 Sb 134 Sb 135 Sb 136 Sb 106 Te 107 Te 108 Te 109 Te 110 Te 111 Te 112 Te 113 Te 114 Te 115 Te 116 Te 117 Te 118 Te 119 Te 120 Te 121 Te 122 Te 123 Te 124 Te 125 Te 126 Te 127 Te 128 Te 129 Te 130 Te 131 Te 132 Te 133 Te 134 Te 135 Te 124

19B2 58/104 39/62 2/5 17/77 2/8 7/49 63* 51* 22* 106* 14* 25* 1* 3* 3* 27* 45* 2/50 2/48 2/46 2/19 3/105 4/81 8/84 4/75 2/95 116/173 7/67 146/212 146/161 146/210 101/153 178/307 119/137 168/253 9/96 319/323 21/85 307/317 84/97 36/36 5/25 17/48

18B 19A 16C 4 261 10 9 2

14 13 28 5 15 7 29 17 21 13 15 9 13

3

395 361 444 297 321 40 23

3

A

Z Te 137 Te 138 Te 139 Te 109 I 111 I 113 I 114 I 115 I 116 I 117 I 118 I 119 I 120 I 121 I 122 I 123 I 124 I 125 I 126 I 127 I 128 I 129 I 130 I 131 I 132 I 133 I 134 I 135 I 136 I 137 I 112 Xe 113 Xe 114 Xe 115 Xe 116 Xe 117 Xe 118 Xe 119 Xe 120 Xe 121 Xe 122 Xe 123 Xe 136

19B2 22/22 11* 6* 5* 11* 38* 124* 37* 100* 54* 157* 26* 172* 80* 27/171 3/22 79/115 4/45 133/151 3/58 58/115 205/232 32/57 29/57 7/83 2/5 2/87 2/9 1/27 2/20 5* 12* 60* 76* 7* 103* 138* 61* 104* 121* 124* 83* 2/94

18B 19A 16C

A

Z Xe 125 Xe 126 Xe 127 Xe 128 Xe 129 Xe 130 Xe 131 Xe 132 Xe 133 Xe 134 Xe 135 Xe 136 Xe 137 Xe 138 Xe 139 Xe 140 Xe 141 Xe 142 Xe 143 Xe 144 Xe 111 Cs 116 Cs 117 Cs 118 Cs 119 Cs 120 Cs 121 Cs 122 Cs 123 Cs 124 Cs 125 Cs 126 Cs 127 Cs 128 Cs 129 Cs 130 Cs 131 Cs 132 Cs 133 Cs 134 Cs 135 Cs 136 Cs 124

14 33 2 8

18 23

19

11

14

27

377 127

19B2 4/105 2/233 3/195 2/107 2/186 2/57 4/103 4/42 27/74 3/28 2/23 18/28 12/76 6/163 2/62 46* 28* 18* 21* 8* 5* 1* 1* 51* 3* 18* 69* 56* 59* 40* 108* 54* 83* 84* 53* 70* 46* 24/37 5/46 24/56 52/111 1/10 1/1

18B 19A 16C 20 4 29 16 3 24 9 10 12 71 15 17 17 43 11 6 10 6 13 1 35

14 11 12 4

324 8 6



17


Z Cs 138 Cs 139 Cs 140 Cs 141 Cs 142 Cs 143 Cs 144 Cs 120 Ba 121 Ba 122 Ba 123 Ba 124 Ba 125 Ba 126 Ba 127 Ba 128 Ba 129 Ba 130 Ba 131 Ba 132 Ba 133 Ba 134 Ba 135 Ba 136 Ba 137 Ba 138 Ba 139 Ba 140 Ba 141 Ba 142 Ba 143 Ba 144 Ba 145 Ba 146 Ba 147 Ba 148 Ba 121 La 123 La 124 La 125 La 126 La 127 La 137

19B2 12/60 28* 70* 40* 32* 44* 29* 1* 38* 60* 62* 52* 81* 64* 133* 98* 38/130 78/143 3/74 77/129 81/159 44/46 98/116 94/100 34/98 82/85 105/163 78/108 58/60 94* 37* 49* 31* 44* 42* 58* 15* 21* 79* 42* 59* 37* 107*

18B 16C 4

21 13 24 30 9 20 8 21 14 30 17

41 17 6 90 156 189 81 148

A

Z La 129 La 130 La 131 La 132 La 133 La 134 La 135 La 136 La 137 La 138 La 139 La 140 La 141 La 142 La 143 La 144 La 145 La 146 La 147 La 148 La 124 Ce 125 Ce 126 Ce 127 Ce 128 Ce 129 Ce 130 Ce 131 Ce 132 Ce 133 Ce 134 Ce 135 Ce 136 Ce 137 Ce 138 Ce 139 Ce 140 Ce 141 Ce 142 Ce 143 Ce 144 Ce 145 Ce 128

19B2 90* 74* 107* 120* 28* 4/141 4/63 4/77 13/87 5/61 38/62 94/94 218/233 32* 23* 46* 25* 33* 48* 50* 25* 7* 19* 62* 44* 122* 93* 151* 121* 159* 129* 9/83 3/70 44/96 4/79 46/78 47/52 165/180 88/88 68/104 38/76 3/61 8/42

18B 19A 16C

A

Z Ce 147 Ce 148 Ce 149 Ce 150 Ce 151 Ce 152 Ce 126 Pr 128 Pr 129 Pr 130 Pr 131 Pr 132 Pr 133 Pr 134 Pr 135 Pr 136 Pr 137 Pr 138 Pr 139 Pr 140 Pr 141 Pr 142 Pr 143 Pr 144 Pr 145 Pr 146 Pr 147 Pr 148 Pr 149 Pr 150 Pr 128 Nd 129 Nd 130 Nd 131 Nd 132 Nd 133 Nd 134 Nd 135 Nd 136 Nd 137 Nd 138 Nd 139 Nd 146

5 5 8 13

8

11

16

11 173

15 12 10 19 10 52 23 14 11

14 198 6 76

19B2 18B 19A 16C 118* 32* 49* 40* 4* 13* 8* 46* 47* 23* 152* 30* 144* 170* 75* 104* 105* 93* 69* 8/69 37/37 22/111 31 18 166/170 258 9/29 6 8 4/4 5 6/24 8* 36* 16* 20* 1* 41* 17* 52* 155* 89* 173* 86* 85* 174* 144* 104* 49*



18


Z Nd 141 Nd 142 Nd 143 Nd 144 Nd 145 Nd 146 Nd 147 Nd 148 Nd 149 Nd 150 Nd 151 Nd 152 Nd 153 Nd 154 Nd 156 Nd 133 Pm 134 Pm 135 Pm 136 Pm 137 Pm 138 Pm 139 Pm 140

19B2 58/74 82/88 156/246 146/252 187/202 123/139 280/291 138/138 26/113 82/82 32/133 21/95 14/53 17* 24* 9* 67* 50* 32* 103* 38* 60* 70*

A

18B 16C 18 41 71 18 41 146 23 22

Z Pm 141 Pm 142 Pm 143 Pm 144 Pm 145 Pm 146 Pm 147 Pm 148 Pm 149 Pm 151 Pm 152 Pm 153 Pm 154 Pm 155 Pm 132 Sm 133 Sm 134 Sm 135 Sm 136 Sm 137 Sm 138 Sm 139 Sm 140

85 150 90 210 93 12 123

72 79

19B2 63* 92* 2/79 52/90 39/84 37/53 5/78 62/65 4/43 37/73 57/131 4/14 39/70 28* 36* 8* 65* 6* 50* 79* 41* 82* 106*

A

18B 19A 16C

Z Sm 141 Sm 142 Sm 143 Sm 144 Sm 145 Sm 146 Sm 147 Sm 148 Sm 149 Sm 150 Sm 151 Sm 152 Sm 153 Sm 154 Sm 155 Sm 156 Sm 157 Sm 158 Sm 159 Sm 160 Sm 140

18

8

21

4

7 2 24

4 42 1 2

19B2 71* 83* 23/98 56/89 98/183 42/169 100/190 27/99 132/289 115/193 88/191 63/240 47/152 272/296 14/110 100/141 9/38 17* 11* 1* 7*

18B 19A 16C

34 35 64 22 49 31 47 19 46

206

213 25 160 25 121 92

47 36

Properties of nuclear excitations and binding energies have a general origin. The interconnection between values of nuclear excitations and nuclear binding energies was pointed out by I. Arima and A. Bohr [90Ar0A, 68Bo0A]. In Table 2 the standard parameters of the residual nucleon interaction εN,2N derived from the differences of valence nucleon separation energies (for nuclei differing by two additional nucleons of another type) are compared with excitations of near-magic nuclei (Z = 50 + 2, Z = 82 + 2). The stable character of E ∗ in Z = 84 isotopes was noticed [95Be31, 90Ma14]. Table 2. Comparison of E ∗ (keV) in near-magic nuclei with Z = 84 (and N = 90 top part of the Table) and in tellurium isotopes (Z = 52) with the parameters of the residual interaction of valence nucleons εN,2N = 682 keV (Z = 51, Z = 83, N = 83 [96Su0A, 97SuZX]), n = E ∗ /εN,2N . A

200

Z

π

π

2J ,J E∗ εN,2N A

Z

π

π

2J ,J E∗, nεN,2N

Po

+

202

Po

+

204

Po

+

206

Po

+

208

Po

+

208

Po

+

211

Po +

Te

125

Nd +

119

Sm +

113

Gd +

116

Dy

+

2 2 665.9 677.3 682 682

2 2 2 4 684.3 700.7 686.5 1347 682 682 682 1364

11 687.2 682

0 0 675.4 684.7 682 682

0 680.7 682

0 675.6 682

116

116

121

122

126

127

Te

+

116

Te

+

Te

+

117

Te

+

121

Te

+

121

Te

+

+

+

2 4 6 7 1 7 3 ,5 678.9 1359.4 2002.2 681.5 681.3 683.1 1364.0 682 1364 2044 682 682 682 1364

Te

+

122

Te

+

Te

+

Te

+

0 4 4 7 1357.4 2042.0 1361.4 685.02 1364 2044 1364 682



1.2

19

List of notations

Table 3. List of principal notations in Volume I/19B3. No. Symbol 1

REFERENCE Its meaning

Explanation

PROPERTIES OF COMPOUND NUCLEUS Z A Abundance J π , 2J π , J T T1/2

2

Atomic number Atomic weight Abundance Spin of the state Isotopic spin Half-life

Integer number Z Integer number A Percentage of isotope abundance π indicates parity Tg.s =|N − Z|/2 [04Nu0A]

PARAMETERS OF EXCITED STATES E∗ X, Y, Z, U... ∗ Eanal Ef∗ Γcm , Γ Γn , Γp , Γd , Γα

3

Excitation energy Additional energy Excitation energy Final energy Γcm = M/(M + m) Γ Nucleon width

Total excitation energy Additional unknown energy E ∗ of the analog state Energy of the final state Width in center-of-mass frame Width of capture/emission

TRANSFER REACTIONS (α,p); σ(α,p); Ip (α,n); σ(α,n); In (α,d); σ(α,d); Id (α,t); σ(α,t); It (α,3 He); σ(α,τ ); Iτ (α,2 He); σ(α,2 He) (3 He,d); σ(τ ,d); Id (3 He,n); σ(τ ,n); In (3 He,p); σ(τ ,p); Ip (t,p); σ(t,p); Ip (t,d); σ(t,d); Id (d,n); σ(d,n); In (d,p); σ(d,p); Ndp (16 O,14 N); σ(16 O,14 N) (16 O,15 N); σ(16 O,15 N) (12 C,10 Be); σ(12 C,10 Be) (12 C,α); σ(12 C,α) (6 Li,d); σ(6 Li,d) (7 Li,p); σ(7 Li,p) (7 Li,t); σ(7 Li,t) 6 (7 Li,6 He); σ(7 Li,6 He); I He

Three-nucleon transfer Three-nucleon transfer Two-neutron transfer Proton transfer One-neutron transfer Two-neutron transfer Proton transfer Two-nucleon transfer Two-nucleon transfer Two-neutron transfer One-neutron transfer One-proton transfer One-neutron transfer Two-nucleon transfer One-proton transfer Two-proton transfer α transfer He transfer α transfer One-proton transfer 6

Cross section, proton yield Cross section, neutron yield Cross section, deuteron yield Cross section, tritium yield Cross section, yield of 3 He Cross section of (α,2 He) reaction Cross section, deuteron yield Cross section, neutron yield Cross section, proton yield Cross section, proton yield Cross section, deuteron yield Deuteron stripping, yield Deuteron stripping, yield All differential cross sections dσ/dΩ are given in [µbarn/sr] All integral cross sections σ are given in [µbarn] or [mbarn] Sα – spectroscopic factor Cross section of 6 He transfer Cross section, yield of 6 He



20

Table 3. (continued) List of principal notations in Volume I/19B3. No.


Symbol 4

Explanation

TRANSFER PICKUP REACTIONS ETC. (d,τ ); σ(d,τ ); Iτ ; Idτ (e,e p); σ(e,e p) (p,t); σ(p,t); It (p,d); σ(p,d); Id (d,t); σ(d,t) (p,α); σ(p,α) (d,α); σ(d,α) (t,α); σ(t,α) (τ, α); σ(τ, α); Iτ α (p,τ ); σ(p,τ ) (d,6 Li); σ(d,6 Li) (t,6 Li); σ(t,6 Li) (τ ,6 He); σ(τ ,6 He) Ip , In , Iα (τ ,t); σ(τ ,t); (t,τ ) (p,p ); σ(p,p ) (d,d ); σ(d,d ) (α, α ); σ(α, α ) 2 γp2 ; γα2 ; γα2 /γW β, βL , βL R

5

One-proton pickup One-proton pickup Two-neutron pickup One-neutron pickup One-neutron pickup Three-nucleon pickup Two-nucleon pickup One-proton pickup One-neutron pickup Two-nucleon pickup α pickup

Cross section, 3 He yield Cross section Cross section, tritium yield Cross section, deuteron yield Cross section Cross section Cross section Cross section Cross section, α yield Cross section Sα – spectroscopic factor

Three-neutron pickup Particle yield Charge-exchange Inelastic scattering Inelastic scattering Inelastic scattering Reduced widths β-parameters

(3 He,6 He) reaction Proton–, neutron–, α–yield Charge-exchange reactions (t,τ ), (τ ,t) Inelastic scattering of protons Inelastic scattering of deuterons Inelastic scattering of α-particles Widths of resonances, see LB I/19A Deformation parameters, βL R in [fm] calculated with the parameter r◦

SPECTROSCOPIC FACTORS 2

S, SN , C S C2 Sp+ , S + Sp− , S − Sn+ , S + Sn− , S − S; C 2S S ; C 2 S SGlj l, lp , ln , l1 + l2 ,... Sdp , Ndp , Sdn Spd , Sdt , Sτ α Spt , Sdτ , Spτ , Sαtγ dσ/dΩ ε

Spectr. factor Clebsch-Gordon factor Spectr. factor Spectr. factor Spectr. factor Spectr. factor Spectr. factor Spectr. factor Spectr. factor Orbital moments S factor, yield Spectr. factor Spectr. factors Experimental yield Enhancement factor

N

Norm. parameter

Factors of stripping or pick-up reaction Isospin factor, see LB Vol. I/18A, p. 2-5 Single proton transfer reaction (d,n),... Single proton pick-up reaction (d,τ ),... Single neutron transfer reaction (d,p),... Single neutron pick-up reaction (p,d),... (2J + 1)S; (2J + 1)C 2 S (2J + 1)/(2I + 1)S, I is the initial spin (2J + 1)/(2I + 1)C 2 S; other factors See definitions of S in the works S of deuteron stripping reaction (yield) Sn− of neutron pick-up reaction S of the different transfer reactions Yield of transfer reaction [µbarn/sr] Parameter which shows the goodness of the fit of a few-nucleon transfer Theoretically calculated overlap of the wave-functions of interacting particles in a transfer, see original work



21

Table 3. (continued) List of principal notations in Volume I/19B3. No. Symbol 6


Explanation

PROPERTIES OF GAMMA TRANSITIONS Eγ Iγ Br; BR M ult. E1, E2, E3 M1, M2, M3 Ef∗ , Jf , Jfπ Is,0 , Is Γγ◦ ,Γγf , Γγ Γγ /ΓW Γ◦ 2 /Γ , gΓ◦ 2 /Γ Γ◦red , gΓ◦red B(M1), B(GT), ... EWSR ωγ , Spγ , σ, σγ Γα Γγ /Γ , Γp Γα /Γ Eγ1 +Eγ2

7

Energy of γ-quanta Relative intensity of γ Branching ratio Multipolarity Multipolarity Multipolarity Excitation, spin Cross section in [eVbarn] Total radiative width Γγ in Wigner units Observed quantity Reduced radiative width Transition intensity γ-transition strength Radiative strength

Normalized at 100 for the strongest one Percentage of the relative intensity [%] In units [e2 fm4 ], [e2 fm2 ], [10−3 e2 fm2 ] In units of µ2N etc. Excitation energy and spin of final state In NRF In NRF See LB Vol. I/18 In NRF (in units [eV] or [meV]) In units [meV/MeV3 ]=[meV ] See LB Vol. I/18 Energy Weighted Sum Rule (in [%]) See LB Vol. I/19A Strength of (α, γ) or (p, α) reactions Sum energy of γ cascade

OTHER PARAMETERS Ay

VAP parameter

T20 E◦ , E◦cm σpγ , σnγ nlj L, ln , lp , l j, 2j, 2jp , 2jn rel., arb.u. eval., theor.

Tensor parameter Eαcm , Epcm Cross sections Quantum numbers Quantum number Quantum number

Vector Analyzing Power of the nucleon transfer (σ+ -σ− )/(σ+ +σ− ) Parameter of nucleon transfer Resonance energy in lab. or cm. frame Radiative cross sections Quantum numbers of a certain state Orbital momentum Momentum of the transferred nucleon Relative, arbitrary units Evaluated, theoretical values

The abbreviation Br is used for the branching ratios of transitions from the neutron capturing state. This column is located, together with the spectroscopic factors, before the branching ratios of all other states. Due to the limited space many parameters are only given in the Supplement. The abundance of stable isotopes [05TuZX] is given as Comments. Doublets and triplets are marked ”doublt” and ”triplt”. For parameters in the tables, a quantity enclosed in angular brackets ... indicates that it is preferred by the authors of the original work, a quantity enclosed in square brackets [...] is guessed by the compilers. In all tables the mark ”include” means that the value given in the line above the marked one belongs to two states. As in many other compilations we give values 2J π and 2T for all A-odd nuclei ( 2J = 1+ instead of J = 1/2+ , etc.). Double spin notation 1− ,3− or 3+ ,5+ is widely used. Alternative values (A,B ...) of the parameter are given as A,B ... while a mixture of parameters for one state are given as A+B ... Notations presented in Table 3 are common for the data in all four Volumes I/19BC.



1.3

22

Data presentation

The data in Vol. LB I/19B3 are presented in tables whose format is analogous to that of the compilation of energy levels of light nuclei by P. Endt [98En04]. In these tables each horizontal line belongs to one excited state. The line starts with such standard parameters as energy of excitation E ∗ , spin J π and isospin T . Each date-line in the Volumes I/19B contains also the halflife T1/2 of the state or its total width Γcm . Spectroscopic information on different nuclear transfer reactions together with one (main) reference in NSR-code forms the central part of each data-line. The notations of the parameters given in CRF are listed in Table 3. They are the same as those used in original works, review papers and compilation LB I/18. The general properties of nuclei are presented in two sections (Nos. 1-2) of Table 3. Data on the charged particle reactions: yields and cross sections (dσ/dΩ, σ, etc., see Nos. 3-4 of Table 3) and spectroscopic factors (SN , see No. 5) derived from the experimental data on cross sections of transfer reactions are given after E ∗ and are followed by the main reference. Direct referencing to the original papers in each data-line could be used by the interested reader for his own judgment. At the bottom of each column with the experimental data we give again the corresponding reference (seen only in Supplement). Additional references given at the end of the Tables and references in comments could serve for a better orientation in the material. Data taken from papers not included in the Nuclear Science Reference system are provided by reference which is shown as NSR reference with zero and a letter in the last two (out of 6) characters. Each data-line contains at the end branching ratios (in percents) of γ-transitions to the levels situated below this excited state. In cases when there are many transitions from a certain initial state the corresponding horizontal line has a continuation in the Supplement (CD) where branching ratios of all known transitions are given. For each isotope, data-lines for states are ordered by increasing E ∗ and form one isotope-table which ends by reference-codes and by short comments where additional information can be found. Each isotope-table is labelled by the atomic number (Z) and the atomic weight (A) of the nucleus. The whole set of isotope-tables for a given element (Z) is ordered by the increasing atomic weights (A) of the compound nucleus and forms the unit of the total file mentioned in the list of Contents. Ordered by Z these files for all the elements make up the total file CRF with references presented at the end of each book. Additional references given after the Tables and references in comments serve for better orientation in the material. As in many other compilations we give values 2J π and 2T for all A-odd nuclei ( 2J = 1+ instead of J = 1/2+ , etc.). Double spin notation 1− ,3− or 3+ ,5+ is widely used. Data from the great number of transfer reactions used for obtaining information on properties of excited states are grouped in the following way. Transfer reactions with the stripping of the ongoing particle are given first. The sequence of data for these reactions starts with many-nucleon transfer and ends with one-nucleon transfer like the well-known deuteron stripping reaction. Data from pickup reactions are given in the inverse order – one-nucleon transfer first, manynucleon pickup reaction at the end. Such a method of data presentation (used also in NDS) permits a more effective comparison of results for one-nucleon transfer reactions (stripping and pickup) obtained by the use of different projectiles. For example, data on one-neutron transfer reactions (α,3 He), (t,d) and (d,p) can be compared between themselves as well as with data on one-neutron pickup transfer reactions (p,d), (d,t) and (τ, α). Spectroscopic factors together with occupation probabilities and magnetic moments are basic elements needed for the understanding of nuclear structure. The spectroscopic factor S is defined as the probability to reach a final single-particle (hole) state when a nucleon is added to (or removed from) the target nucleus (correspondingly Sp+ , Sn+ or Sp− , Sn− ). The mean field approximation is a basic idea of nuclear shell-models used for description of nuclear states. The occupation number is the number of nucleons in the certain quantum state in the target nucleus, relative to the 2j + 1 limit. The commonly used method of data analysis consists in the comparison with results of Landolt-B¨ ornstein New Series I/19B3


23

calculations by Distorted Waives Born Approximation (DWBA) (see references in I/19B1). The measured cross section σexp and nucleon transfer reaction spectroscopic factor SN are connected with the theoretically estimated cross section σDWBA by the relation: σexp =(2J + 1)(2I + 1)−1 (2j + 1)−1 × SN × N × σDWBA with N – normalization parameter, J, I, j – total moments of the final state, the target nuclei and the transferred nucleon, respectively. The measured cross section σexp of few-nucleon transfer reaction is connected with the estimated cross section σDWBA by the relation which includes the spectroscopic ”enhancement factor” ε: σexp =(2J + 1)(2I + 1)−1 (2j + 1)−1 × ε × N × σDWBA . The final goal of the comparison consists in a judgement on the validity of single-particle approximation of the shell-model. It was found after many experimental works that in near-magic nuclei this model gives good results. It permits to determine the single-particle properties of the real excited states. The closeness of their spectroscopic factors to shell-model values is in accordance with the observed closeness of magnetic moments of near-magic nuclei to the single-particle limit. Data from inelastic scattering of different particles and data obtained by NRF – Nuclear Resonance Fluorescence method – can be found at the end of the data-line or between transfer reaction data. In some cases we use Wigner units 1W.u.(M1) = 1.79µ2N and 1W.u.(E1) = 1.28e2 fm2 . In Table 3 different reactions are given in the same order as they appear in data-lines of LB Vol. I/19B3.

1.4

Interpretation of data of nuclear excitations

The general description of the spectroscopic information for nuclear bound states is given in the Introduction to Vol. I/18 written by V. Soloviev and coauthors. V. Soloviev also studied the structure of deformed nuclei [97So21] and transition from order in low-lying levels to quantum chaos. References for these works can be found in Vols. I/18ABC [01Sc0A, 02Sc0A, 03Sc0A]. The shell model as a unified view of nuclear structure and the role of dynamical symmetries in nuclear collective models are discussed in works by A. Arima, F. Iachello, R. Jolos and others [97Jo06]. Now it is known as IBA – Interacting Boson Approximation [85Ca13, 85Ca19, 85Ca29, 85Ca33] and references in Vol. I/19B2. New results in the study of high-spin excitations and many examples of the application of IBA can be found in Proceedings of International Conferences on Nuclear Structure held in Berkeley (2001), Lund (2000) and Goeteborg (2004). Numbers of rotational bands evaluated in PNPI are given in Table 4. The information concerning the low-lying rotational-band energies in rare-earth A-odd nuclei was analyzed in [76Bo0A]. The application of nuclear physics to many practical tasks including astrophysics demands knowledge of properties of nuclear states in the whole energy region of nuclear excitations. Besides the statistical approach based on N. Bohr’s hypothesis about the chaotic motion of the nucleons in nuclei, the study of the role of symmetries in the description of the properties of nuclear levels is the commonly used method of general data interpretation. For obtaining parameters of many excited states different experimental methods are used and we include in this compilation accurate data obtained by the Nuclear Resonance Fluorescence method by P. von Brentano and co-workers [90Zi05, 92Zi02, 96Kn0A, 98Fr01] (see also references in Vols. I/19B1 and I/19B2). A great number of data on heavy nuclei were obtained in measurements of γγ cascades after thermal neutron capture performed in JINR by A. Sukhovoy and co-workers [97Kh0A, 99BoZR, 99BoZT,01Kh0A]. Neutron strength function, population of superdeformed bands and some other related topics were discussed in [74Ba26, 83Ci01, 90Sc31, 93Ba35, 00Gi05, 02Mi16, 04Ga03].



24

Table 4. Number of rotational bands in nuclei with Z = 63 − 100 evaluated in PNPI Nuclear Data Center [03AlZX] (see corresponding tables in I/19B1 and I/19B2). A

Z

149

Eu Gd 157 Gd 153 Tb 143 Dy 163 Dy 159 Ho 155 Er 167 Er 161 Tm 175 Tm 167 Yb 161 Lu 173 Lu 165 Hf 177 Hf 167 Ta 179 Ta 171 W 183 W 177 Re 171 Os 183 Os 173 Ir 187 Ir 175 Pt 187 Pt 185 Au 183 Hg 197 Hg 195 Tl 195 Pb 217 Fr 223 Ra 227 Ac 233 Th 235 U 237 Pu 241 Am 249 Cm 247 Cf 139

N 7 3 6 6 7 10 5 3 12 5 3 7 2 7 6 7 4 11 5 6 4 6 5 3 5 1 2 5 3 2 2 4 2 6 6 5 15 6 3 4 3

A

Z 137 Eu 151 Eu 141 Gd 159 Gd 155 Tb 153 Dy 165 Dy 161 Ho 157 Er 169 Er 163 Tm 153 Yb 169 Yb 163 Lu 175 Lu 167 Hf 179 Hf 169 Ta 181 Ta 173 W 185 W 179 Re 173 Os 185 Os 175 Ir 189 Ir 177 Pt 191 Pt 187 Au 185 Hg 199 Hg 197 Tl 197 Pb 219 Fr 225 Ra 229 Ac 229 Pa 237 U 239 Pu 243 Am 241 Bk 249 Cf

N 1 8 6 10 5 7 7 8 5 8 5 1 9 3 7 7 9 1 2 3 6 7 3 5 4 4 3 2 5 4 2 2 2 2 3 1 1 6 9 4 1 6

A

Z 139 Eu 153 Eu 149 Gd 161 Gd 157 Tb 155 Dy 167 Dy 163 Ho 159 Er 171 Er 165 Tm 159 Yb 171 Yb 165 Lu 177 Lu 169 Hf 181 Hf 171 Ta 185 Ta 175 W 187 W 181 Re 175 Os 187 Os 179 Ir 191 Ir 179 Pt 193 Pt 191 Au 187 Hg 187 Tl 199 Tl 199 Pb 225 Fr 227 Ra 223 Th 231 Pa 239 U 241 Pu 245 Am 243 Bk 251 Cf

N 5 5 8 7 8 9 1 11 6 5 6 3 10 7 6 3 2 5 1 3 2 3 3 5 6 6 3 3 3 3 5 1 1 1 3 2 5 9 4 3 1 6

A

Z 141 Eu 155 Eu 151 Gd 143 Tb 159 Tb 157 Dy 151 Ho 165 Ho 161 Er 153 Tm 169 Tm 161 Yb 173 Yb 167 Lu 179 Lu 171 Hf

N 5 8 5 6 6 8 2 11 5 2 5 5 5 7 3 8

A

Z 143 Eu 157 Eu 153 Gd 149 Tb 161 Tb 159 Dy 155 Ho 167 Ho 163 Er 157 Tm 171 Tm 163 Yb 175 Yb 169 Lu 157 Hf 173 Hf

N 3 4 10 5 6 9 6 3 14 4 5 4 7 5 4 8

A

Z Eu 159 Eu 155 Gd 151 Tb 163 Tb 161 Dy 157 Ho 169 Ho 165 Er 159 Tm 173 Tm 165 Yb 177 Yb 171 Lu 163 Hf 175 Hf

N 1 4 12 2 5 12 4 2 7 4 2 4 4 10 3 7

173

5 4 2 5 5 3 2 4 5 5 4 4 8 3 1 1 3 3 1 1 4 7 2 5 2

175

4 4 18 4 3 8 1 2 3 5 6 1 11 5 1 11 3 3 5 1 6 2 7 5 1

177

Ta W 181 W 175 Re 187 Re 181 Os 171 Ir 185 Ir 171 Pt 185 Pt 183 Au 181 Hg 195 Hg 193 Tl 193 Pb

6 3 8 6 2 6 6 4 1 7 4 3 8 6 7

221

1 4 9 6 7 2 4 1 2

Ta W 177 W 171 Re 183 Re 177 Os 189 Os 181 Ir 193 Ir 181 Pt 195 Pt 193 Au 191 Hg 189 Tl 201 Tl 199 Po 217 Ra 219 Ac 225 Th 233 Pa 235 Np 243 Pu 243 Cm 247 Bk 253 Cf 165

Ta W 179 W 173 Re 185 Re 179 Os 191 Os 183 Ir 195 Ir 183 Pt 181 Au 195 Au 193 Hg 191 Tl 187 Pb 201 Bi 219 Ra 223 Ac 229 Th 235 Pa 237 Np 245 Pu 245 Cm 249 Bk 251 Fm 167

147

169

Ra Ac 231 Th 233 U 239 Np 239 Am 247 Cm 251 Bk 253 Es 225

The stable character of several few-nucleon excitation shown in Table 2 can be considered as the ”tuning effect” in nuclear data seen simultaneously in the stable character of differences of nuclear binding energies. Standard parameters of the residual interactions εn2p = ∆Sn (∆Z = 2) and εn2n = ∆Sn (∆N = 2) have distributions with maxima at 680keV = εN,2N and at 340keV = εN,2N /2 Landolt-B¨ ornstein New Series I/19B3


25

corresponding to the linear trends in valence nucleon separation energies [97SuZX]. For nuclei situated after lead the stability of εnp = 340 keV was noticed in [90Mo11]. In the same nuclei the stable character of excitation shown in Table 2 persists in other neighbour nuclei (Table 5). Table 5. Comparison of E ∗ (keV) in heavy nuclei (Z = 84−90) with the parameter of the residual interaction εN,2N = 682 keV (closeness of stable excitation to εN,2N , continuation of Table 2). A

203

Z

π

π

2J ,J E∗ εN,2N

Po

−

207

Po

+

5 5 686.5 685.8 682 682

205

At −

13 664.3 646

206

At

+

9 686 682

207

At

−

5 674 682

207

At −

13 686 682

211

At

−

(7 ) 674.1 682

214

Rn

+

216

Ra

+

2 2 694.7 688.2 682 682

218

Th

+

2 689.6 682

Parameters of the residual interaction of valence nucleons can be estimated from excitations in nuclei with three neutrons above the double-magic core. In case of Z = N = 28 and Z = N = 50 cores the values E ∗ = 340 keV in 59 Ni and E ∗ = 168.0(1) keV are rational to the stable parameters of the residual interaction of valence neutrons determined from differences of binding energies [01Su0A, 01So01, 03So0B, 03Su0B]. The observation of the stable character of intervals between excited states in neighbour nuclei is another method to check this ”tuning effect” of low-energy excitations. Data in LB I/19BC can be used for this purpose. For example, stable interval in the sum distribution of spacings in 125 Te and 127 Te (Dij = 1360 keV) corresponds to the two-phonon excitation in the neighbour 126 Te with E ∗ = 2εN,2N (see Table 2). Collected information on the properties of excited states of all nuclei permits a study of few-nucleon effects of very general origin [06Su0A, 05Su0A, 01So0A].

1.5

Conclusions

This file (Vol. LB I/19B3) has a complimentary character to compilations of data on low-lying levels of the selected number of heavy nuclei presented in I/18C [03Sc0A]. Together with Vols. I/19B1, I/19B2, I/19C and compilations of parameters of resonances in reactions with neutrons and charged particles it gives almost all information about all known excited states of all nuclei.

1.6

Acknowledgments

This project much benefitted from the existence of international computer Nuclear Science References file maintained in NNDC (Brookhaven National Laboratory, USA). We are grateful to the PNPI scientific library staff headed by Irina Spiridonova. Programs for data handling and text preparation were developed by D. Sukhoruchkin.


R1

References 68Bo0A

Bohr, A.: Proc. Int. Symp. Nucl. Struct., Dubna, 1968. IAEA, p. 179.

74Ba26

Back, B.B., Bang, J., Bjornholm, S., Hattula, J., Kleinheinz, P., Lien, J.R.: Nucl. Phys. A 222 (1974) 377.

76Bo0A

Boisson, J.P., Piepenbring, R., Ogle, W.: Phys. Rep. 26, No.3 (1976) 999.

83Ci01

Cizewski, J.A., Burke, D.G., Flynn, E.R., Brown, R.E., Sunier, J.W.: Phys. Rev. C 27 (1983) 1040.

85Ca13

Casten, R.F.: Phys. Lett. B 152 (1985) 145.

85Ca19

Casten, R.F.: Phys. Rev. Lett. 54 (1985) 1991.

85Ca29

Casten, R.F.: Nucl. Phys. A 443 (1985) 1.

85Ca33

Casten, R.F., Frank, W., Von Brentano, P.: Nucl. Phys. A 444 (1985) 133.

90Ar0A

Arima, A.: Nucl. Phys. A 507 (1990) 305c.

90Ma14

Maj, A., Grawe, H., Kluge, H., Kuhnert, A., Maier, K.H., Recht, J., Roy, N., Hubel, H., Guttormsen, M.: Nucl. Phys. A 509 (1990) 413.

90Mo11

Mouze, G., Ythier, C.: Nuovo Cim. A 103 (1990) 105.

90Sc31

Schiffer, K., Herskind, B.: Nucl. Phys. A 520 (1990) 521c.

90Zi05

Zilges, A., Von Brentano, P., Richter, A., Heil, R.D., Kneissl, U., Pitz, H.H., Wesselborg, C.: Phys. Rev. C 42 (1990) 1945.

92Zi02

Zilges, A., Von Brentano, P., Richter, A.: Z. Phys. A 341 (1992) 489.

93Ba35

Baktash, C., Winchell, D.F., Garrett, J.D., Smith, A.: Nucl. Phys. A 557 (1993) 145c.

95Be31

Bernstein, L.A., Cizewski, J.A., Jin, H.-Q., Younes, W., Henry, R.G., Farris, L.P., Charos, A., Carpenter, M.P., Janssens, R.V.F., Khoo, T.L., Lauritsen, T., Bearden, I.G., Ye, D., Becker, J.A., Henry, E.A., Brinkman, M.J., Hughes, J.R., Kuhnert, A., Wang, T.F., Stoyer, M.A., Diamond, R.M., Stephens, F.S., Deleplanque, M.A., Macchiavelli, A.O., Lee, I.Y., Cederwall, B., Oliveira, J.R.B., Burde, J., Fallon, P., Duyar, C., Draper, J.E., Rubel, E., Vo, D.T.: Phys. Rev. C 52 (1995) 621.

96Kn0A

Kneissl, U., Pitz, H.H., Zilges, A.: Progr. Part. Nucl. Phys. vol. 37 (1996) 349.

96Su0A

Sukhoruchkin, S.I.: Proc. 4th Int. Seminar on Interact. Neutr. Nucl. ISINN-4, Dubna, 1996. JINR -E3-96-336 p. 82.

97Jo06

Jolos, R.V., Von Brentano, P., Pietralla, N., Schneider, I.: Nucl. Phys. A 618 (1997) 126.

97Kh0A

Khitrov, V.A., Sukhovoj, A.M., Voinov, A.V., Vasilieva, E.V.: Proc. 9th Int. Symp. on Capture Gamma-Ray Spectroscopy and Related Topics, Budapest, Hungary, 1996. Eds.: Molnar, G.L., Belgya, T., Revay, Zs. Vol. 1, p. 436. Springer, 1997.

97So21

Soloviev, V.G., Sushkov, A.V., Shirikova, N.Y.: Z. Phys. A 358 (1997) 117.

97SuZX

Sukhoruchkin, S.I.: Proc. 9th Int. Symp. on Capture Gamma-Ray Spectroscopy and Related Topics, Budapest, Hungary, 1996. Eds: Molnar, G.L., Belgya, T., Revay, Zs. Vol. 1 p. 358. Springer, 1997.

98En04

Endt, P.M.: Nucl. Phys. A 633 (1998) 1.

Landolt-Börnstein New Series I/19B3

References

R2

98Fr01

Fransen, C., Beck, O., Von Brentano, P., Eckert, T., Herzberg, R.-D., Kneissl, U., Maser, H., Nord, A., Pietralla, N., Pitz, H.H., Zilges, A.: Phys. Rev. C 57 (1998) 129.

98Sc0A

Schopper, H. (Ed.): Landolt Börnstein New Series, vol. I/16B. Springer, 1998. ISBN 3540-63277-8.

99BoZR

Bondarenko, V.A., Honzatko, J., Khitrov, V.A., Sukhovoj, A.M., Tomandl, I.: Proc. 7th Int. Seminar on Interact. Neutr. Nucl. ISINN-7, Dubna, 1999. JINR -E3--98--212 p. 187.

99BoZT

Bondarenko, V.A., Honzatko, J., Khitrov, V.A., Sukhovoj, A.M., Tomandl, I.: Rep. JINR-E3-99-343 (1999).

00Gi05

Gillitzer, A., Gilg, H., Hayano, R.S., Hirenzaki, S., Itahashi, K., Iwasaki, M., Kienle, P., Munch, M., Munzenberg, G., Schott, W., Suzuki, K., Tomono, D., Weick, H., Yamazaki, T., Yoneyama, T., and the GSI-S160 Collaboration: Nucl. Phys. A 663-664 (2000) 206c.

01Kh0A

Khitrov, V.A., Sukhovoj, A.M., Georgiev, E.P. Proc. 9th Int. Seminar on Interact. Neutr. Nucl. ISINN--9, Dubna, 2001. JINR E3--2001--192 p. 173.

01Sc0A

Schopper, H. (Ed.): Landolt Börnstein New Series, vol. I/18A. Springer, 2001.

01So01

Soroko, Z.N., Sukhoruchkin, S.I., Sukhoruchkin, D.S.: Nucl. Phys. A 680 (2001) 254c.

01So0A

Soroko, Z.N., Sukhoruchkin, S.I., Sukhoruchkin, D.S.: Proc. 9th Int. Seminar on Interact. Neutr. Nucl. ISINN--9, Dubna, 2001. JINR E3--2001--192 p. 334.

01Su0A

Sukhoruchkin, S.I.: Proc. 9th Int. Seminar on Interact. Neutr. Nucl. ISINN--9, Dubna, 2001. JINR E3--2001--192 p. 342.

02Mi16

Misicu, S., Bastrukov, S.I.: Eur. Phys. J. A 13, 399 (2002).

02Sc0A

Schopper, H. (Ed.): Landolt Börnstein New Series, vol. I/18B. Springer, 2001.

03AlZX

Alenicheva, T.V., Kabina, L.P., Mitropolsky, I.A., Tyukavina, T.M.: in: Atlas of Rotational Bands in Odd-A Nuclei, PNPI, Gatchina (2003).

03Sc0A

Schopper, H. (Ed.): Landolt Börnstein New Series, vol. I/18C. Springer, 2001.

03So0B

Soroko, Z.N., Sukhoruchkin, S.I., Sukhoruchkin, D.S.: Proc. 9th Int. Seminar on Interact. Neutr. Nucl. ISINN--10, Dubna, 2001. JINR E3--2003--10 p. 289.

03Su0B

Sukhoruchkin, S.I.: Proc. 9th Int. Seminar on Interact. Neutr. Nucl. ISINN--10, Dubna, 2001. JINR E3--2003--10 p. 299.

04BrZU

Brusegan, A., Corvi, F., Rullhusen, P., Soroko, Z.N., Sukhoruchkin, S.I., Weigmann, H.: in: Landolt Börnstein New Series, vol. I/16C; Schopper, H. (Ed.). Springer, 2004. ISBN 3-540-42828-3.

04Ga03

Ganev, H., Garistov, V.P., Georgieva, A.I.: Phys. Rev. C 69 (2004) 014305.

04Nu0A

Nucl. Data Sheets, current issues (2004); http://www.sciencedirect.com.

04Sc0B

Schopper, H. (Ed.): Landolt Börnstein New Series, vol. I/19A1. Springer, 2004.

05Sc0A

Schopper, H. (Ed.): Landolt Börnstein New Series, vol. I/19A2. Springer, 2005.

05Su0A

Sukhoruchkin, S.I.: Proc. 8th Int. Conf. on Low Energy Antiproton Physics, Bonn, Germany, 2005. AIP Conf. Proc. 796, p. 221.

05TuZX

Tuli, J.K.: Nuclear Wallet Cards (7th ed.). BNL., N.-Y, 2005.

06Su0A

Sukhoruchkin, S.I.: Nucl. Phys. A (in press).


Nuclear States from Charged Particle Reactions – Tables of Excitations from Reactions with Charged Particles. Vol. I/19B1: 3-Lithium ... 36-Krypton Vol. I/19B2: 37-Rubidium ... 62-Samarium Vol. I/19B3: 63-Rubidium ... 99-Einsteinium 63-Europium Eu-145 Eu-146 Eu-147 Eu-148 Eu-149 Eu-150 Eu-151 Eu-152 Eu-153 Eu-154 Eu-155 Eu-156 Eu-157 Eu-159 Eu-160

65-Terbium Tb-149 Tb-150 Tb-151 Tb-152 Tb-153 Tb-154 Tb-155 Tb-156 Tb-157 Tb-158 Tb-159 Tb-160 Tb-161 Tb-162 Tb-163

64-Gadolinium Gd-146 Gd-147 Gd-148 Gd-149 Gd-150 Gd-151 Gd-152 Gd-153 Gd-154 Gd-155 Gd-156 Gd-157 Gd-158 Gd-159 Gd-160 Gd-161 Gd-162

66-Dysprosium Dy-154 Dy-155 Dy-156 Dy-157 Dy-158 Dy-159 Dy-160 Dy-161 Dy-162 Dy-163 Dy-164 Dy-165 Dy-166


67-Holmium Ho-157 Ho-158 Ho-159 Ho-160 Ho-161 Ho-162 Ho-163 Ho-164 Ho-165 Ho-166 Ho-167 Ho-168 Ho-169 Ho-170 68-Erbium Er-161 Er-162 Er-163 Er-164 Er-165 Er-166 Er-167 Er-168 Er-169 Er-170 Er-171 Er-172 69-Thulium Tm-165 Tm-166 Tm-167 Tm-168 Tm-169 Tm-170 Tm-171 Tm-172 Tm-173 Tm-174 Tm-175

70-Ytterbium Yb-166 Yb-167 Yb-168 Yb-169 Yb-170 Yb-171 Yb-172 Yb-173 Yb-174 Yb-175 Yb-176 Yb-177 Yb-178 71-Lutetium Lu-171 Lu-172 Lu-173 Lu-174 Lu-175 Lu-176 Lu-177 Lu-178 Lu-179 Lu-180 72-Hafnium Hf-173 Hf-174 Hf-175 Hf-176 Hf-177 Hf-178 Hf-179 Hf-180 Hf-181 Hf-182 Hf-183

Index of nuclides 73-Tantalum Ta-179 Ta-180 Ta-181 Ta-182 Ta-183 Ta-184 Ta-185 74-Tungsten W-178 W-179 W-180 W-181 W-182 W-183 W-184 W-185 W-186 W-187 W-188 75-Rhenium Re-181 Re-182 Re-183 Re-184 Re-185 Re-186 Re-187 Re-188 Re-189 Re-190 Re-191 76-Osmium Os-184 Os-185 Os-186 Os-187 Os-188 Os-189 Os-190 Os-191 Os-192 Os-193 Os-194


77-Iridium Ir-183 Ir-184 Ir-185 Ir-186 Ir-187 Ir-188 Ir-189 Ir-190 Ir-191 Ir-192 Ir-193 Ir-194 Ir-195 78-Platinum Pt-180 Pt-181 Pt-182 Pt-183 Pt-184 Pt-185 Pt-186 Pt-187 Pt-188 Pt-189 Pt-190 Pt-191 Pt-192 Pt-193 Pt-194 Pt-195 Pt-196 Pt-197 Pt-198 Pt-199 Pt-200 79-Gold Au-186 Au-187 Au-188 Au-189 Au-190 Au-191 Au-192 Au-193 Au-194 Au-195 Au-196 Au-197 Au-198 Au-199

80-Mercury Hg-184 Hg-185 Hg-186 Hg-187 Hg-188 Hg-189 Hg-190 Hg-191 Hg-192 Hg-193 Hg-194 Hg-195 Hg-196 Hg-197 Hg-198 Hg-199 Hg-200 Hg-201 Hg-202 Hg-203 Hg-204 Hg-205 Hg-206 81-Thallium Tl-195 Tl-196 Tl-197 Tl-198 Tl-199 Tl-200 Tl-201 Tl-202 Tl-203 Tl-204 Tl-205 Tl-206 Tl-207 Tl-208 Tl-209

82-Lead Pb-196 Pb-197 Pb-198 Pb-199 Pb-200 Pb-201 Pb-202 Pb-203 Pb-204 Pb-205 Pb-206 Pb-207 Pb-208 Pb-209 Pb-210 Pb-211 Pb-212 Pb-213 Pb-214 83-Bismuth Bi-201 Bi-202 Bi-203 Bi-204 Bi-205 Bi-206 Bi-207 Bi-208 Bi-209 Bi-210 Bi-211 Bi-212 Bi-213 Bi-214 Bi-215

Index of nuclides 84-Polonium Po-196 Po-197 Po-198 Po-199 Po-200 Po-201 Po-202 Po-203 Po-204 Po-205 Po-206 Po-207 Po-208 Po-209 Po-210 Po-211 Po-212 Po-213 Po-214 Po-215 Po-216 85-Astatine At-203 At-204 At-205 At-206 At-207 At-208 At-209 86-Radon Rn-208 Rn-209 Rn-210 Rn-211 Rn-212 Rn-213 Rn-214 Rn-215 Rn-216 Rn-217 Rn-218 Rn-219 Rn-220 Rn-222


87-Francium Fr-213 Fr-214 Fr-215 Fr-216 Fr-217 Fr-218 Fr-219 Fr-220 Fr-221 Fr-222 Fr-223 Fr-225 88-Radium Ra-212 Ra-213 Ra-214 Ra-215 Ra-216 Ra-217 Ra-218 Ra-219 Ra-220 Ra-221 Ra-222 Ra-223 Ra-224 Ra-225 Ra-226 Ra-227 Ra-228 89-Actinium Ac-219 Ac-220 Ac-221 Ac-222 Ac-223 Ac-224 Ac-225 Ac-226 Ac-227 Ac-228 Ac-229 Ac-230 Ac-231 Ac-232

90-Thorium Th-217 Th-218 Th-220 Th-221 Th-222 Th-223 Th-224 Th-225 Th-226 Th-227 Th-228 Th-229 Th-230 Th-231 Th-232 Th-233 Th-234 91-Protactinium Pa-229 Pa-230 Pa-231 Pa-232 Pa-233 Pa-234 Pa-235 Pa-236 Pa-237 92-Uranium U-230 U-231 U-232 U-233 U-234 U-235 U-236 U-237 U-238 U-239 U-240 93-Neptunium Np-233 Np-234 Np-235 Np-236 Np-237 Np-238 Np-239 Np-240 Np-242

94-Plutonium Pu-235 Pu-236 Pu-237 Pu-238 Pu-239 Pu-240 Pu-241 Pu-242 Pu-243 Pu-244 Pu-245 Pu-246 95-Americium Am-239 Am-240 Am-241 Am-242 Am-243 Am-244 Am-245 96-Curium Cm-242 Cm-243 Cm-244 Cm-245 Cm-246 Cm-247 Cm-248 Cm-249 Cm-250 97-Berkelium Bk-247 Bk-248 Bk-249 Bk-250 Bk-251 98-Californium Cf-246 Cf-247 Cf-248 Cf-249 Cf-250 Cf-251 Cf-252 Cf-253 99-Einsteinium Es-251 Es-252 Es-253 Es-254


1

145 63 Eu

Energy levels and branching ratios [93Pe07]. E∗

2J π

L

C 2S

[keV]

(α,t)

0.0 5+ 2 4 329.92(7) 7+ 5 716.0(3) 11− 808.33(5) 1+ 2 1041.71(6) 3+ 1368 9− 1459.7(1) 1500 7− 1567.12(7) 3− ,5− 1600.26(6) 3− 1601.2(4) 11− 1745 7− ,5− 4+2 1758.0(1) 3+ 1761.32(8) 3− 1765.8(1) 5− 1792 11− 1828.5(4) 9− 1844.6(4) 13− 1845.32(9) 5+ 1880.62(5) 3+ ,1+ 1915.5(2) 3+ + + 2027.8(1) 1 ,3 2042.9(1) 1+ ,3+ 2048.8(1) 3+ 2054.1(1) 2079.1(1) 2114.3(1) 3+ − 2117 9 ,11− 2149.6(1) 2188.4(1) 2195 9+ 2203.4(1) 3+ + 2237 9 ,7+ 2244.4(5) 15+ 2284.1(4) 15− 2295 11+ 2314 13− 2318.68(8) 5+ 2321.72(7) 3+ 2327.3(6) 2349.0(1) 2352 11,13− 2400 13+ 2402.25(9) 2416.8(1)

0.37 0.24 0.98 0.74

L Sτ d

Sτ d

L C 2S (7 Li,6 He)

mod. stand 2 4 5 0 2

0.33 0.17 0.82 0.98 1.01

0.33 0.22 0.72 1.05

2 4 5 0 2

0.19(3) 0.12(3) 0.45(7) 0.60(9) 0.66(9)

0.02 incl 0.1+0.2 2 0.02

Ref.

85Ga01 85Ga01 85Ga01

Branching ratios in percentage 329.9 716 808 1042 Ef∗ : 0.0 2Jfπ : 5+ 7+ 11− 1+ 3+

85Ga01

100 22(1) 100 100

70Ne04

77(8) x 100 100

85Ga01

x 98(6)

78(5)

x 23(3)

x

100 2 0.014(6)

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