The Confined beta-Soft rotor model in rare-earth nuclei
Pith reviewed 2026-06-30 11:31 UTC · model grok-4.3
The pith
The confined beta-soft rotor model reproduces ground-state energies, B(E2) rates, and beta-band excitations in even-even rare-earth nuclei where the R4/2 ratio lies between 2.904 and 3.333.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The confined beta-soft rotor model bridges the X(5) critical point symmetry and the rigid rotor limit for nuclei where the ratio of the first 4+ to 2+ state energies lies between 2.904 and 3.333. When applied to rare-earth nuclei, it yields calculated ground-state band energies, B(E2) values, and beta-band excitations that agree with available data and allow predictions for unmeasured observables.
What carries the argument
The Confined beta-Soft (CBS) rotor model, which parametrizes beta-vibration confinement to interpolate between the X(5) critical point and the rigid rotor.
If this is right
- Systematic comparison shows agreement between CBS predictions and experimental ground-state band energies and B(E2) rates.
- Beta-band excitations are calculated and can be compared to data where available.
- Predictions are provided for nuclear observables that have not yet been measured.
- The results offer guidance for future experimental investigations in the rare-earth region.
Where Pith is reading between the lines
- The model may serve as a quick classifier for nuclei in the transitional deformation window without full microscopic calculations.
- Significant mismatches with new data could indicate where gamma degrees of freedom or other effects need inclusion.
- The predictions supply concrete targets that experiments can use to test the model's range of validity.
Load-bearing premise
The confined beta-soft rotor model remains an accurate description for rare-earth nuclei whose R4/2 ratio lies between 2.904 and 3.333.
What would settle it
An experimental measurement of the 4+ energy level or a B(E2) transition strength in a rare-earth nucleus with R4/2 in the stated range that deviates substantially from the CBS calculation.
read the original abstract
Contemporary theoretical descriptions of nuclear structure rely mainly on microscopic, single-particle frameworks often in competition with collective degrees of freedom, especially when deformation plays a dominant role. Such phenomena are prominent in the rare-earth region, where rotational band structures and enhanced electric quadrupole transitions are systematically examined. The Confined beta-Soft (CBS) rotor model, introduced by N. Pietralla and O.M. Gorbachenko, bridges the gap between the X(5) critical point and the rigid-rotor limit in the region where the R_4/2 = E(4+)/E(2+) ratio lies between 2.904 and 3.333. In the present work, the CBS framework is employed to calculate ground-state band energies, associated B(E2) transition rates, and beta-band excitations of even-even nuclei in the rare-earth region. The theoretical results are systematically compared with available experimental data, and predictions are provided for nuclear observables that have not yet been measured, offering guidance for future experimental investigations.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript applies the pre-existing Confined beta-Soft (CBS) rotor model (Pietralla and Gorbachenko) to even-even rare-earth nuclei with 2.904 < R_{4/2} < 3.333. It computes ground-state band energies, B(E2) transition rates, and beta-band excitations, performs systematic comparisons to experimental data, and supplies predictions for unmeasured observables.
Significance. If the data comparisons hold, the work supplies a systematic test of the CBS framework across the X(5)-to-rigid-rotor interval in a deformation-dominated region. The emphasis on collective observables and the provision of falsifiable predictions for future experiments constitute clear strengths for nuclear-structure phenomenology.
minor comments (2)
- [Abstract] Abstract: the applicability window is stated as lying between 2.904 and 3.333; clarify whether the bounds are inclusive and list the specific nuclei (or at least the count) examined so readers can immediately gauge the scope of the comparison.
- The manuscript should explicitly state whether any CBS parameters are adjusted to the present data set or whether all calculations use the original, fixed CBS values; this directly affects the interpretation of the agreement with experiment.
Simulated Author's Rebuttal
We thank the referee for the positive evaluation of our manuscript and the recommendation for minor revision. The report correctly summarizes the scope of the work as a systematic application of the CBS rotor model to even-even rare-earth nuclei in the specified R_{4/2} range, with comparisons to data and predictions for unmeasured observables. No specific major comments were raised in the report.
Circularity Check
No significant circularity: application of pre-existing external model
full rationale
The paper applies the Confined beta-Soft (CBS) rotor model, introduced by Pietralla and Gorbachenko (distinct authors), to compute ground-state band energies, B(E2) rates, and beta-band excitations for selected rare-earth nuclei within the stated R_{4/2} window. It then performs direct comparisons to experimental data and offers predictions for unmeasured observables. No equations or steps in the provided text reduce the central results to self-defined quantities, fitted inputs renamed as predictions, or load-bearing self-citations; the model framework and its applicability range are imported from prior independent work, and the comparisons serve as external tests rather than internal re-derivations.
Axiom & Free-Parameter Ledger
Reference graph
Works this paper leans on
-
[1]
I. Hamamoto, B. Mottelson, Shape deformations in atomic nuclei, Scholarpedia 7 (2012) 10693. doi:10.4249/scholarpedia.10693
-
[2]
Litvinova, Recent advancements in the strongly coupled many-body problem, arXiv (2025)
E. Litvinova, Recent advancements in the strongly coupled many-body problem, arXiv (2025). doi:10.48550/arXiv.2512.23644
-
[3]
Hergert, A guided tour ofab initionuclear many-body theory, fphy 8 (2020) 379
H. Hergert, A guided tour ofab initionuclear many-body theory, fphy 8 (2020) 379. doi:10. 3389/fphy.2020.00379
-
[4]
A. Ekström, C. Forssén, T. Papenbrock, et al., What isab initioin nuclear theory?, fphy 11 (2023) 1129094. doi:10.3389/fphy.2023.1129094
-
[5]
Iachello, Dynamic symmetries at the critical point, Phys
F. Iachello, Dynamic symmetries at the critical point, Phys. Rev. Lett. 85 (2000) 3580–3583. doi:10.1103/PhysRevLett.85.3580
-
[6]
F. Iachello, Analytic description of critical point nuclei in a spherical-axially deformed shape phase transition, Phys. Rev. Lett. 87 (2001) 052502. doi:10.1103/PhysRevLett.87.052502
-
[7]
P. Cejnar, J. Jolie, R. F. Casten, Quantum phase transitions in the shapes of atomic nuclei, Rev. Mod. Phys. 82 (2010) 2155–2212. doi:10.1103/RevModPhys.82.2155
-
[8]
N. Pietralla, O. M. Gorbachenko, Evolution of the “βexcitation” in axially symmetric transitional nuclei, Phys. Rev. C 70 (2004, 011304). doi:10.1103/PhysRevC.70.011304
-
[9]
Reese, CBS model program,https://sourceforge.net/projects/cbsmodel/, 2011
M. Reese, CBS model program,https://sourceforge.net/projects/cbsmodel/, 2011
2011
-
[10]
P. E. Garrett, Characterization of theβvibration and0 + 2 states in deformed nuclei, Journal of Physics G: Nuclear and Particle Physics 27 (2001) R1–R29. URL:https://doi.org/10.1088/ 0954-3899/27/1/201. doi:10.1088/0954-3899/27/1/201
-
[11]
J. Sharpey-Schafer, R. Bark, S. Bvumbi, E. Lawrie, J. Lawrie, T. Madiba, S. Majola, A. Minkova, S. Mullins, P. Papka, D. Roux, J. Timár, A double vacuum, configuration dependent pairing and lack ofβ-vibrations in transitional nuclei: Band structure of N = 88 to N = 91 nuclei, Nu- clear Physics A 834 (2010) 45c–49c. URL:https://www.sciencedirect.com/scienc...
-
[12]
Sharpey-Schafer, R
J. Sharpey-Schafer, R. Bark, S. Bvumbi, T. Dinoko, S. Majola, “stiff” deformed nuclei, configu- ration dependent pairing and theβandγdegrees of freedom, The European Physical Journal A 55 (2019) 15
2019
-
[13]
A. Aprahamian, K. Lee, S. R. Lesher and R. Bijker, The nature of 0+ excitations in deformed nuclei, Progress in Particle and Nuclear Physics 143 (2025, 104173). doi:10.1016/j.ppnp.2025. 104173
-
[14]
K. Dusling, N. Pietralla, Description of ground-state band energies in well-deformed even-even nu- clei with the confinedβ-soft rotor model, Phys. Rev. C 72 (2005) 011303. doi:10.1103/PhysRevC. 72.011303
-
[15]
Bohr, The Coupling of Nuclear Surface Oscillations to the Motion of Individual Nucleons, Det Kgl
A. Bohr, The Coupling of Nuclear Surface Oscillations to the Motion of Individual Nucleons, Det Kgl. Danske Videnskabernes Selskab. Matematisk-fysiske meddelelser, Komm. Munksgaard, 1952. URL:https://books.google.gr/books?id=A8QTtQEACAAJ
1952
-
[16]
A. Bohr, B. R. Mottelson, Nuclear Structure, World Scientific, New York, 1997
1997
-
[17]
A. Bohr, B. Mottelson, Nuclear Structure, Volume II: Nuclear Deformations, W.A. Benjamin, 1975
1975
-
[18]
Solutions of the Bohr hamiltonian, a compendium
L. Fortunato, Solutions of the Bohr Hamiltonian, a compendium, Eur. Phys. J. A 26S1 (2005) 1–30. doi:10.1140/epjad/i2005-07-115-8.arXiv:nucl-th/0411087
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1140/epjad/i2005-07-115-8.arxiv:nucl-th/0411087 2005
-
[19]
D. Bonatsos, P. E. Georgoudis, D. Lenis, N. Minkov, C. Quesne, Bohr hamiltonian with a deformation-dependent mass term for the davidson potential, Phys. Rev. C 83 (2011). doi:10.1103/physrevc.83.044321
-
[20]
P. Buganu, L. Fortunato, Recent approaches to quadrupole collectivity: models, solutions and applications based on the Bohr hamiltonian, Journal of Physics G: Nuclear and Particle Physics 43 (2016) 093003. URL:https://doi.org/10.1088/0954-3899/43/9/093003. doi:10. 1088/0954-3899/43/9/093003
-
[21]
J. A. Papadopoulos, T. J. Mertzimekis, P. Koseoglou, D. Bonatsos, P. Vasileiou, M. Efstathiou, Investigation of the Yb and W Isotopic Chains using the Confinedβ-Soft Rotor Model, HNPS Adv. Nucl. Phys. 32 (2026) 107–112. doi:10.12681/hnpsanp.8764. 17
-
[22]
D. Kocheva, K. A. Gladnishki, A. Blazhev, et al., Lifetimes and electromagnetic transition strengths in Er, Eur. Phys. J. A 62 (2026) 18. doi:10.1140/epja/s10050-025-01778-0
-
[23]
NUDAT, National Nuclear Data Center, online.https://www.nndc.bnl.gov/nudat3/
-
[24]
S. Basu, A. Sonzogni, Nuclear Data Sheets forA=150, Nucl. Data Sheets 114 (2013) 435–660. doi:10.1016/j.nds.2013.04.001
-
[25]
Martin, Nuclear Data Sheets forA=152, Nucl
M. Martin, Nuclear Data Sheets forA=152, Nucl. Data Sheets 114 (2013) p. 1497–1847. doi:10. 1016/j.nds.2013.11.001
2013
-
[26]
Nica, Nuclear Data Sheets for A=154, Nuclear Data Sheets 200 (2025) 2–524
N. Nica, Nuclear Data Sheets for A=154, Nuclear Data Sheets 200 (2025) 2–524. doi:https: //doi.org/10.1016/j.nds.2025.02.002
-
[27]
H. Iimura, J. Katakura, S. Ohya, Nuclear data sheets for A = 126, Nucl. Data Sheets 180 (2022) 1–413. doi:https://doi.org/10.1016/j.nds.2022.02.001
-
[28]
Z. Elekes, J. Timar, Nuclear data sheets for A = 128, Nuclear Data Sheets 129 (2015) 191–436. doi:https://doi.org/10.1016/j.nds.2015.09.002
-
[29]
Reich, Nuclear Data Sheets forA=156, Nucl
C. Reich, Nuclear Data Sheets forA=156, Nucl. Data Sheets 113 (2012) 2537–2840. doi:10.1016/ j.nds.2012.10.003
2012
-
[33]
Singh, J
B. Singh, J. Chen, Nuclear Data Sheets forA=164, Nucl. Data Sheets 147 (2018). doi:10.1016/ j.nds.2018.01.001
2018
-
[34]
C. M. Baglin, Nuclear Data Sheets forA=166, Nucl. Data Sheets 109 (2008) 1103–1382. doi:10. 1016/j.nds.2008.04.001
2008
-
[35]
C. M. Baglin, Nuclear Data Sheets forA=168, Nucl. Data Sheets 111 (2010) 1807 – 2080. doi:10.1016/j.nds.2010.07.001
-
[36]
C. Baglin, E. McCutchan, S. Basunia, E. Browne, Nuclear Data Sheets forA=170, Nucl. Data Sheets 153 (2018) 1–494. doi:10.1016/j.nds.2018.11.001. 18
-
[37]
Singh, Nuclear Data Sheets forA=172, Nucl
B. Singh, Nuclear Data Sheets forA=172, Nucl. Data Sheets 75 (1995) 199 – 376. doi:10.1006/ ndsh.1995.1025
-
[38]
Basunia, Nuclear Data Sheets forA=176, Nucl
M. Basunia, Nuclear Data Sheets forA=176, Nucl. Data Sheets 107 (2006) p. 791–1026. doi:10. 1016/j.nds.2006.03.001
2006
-
[39]
E. Achterberg, O. A. Capurro, G. V. Marti, Nuclear Data Sheets forA=178, Nucl. Data Sheets 110 (2009) 1473 – 1688. doi:10.1016/j.nds.2009.05.002
-
[40]
E. A. McCutchan, Nuclear Data Sheets forA=180, Nucl. Data Sheets 126 (2015) 151 – 372. doi:10.1016/j.nds.2015.05.002
-
[41]
Comput- ers and Education: Artificial Intelligence 6, 100234
B. Singh, Nuclear Data Sheets forA=182, Nucl. Data Sheets 130 (2015) 21–126. doi:10.1016/j. nds.2015.11.002
work page doi:10.1016/j 2015
-
[42]
C. M. Baglin, Nuclear Data Sheets forA=184, Nucl. Data Sheets 111 (2010) 275–523. doi:10. 1016/j.nds.2010.01.001
2010
-
[43]
J. Batchelder, A. Hurst, M. Basunia, Nuclear Data Sheets forA=186, Nucl. Data Sheets 183 (2022) 1–346. doi:10.1016/j.nds.2022.06.001
-
[44]
F. Kondev, S. Juutinen, D. Hartley, Nuclear Data Sheets forA=188, Nucl. Data Sheets 150 (2018) 1–364. doi:10.1016/j.nds.2018.05.001
-
[45]
Singh, J
B. Singh, J. Chen, Nuclear Data Sheets forA=190, Nucl. Data Sheets 169 (2020) 1–390. doi:10. 1016/j.nds.2020.10.001
2020
-
[46]
B. Pritychenko, M. Birch, B. Singh, M. Horoi, Tables of E2 transition probabilities from the first 2+ states in even–even nuclei, At. Data Nucl. Data Tables 107 (2016) 1–139. doi:10.1016/j.adt. 2015.10.001
-
[47]
C. W. Reich, Nuclear Data Sheets forA=154, Nucl. Data Sheets 110 (2009) 2257–2532. doi:10. 1016/j.nds.2009.09.001
2009
-
[48]
R. L. Canavan, M. Rudigier, P. H. Regan, M. Lebois, J. N. Wilson, N. Jovancevic, P.-A. Söderström, S. M. Collins, D. Thisse, J. Benito, S. Bottoni, M. Brunet, N. Cieplicka-Oryńczak, S. Courtin, D. T. Doherty, L. M. Fraile, K. Hadyńska-Klęk, G. Häfner, M. Heine, L. W. Iskra, V. Karayonchev, A. Kennington, P. Koseoglou, G. Lotay, G. Lorusso, M. Nakhostin, C...
-
[49]
Petkov, A
P. Petkov, A. Dewald, O. Möller, I. Deloncle, R. Chapman, S. Pascu, D. Bucurescu, D. Tonev, M. Reese, C. Fransen, S. Araddad, G. Asova, J. Copnell, N. Goutev, M. Hackstein, J. Jolie, J. Lisle, J. Mo, T. Pissulla, W. Rother, A. Smith, C. Tenereiro, D. Thompson, K. Zell, On the quadrupole collectivity in the yrast band of168Yb, Nucl. Phys. A 957 (2017) 240–...
2017
-
[50]
V. Karayonchev, J.-M. Régis, J. Jolie, A. Blazhev, R. Altenkirch, S. Ansari, M. Dannhoff, F. Diel, A. Esmaylzadeh, C. Fransen, R.-B. Gerst, K. Moschner, C. Müller-Gatermann, N. Saed-Samii, S. Stegemann, N. Warr, K. O. Zell, Evolution of collectivity in then= 100isotones near170Yb, Phys. Rev. C 95 (2017) 034316. doi:10.1103/PhysRevC.95.034316
-
[51]
M. Rudigier, K. Nomura, M. Dannhoff, R.-B. Gerst, J. Jolie, N. Saed-Samii, S. Stegemann, J.- M. Régis, L. M. Robledo, R. Rodríguez-Guzmán, A. Blazhev, C. Fransen, N. Warr, K. O. Zell, Evolution of E2 transition strength in deformed hafnium isotopes from new measurements on 172Hf, 174Hf, and 176Hf, Phys. Rev. C 91 (2015) 044301. doi:10.1103/PhysRevC.91.044301
-
[52]
J. Wiederhold, V. Werner, R. Kern, N. Pietralla, D. Bucurescu, R. Carroll, N. Cooper, T. Daniel, D. Filipescu, N. Florea, R.-B. Gerst, D. Ghita, L. Gurgi, J. Jolie, R. S. Ilieva, R. Lica, N. Marginean, R. Marginean, C. Mihai, I. O. Mitu, F. Naqvi, C. Nita, M. Rudigier, S. Stege- mann, S. Pascu, P. H. Regan, Evolution of E2 strength in the rare-earth isoto...
-
[53]
A. Harter, L. Knafla, G. Frießner, G. Häfner, J. Jolie, A. Blazhev, A. Dewald, F. Dunkel, A. Esmaylzadeh, C. Fransen, V. Karayonchev, K. Lawless, M. Ley, J.-M. Régis, K. O. Zell, Lifetime measurements in the tungsten isotopes176,178,180W, Phys. Rev. C 106 (2022) 024326. doi:10.1103/PhysRevC.106.024326
-
[54]
A. Harter, A. Esmaylzadeh, L. Knafla, C. Fransen, F. v. Spee, J. Jolie, M. Ley, V. Karayonchev, J. Fischer, A. Pfeil, Lifetime measurements in low yrast states and spectroscopic peculiarities in 182Os, Phys. Rev. C 108 (2023) 024305. doi:10.1103/PhysRevC.108.024305
-
[55]
A. Costin, M. Reese, H. Ai, R. F. Casten, K. Dusling, C. R. Fitzpatrick, G. Gürdal, A. Heinz, E. A. McCutchan, D. A. Meyer, O. Möller, P. Petkov, N. Pietralla, J. Qian, G. Rainovski, V. Werner, Centrifugal stretching along the ground state band of168Hf, Phys. Rev. C 79 (2009) 024307. doi:10.1103/PhysRevC.79.024307. 20
-
[56]
F. Stephens, R. Simon, Coriolis effects in the yrast states, Nucl. Phys. A 183 (1972) 257–284. doi:10.1016/0375-9474(72)90658-6
-
[57]
R. Wyss, M. A. Riley, Fifty years of backbending, Nucl. Phys. News 32 (2022) 16–20. doi:10. 1080/10619127.2022.2063000.arXiv:10.1080/10619127.2022.2063000
-
[58]
P. Ring, P. Schuck, The Nuclear Many-Body Problems, volume 103, Springer, 1980. doi:10.1063/ 1.2915762
1980
-
[59]
F. S. Stephens, R. S. Simon, Properties of rotational bands in heavy nuclei, Nucl. Phys. A 183 (1972) 257–270. doi:10.1016/0375-9474(72)90619-4
-
[60]
F. S. Stephens, Phenomena associated with the rotational alignment of nucleons, Rev. Mod. Phys. 47 (1975) 43–65. doi:10.1103/RevModPhys.47.43
-
[61]
R. Bengtsson, S. Frauendorf, Rotational bands and particle alignment, Nucl. Phys. A 327 (1979) 139–160. doi:10.1016/0375-9474(79)90509-8
-
[62]
P. Koseoglou, V. Werner, N. Pietralla, D. Bonatsos, N=90 QSPT: Cerium, neodymium and samarium isotopic chains in the IBM symmetry triangle, HNPS Adv. Nucl. Phys. 26 (2019) 37–43. doi:10.12681/hnps.1793
-
[63]
P. Koseoglou, V. Werner, N. Pietralla, S. Ilieva, T. Nikšić, D. Vretenar, P. Alexa, M. Thürauf, C. Bernards, A. Blanc, A. M. Bruce, R. B. Cakirli, N. Cooper, L. M. Fraile, G. de France, M. Jentschel, J. Jolie, U. Köster, W. Korten, T. Kröll, S. Lalkovski, H. Mach, N. Mărginean, P. Mutti, Z. Patel, V. Paziy, Z. Podolyák, P. H. Regan, J.-M. Régis, O. J. Rob...
-
[64]
P. Koseoglou, V. Werner, N. Pietralla, N = 90 shape phase transition: increasing axial asymmetry towards 148Ce, Bulg. J. Phys. 49 (2022) p. 89–96. doi:10.55318/bgjp.2022.49.1.089
-
[65]
Koseoglou, et al., 2026
P. Koseoglou, et al., 2026. (in preparation)
2026
-
[66]
R. F. Casten, Possible unified interpretation of heavy nuclei, Physical Review Letters 54 (1985) 1991–1994. doi:10.1103/PhysRevLett.54.1991
-
[67]
D. H. Feng, C.-L. Wu, M. W. Guidry, Z.-P. Li, Dynamical Pauli effects and the saturation of nuclear collectivity, Phys. Lett. B 205 (1988) 156–162. doi:10.1016/0370-2693(88)91639-5. 21
-
[68]
P. Koseoglou, T. J. Mertzimekis, M. Efstathiou, P. Vasileiou, H. Mayr, C. M. Nickel, N. Pietralla, V. Werner, A. Blazhev, A. Esmaylzadeh, J. Fischer, C. Fransen, J. Jolie, M. Ley, A. Pfeil, F. von Spee, K. Gladnishki, D. Kocheva, G. Rainovski, N. Florea, A. Radu, D. Tofan, D. Bonatsos, K. E. Karakatsanis, Gamma-spectrometry on the well-deformed 178Yb: exc...
-
[69]
Zyriliou, et al., Nuclear Structure Investigations in Yb isotopes, HNPS Adv
A. Zyriliou, et al., Nuclear Structure Investigations in Yb isotopes, HNPS Adv. Nucl. Phys. 28 (2022) 104–108. doi:10.12681/hnps.3609
-
[70]
J. Gupta, V. Katoch, Review of nuclear structure N=86–118 of W isotopes, Nucl. Phys. A 1057 (2025, 123032). doi:10.1016/j.nuclphysa.2025.123032
-
[71]
M. A. Caprio, Structure of collective modes in transitional and deformed nuclei, arXiv: Nuclear Experiment (2005). URL:https://api.semanticscholar.org/CorpusID:119368092
2005
-
[72]
J. B. Gupta, J. H. Hamilton, Outstanding problems in the band structures of152Sm, Phys. Rev. C 96 (2017) 034321. doi:10.1103/PhysRevC.96.034321
-
[73]
Balabanski et al., Evidence for x(5) critical point symmetry in128Ce, International Journal of Modern Physics E 15 (2012). doi:10.1142/S0218301306005538
-
[74]
D. Tonev, A. Dewald, T. Klug, P. Petkov, J. Jolie, A. Fitzler, O. Möller, S. Heinze, P. von Brentano, R. F. Casten, Transition probabilities in154Gd: Evidence for X(5) critical point sym- metry, Phys. Rev. C 69 (2004) 034334. doi:10.1103/PhysRevC.69.034334
-
[75]
E. Mccutchan, N. Zamfir, M. Caprio, R. Casten, H. Amro, C. Beausang, D. Brenner, A. Hecht, C. Hutter, S. Langdown, D. Meyer, P. Regan, J. Ressler, A. Yamamoto, Low spin states in162Y b and the X(5) critical point symmetry, Phys. Rev. C 69 (2004). doi:10.1103/PhysRevC.69.024308
-
[76]
E. Browne, H. Junde, Nuclear Data Sheets forA=174, Nucl. Data Sheets 87 (1999) 15 – 176. doi:10.1006/ndsh.1999.0015. 22 Figures Fig. 2: Evolution of the CBS parameterrβ along the even–even isotopic chains of Ce-Os elements as a function of neutron number N. The bold gray point at178Yb(N= 108) represents the valuer β = 0.509, obtained from the CBS calculat...
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