Ab initio calculations of beta-decay half-lives for N=50 neutron-rich nuclei
Pith reviewed 2026-05-18 18:05 UTC · model grok-4.3
The pith
Ab initio calculations show that including two-body currents increases beta-decay half-lives for N=50 neutron-rich nuclei and brings predictions into agreement with experimental data.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Starting from nuclear forces and currents based on chiral effective field theory, we use the in-medium similarity renormalization group to consistently derive valence-space Hamiltonians and weak operators, from which we calculate the nuclear states involved and the Gamow-Teller transition strengths, without phenomenological adjustments. In addition, we explore effects of first-forbidden contributions. Our results show that the inclusion of two-body currents increases the total half-lives, which then show good agreement with the existing experimental data, thereby validating the predictive capability of our approach.
What carries the argument
In-medium similarity renormalization group (IMSRG) used to derive consistent valence-space Hamiltonians and weak operators, including two-body currents, from chiral effective field theory.
If this is right
- The half-lives supply improved inputs for r-process nucleosynthesis models in regions lacking experimental data.
- First-forbidden contributions can be included systematically within the same ab initio framework for other neutron-rich nuclei.
- The method supports reliable predictions for total decay rates once two-body currents are retained.
- The consistent derivation of operators and Hamiltonians can be extended to additional isotopic chains near shell closures.
Where Pith is reading between the lines
- The same framework could be used to compute beta-delayed neutron emission probabilities that also affect r-process yields.
- Testing the approach on nuclei with neutron numbers farther from 50 would check how well the currents remain predictive closer to the drip line.
- Agreement with data for Gamow-Teller decays suggests the method may apply to other weak observables such as neutrino-nucleus scattering in similar mass regions.
Load-bearing premise
The chiral effective field theory forces and currents together with the IMSRG truncation are accurate enough for these extreme neutron-rich N=50 nuclei without any phenomenological adjustments to the weak operators or states.
What would settle it
New experimental beta-decay half-life measurements for additional N=50 neutron-rich nuclei that differ substantially from the values obtained when two-body currents are included.
Figures
read the original abstract
Beta-decay rates of extreme neutron-rich nuclei remain largely unknown experimentally, while they are critical inputs for $r$-process nucleosynthesis. We present first ab initio calculations of total beta-decay half-lives, with a focus on $N=50$ nuclei. Starting from nuclear forces and currents based on chiral effective field theory, we use the in-medium similarity renormalization group to consistently derive valence-space Hamiltonians and weak operators, from which we calculate the nuclear states involved and the Gamow-Teller transition strengths, without phenomenological adjustments. In addition, we explore effects of first-forbidden contributions. Our results show that the inclusion of two-body currents increases the total half-lives, which then show good agreement with the existing experimental data, thereby validating the predictive capability of our approach.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper presents the first ab initio calculations of total beta-decay half-lives for N=50 neutron-rich nuclei. Starting from chiral EFT nuclear forces and currents, the IMSRG is used to derive consistent valence-space Hamiltonians and weak operators (including two-body currents) without phenomenological adjustments; Gamow-Teller strengths are computed and first-forbidden contributions are explored. The central result is that two-body currents increase the half-lives, producing good agreement with existing experimental data and thereby validating the predictive power of the approach for r-process relevant nuclei.
Significance. If the convergence and error control are adequate, the work supplies much-needed ab initio predictions for beta-decay rates in the N=50 region where data are sparse, directly impacting r-process nucleosynthesis modeling. The consistent derivation of both Hamiltonian and weak operators from the same chiral EFT framework, together with the explicit inclusion of two-body currents, constitutes a clear methodological advance over phenomenological shell-model treatments.
major comments (2)
- [Computational details / Results] The manuscript reports results at a fixed chiral order and IMSRG(2) level but does not present IMSRG(3) calculations, enlarged valence spaces, or explicit convergence tests with respect to the many-body truncation for the N=50 systems. Because the Gamow-Teller matrix elements (and therefore the half-lives that are claimed to agree with data after two-body currents are added) are directly sensitive to missing higher-body induced terms, this omission is load-bearing for the central claim of predictive accuracy.
- [Results and Discussion] Quantitative measures of agreement with experiment (e.g., mean deviation, rms error, or per-nucleus comparison tables) and error estimates arising from the chiral truncation and IMSRG approximation are not provided. Without these, the statement that the half-lives “show good agreement with the existing experimental data” cannot be rigorously assessed.
minor comments (1)
- [Abstract] The abstract states that first-forbidden contributions are explored but does not indicate how they are quantified or whether they are included in the final half-life values shown to agree with data.
Simulated Author's Rebuttal
We thank the referee for the careful and constructive review. The positive evaluation of the work's significance for r-process modeling is appreciated. We address each major comment below and indicate the changes made to strengthen the manuscript.
read point-by-point responses
-
Referee: [Computational details / Results] The manuscript reports results at a fixed chiral order and IMSRG(2) level but does not present IMSRG(3) calculations, enlarged valence spaces, or explicit convergence tests with respect to the many-body truncation for the N=50 systems. Because the Gamow-Teller matrix elements (and therefore the half-lives that are claimed to agree with data after two-body currents are added) are directly sensitive to missing higher-body induced terms, this omission is load-bearing for the central claim of predictive accuracy.
Authors: We agree that systematic convergence studies would further bolster the error analysis. However, IMSRG(3) calculations for N=50 nuclei remain computationally prohibitive at present given the scaling of the method. We have added a dedicated paragraph discussing the expected magnitude of IMSRG(2) truncation errors, drawing on benchmark comparisons between IMSRG(2) and IMSRG(3) in lighter systems from the literature. We have also performed and reported calculations in an alternative, enlarged valence space for selected nuclei to quantify model-space sensitivity. These additions provide a more complete picture of theoretical uncertainties without altering the central results. revision: partial
-
Referee: [Results and Discussion] Quantitative measures of agreement with experiment (e.g., mean deviation, rms error, or per-nucleus comparison tables) and error estimates arising from the chiral truncation and IMSRG approximation are not provided. Without these, the statement that the half-lives “show good agreement with the existing experimental data” cannot be rigorously assessed.
Authors: We accept this criticism and have revised the manuscript to include quantitative metrics. A new table now lists calculated versus experimental half-lives for all nuclei with available data. We report the mean absolute deviation and root-mean-square deviation in the text. Error estimates from the chiral truncation are provided by comparing results at successive orders in the EFT expansion, while IMSRG-related uncertainties are estimated from the benchmarks discussed in response to the first comment. These changes allow a more rigorous evaluation of the agreement with data. revision: yes
- Full IMSRG(3) calculations for the complete set of N=50 nuclei, which exceed current computational resources.
Circularity Check
No circularity: ab initio derivation from chiral EFT and IMSRG remains independent of target half-lives
full rationale
The paper's derivation starts from established chiral EFT nuclear forces and currents, applies the standard IMSRG method to derive effective valence-space Hamiltonians and weak operators (including two-body currents), computes nuclear states and Gamow-Teller strengths, and includes first-forbidden contributions. The abstract explicitly states calculations are performed 'without phenomenological adjustments' and presents agreement with experimental data as validation of predictive capability rather than a fitted outcome. No steps reduce by construction to the target half-lives, no parameters are fitted to the N=50 data, and no load-bearing self-citations or uniqueness theorems are invoked to force the result. The central claim is externally falsifiable against measured half-lives and does not rely on self-referential definitions or renamed empirical patterns.
Axiom & Free-Parameter Ledger
axioms (3)
- domain assumption Nuclear forces and currents from chiral effective field theory are sufficiently accurate for N=50 neutron-rich nuclei
- domain assumption The in-medium similarity renormalization group consistently derives valence-space Hamiltonians and weak operators
- domain assumption First-forbidden contributions can be incorporated within the same framework
Lean theorems connected to this paper
-
IndisputableMonolith/Foundation/RealityFromDistinction.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
Starting from nuclear forces and currents based on chiral effective field theory, we use the in-medium similarity renormalization group to consistently derive valence-space Hamiltonians and weak operators... without phenomenological adjustments.
-
IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel contradicts?
contradictsCONTRADICTS: the theorem conflicts with this paper passage, or marks a claim that would need revision before publication.
We use the 1.8/2.0 (EM) NN+3N interaction... fit to NN scattering, the 3H energy, and the 4He radius.
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Forward citations
Cited by 2 Pith papers
-
Ab initio correlations between neutrinoless and two-neutrino double-beta decays in $^{48}$Ca
Ab initio IM-NCCI calculations on 48Ca establish strong linear correlations between 0νββ and 2νββ NMEs across 34 chiral Hamiltonians, yielding a constrained M^{0ν} prediction of 1.30-1.65 after incorporating experimen...
-
Computational schemes for the Magnus expansion of the in-medium similarity renormalization group
The hunter-gatherer scheme for the Magnus expansion in IMSRG(3) approximations introduces differences of up to 7 MeV in ground-state energies and 0.5 MeV in excitation energies compared to standard IMSRG(2) methods.
Reference graph
Works this paper leans on
-
[1]
with a similar estimate of 2.2 MeV for 78Cu. We note that the spectrum is similarly well reproduced as for other VS-IMSRG cal- culations [ 56, 57], where a different valence space (not applicable for beta decays) was used. Moreover, Fig. 1 clearly shows the important impact of 2B currents, which is to decrease the GT strength and thus increase the half-lif...
-
[2]
We emphasize that no adjustments to half-lives or GT transitions have been made
We find that the inclusion of 2B currents leads to longer total half-lives for all N = 50 nuclei stud- ied, leading to a very good agreement with experiment for Z = 28 − 32 and reproducing the trend down to Z = 27. We emphasize that no adjustments to half-lives or GT transitions have been made. The results are obtained only by using the given Hamiltonian w...
-
[3]
The inclusion of 2B currents systemati- cally reduces the B(GT) across the whole energy region, 4 0 5 10 15 20 Ex (MeV) 0 0.2 0.4 0.6 0.8 1.0B(GT) 1.8/2.0 (EM) GT1B GT1B+2B 0 5 10 15 20 25 Ex (MeV) ∆N 2LOGO (394) 78Ni(0+ gs) → 78Cu(1+) GT1B GT1B+2B 2 4 6 8 10 12 Ex (MeV) 0 2 4 6 8Running sum of t− 1 fi (s− 1) 78Ni(0+ gs) → 78Cu(1+) 2 3 4 5 6 7 Ex (MeV) 0 0...
-
[4]
However, for 78Ni the ∆N 2LOGO (394) interaction leads to a longer half- life
Moreover, we find con- sistent results for the total half-lives with 2B currents at Z = 24 and 32 for both interactions. However, for 78Ni the ∆N 2LOGO (394) interaction leads to a longer half- life. To analyze this further, we show in the right panel of Fig. 4 the running sums of the inverse partial half-lives. For 78Ni, we observe quite different running ...
-
[5]
free FF”) or with phenomenological quench- ing (“quenched FF
is replaced by 24 25 26 27 28 29 30 31 32 Z 10− 3 10− 2 10− 1 100 101 T1/2 (s) 1.8/2.0 (EM) GT1B+2B GT1B+2B + quenched FF GT1B+2B + free FF Expt. 0 10 20 30 40FF proportion (%) FIG. 5. Total beta-decay half-lives of N = 50 waiting point nuclei calculated from the VS-IMSRG for the 1.8/2.0 (EM) interaction with 2B currents compared to experiment [ 31, 46]. ...
work page 2020
- [6]
-
[7]
J. J. Cowan, C. Sneden, J. E. Lawler, A. Apra- hamian, M. Wiescher, K. Langanke, G. Martínez- Pinedo, and F.-K. Thielemann, Origin of the heav- iest elements: The rapid neutron-capture process, Rev. Mod. Phys. 93, 015002 (2021)
work page 2021
-
[8]
A. Arcones and F.-K. Thielemann, Origin of the ele- ments, Astron. Astrophys. Rev. 31, 1 (2023)
work page 2023
-
[9]
M. R. Mumpower, R. Surman, G. C. McLaugh- lin, and A. Aprahamian, The impact of individ- ual nuclear properties on r-process nucleosynthesis, Prog. Part. Nucl. Phys. 86, 86 (2016)
work page 2016
- [10]
-
[11]
I. N. Borzov, Gamow-Teller and first-forbidden decays near the r-process paths at N = 50 , 82, and 126, Phys. Rev. C 67, 025802 (2003)
work page 2003
- [12]
-
[13]
T. Marketin, D. Vretenar, and P. Ring, Cal- culation of β -decay rates in a relativistic model with momentum-dependent self-energies, Phys. Rev. C 75, 024304 (2007)
work page 2007
-
[14]
M. T. Mustonen and J. Engel, Global descrip- tion of β − decay in even-even nuclei with the axially-deformed skyrme finite-amplitude method, Phys. Rev. C 93, 014304 (2016)
work page 2016
-
[15]
T. Marketin, L. Huther, and G. Martínez-Pinedo, Large-scale evaluation of β -decay rates of r-process nu- clei with the inclusion of first-forbidden transitions, Phys. Rev. C 93, 025805 (2016)
work page 2016
-
[16]
E. M. Ney, J. Engel, T. Li, and N. Schunck, Global de- scription of β − decay with the axially deformed skyrme finite-amplitude method: Extension to odd-mass and odd-odd nuclei, Phys. Rev. C 102, 034326 (2020)
work page 2020
-
[17]
C. E. P. Robin and G. Martínez-Pinedo, Competition between allowed and first-forbidden β decay in r-process waiting-point nuclei within a relativistic beyond-mean- field approach, Phys. Rev. C 110, 065803 (2024)
work page 2024
-
[18]
G. Martínez-Pinedo and K. Langanke, Shell-model half- lives for N = 82 nuclei and their implications for the r process, Phys. Rev. Lett. 83, 4502 (1999)
work page 1999
-
[19]
J. Cuenca-García, G. Martınez-Pinedo, K. Langanke, F. Nowacki, and I. Borzov, Shell model half-lives for r- process N = 82 nuclei, Eur. Phys. J. A 34, 99 (2007)
work page 2007
- [20]
-
[21]
Q. Zhi, E. Caurier, J. J. Cuenca-García, K. Langanke, G. Martínez-Pinedo, and K. Sieja, Shell-model half- lives including first-forbidden contributions for r-process waiting-point nuclei, Phys. Rev. C 87, 025803 (2013)
work page 2013
-
[22]
S. Yoshida, Y. Utsuno, N. Shimizu, and T. Otsuka, Systematic shell-model study of β -decay properties and Gamow-Teller strength distributions in A ≈ 40 neutron- rich nuclei, Phys. Rev. C 97, 054321 (2018) , [Erratum: Phys. Rev. C 109, 029904 (2024) ]
work page 2018
- [23]
-
[24]
E. Epelbaum, H.-W. Hammer, and U.-G. Meißner, Modern theory of nuclear forces, Rev. Mod. Phys. 81, 1773 (2009)
work page 2009
-
[25]
R. Machleidt and D. Entem, Chiral effective field theory and nuclear forces, Phys. Rep. 503, 1 (2011)
work page 2011
-
[26]
Hergert, A guided tour of ab initio nuclear many-body theory, Front
H. Hergert, A guided tour of ab initio nuclear many-body theory, Front. Phys. 8, 379 (2020)
work page 2020
-
[27]
K. Hebeler, Three-nucleon forces: Implementation 6 and applications to atomic nuclei and dense matter, Phys. Rep. 890, 1 (2021)
work page 2021
-
[28]
P. Gysbers, G. Hagen, J. D. Holt, G. R. Jansen, T. D. Morris, P. Navrátil, T. Papenbrock, S. Quaglioni, A. Schwenk, S. R. Stroberg, and K. A. Wendt, Discrepancy between experimental and theoret- ical β -decay rates resolved from first principles, Nature Phys. 15, 428 (2019)
work page 2019
-
[29]
K. Tsukiyama, S. K. Bogner, and A. Schwenk, In- Medium Similarity Renormalization Group For Nuclei, Phys. Rev. Lett. 106, 222502 (2011)
work page 2011
-
[30]
K. Tsukiyama, S. K. Bogner, and A. Schwenk, In-medium similarity renormalization group for open-shell nuclei, Phys. Rev. C 85, 061304 (2012)
work page 2012
-
[31]
H. Hergert, S. K. Bogner, T. D. Morris, A. Schwenk, and K. Tsukiyama, The In-Medium Similarity Renor- malization Group: A novel ab initio method for nuclei, Phys. Rep. 621, 165 (2016)
work page 2016
-
[32]
S. R. Stroberg, A. Calci, H. Hergert, J. D. Holt, S. K. Bogner, R. Roth, and A. Schwenk, Nucleus- dependent valence-space approach to nuclear structure, Phys. Rev. Lett. 118, 032502 (2017)
work page 2017
-
[33]
S. R. Stroberg, H. Hergert, S. K. Bogner, and J. D. Holt, Nonempirical interactions for the nuclear shell model: An update, Annu. Rev. Nucl. Part. Sci. 69, 307 (2019)
work page 2019
-
[34]
P. T. Hosmer, H. Schatz, A. Aprahamian, O. Arndt, R. R. C. Clement, A. Estrade, K.-L. Kratz, S. N. Liddick, P. F. Mantica, W. F. Mueller, F. Montes, A. C. Morton, M. Ouellette, E. Pellegrini, B. Pfeif- fer, P. Reeder, P. Santi, M. Steiner, A. Stolz, B. E. Tomlin, W. B. Walters, and A. Wöhr, Half- Life of the Doubly Magic r-Process Nucleus 78Ni, Phys. Rev....
work page 2005
-
[35]
P. Hosmer, H. Schatz, A. Aprahamian, O. Arndt, R. R. C. Clement, A. Estrade, K. Farouqi, K.-L. Kratz, S. N. Liddick, A. F. Lisetskiy, P. F. Mantica, P. Möller, W. F. Mueller, F. Montes, A. C. Morton, M. Ouellette, E. Pellegrini, J. Pereira, B. Pfeiffer, P. Reeder, P. Santi, M. Steiner, A. Stolz, B. E. Tomlin, W. B. Walters, and A. Wöhr, Half-lives and bran...
work page 2010
-
[36]
Z. Y. Xu, S. Nishimura, G. Lorusso, F. Browne, P. Door- nenbal, G. Gey, H.-S. Jung, Z. Li, M. Niikura, P.- A. Söderström, T. Sumikama, J. Taprogge, Z. Va- jta, H. Watanabe, J. Wu, A. Yagi, K. Yoshinaga, H. Baba, S. Franchoo, T. Isobe, P. R. John, I. Ko- jouharov, S. Kubono, N. Kurz, I. Matea, K. Matsui, D. Mengoni, P. Morfouace, D. R. Napoli, F. Naqvi, H....
work page 2014
-
[37]
A. Tolosa-Delgado, J. L. Tain, M. Reichert, A. Ar- cones, M. Eichler, B. C. Rasco, N. T. Brewer, K. P. Rykaczewski, R. Yokoyama, R. Grzywacz, I. Dillmann, J. Agramunt, D. S. Ahn, A. Algora, H. Baba, S. Bae, C. G. Bruno, R. Caballero Folch, F. Calvino, P. J. Coleman-Smith, G. Cortes, T. Davinson, C. Domingo- Pardo, A. Estrade, N. Fukuda, S. Go, C. J. Griffin...
work page 2025
-
[38]
Suhonen, From Nucleons to Nucleus: Concepts of Microscopic Nucle (Springer Berlin, Heidelberg, 2007)
J. Suhonen, From Nucleons to Nucleus: Concepts of Microscopic Nucle (Springer Berlin, Heidelberg, 2007)
work page 2007
-
[39]
J. C. Hardy and I. S. Towner, Superallowed 0+ → 0+ nuclear β decays: 2020 critical sur- vey, with implications for Vud and CKM unitarity, Phys. Rev. C 102, 045501 (2020)
work page 2020
-
[40]
H. Behrens and W. Bühring, Nuclear beta decay, Nucl. Phys. A 162, 111 (1971)
work page 1971
-
[41]
H. Behrens and W. Bühring, Electron Radial Wave Functions and Nuclear Beta-Decay (Clarendon Press, 1982)
work page 1982
-
[42]
T.-S. Park, L. E. Marcucci, R. Schiavilla, M. Viviani, A. Kievsky, S. Rosati, K. Kubodera, D.-P. Min, and M. Rho, Parameter-free effective field theory calcu- lation for the solar proton-fusion and hep processes, Phys. Rev. C 67, 055206 (2003)
work page 2003
-
[43]
M. Hoferichter, J. Menéndez, and A. Schwenk, Coherent elastic neutrino-nucleus scattering: EFT analysis and nu- clear responses, Phys. Rev. D 102, 074018 (2020)
work page 2020
-
[44]
Krebs, Nuclear Currents in Chiral Effective Field The- ory, Eur
H. Krebs, Nuclear Currents in Chiral Effective Field The- ory, Eur. Phys. J. A 56, 234 (2020)
work page 2020
-
[45]
K. Hebeler, S. K. Bogner, R. J. Furnstahl, A. Nogga, and A. Schwenk, Improved nuclear matter cal- culations from chiral low-momentum interactions, Phys. Rev. C 83, 031301 (2011)
work page 2011
-
[46]
S. R. Stroberg, J. D. Holt, A. Schwenk, and J. Simonis, Ab initio limits of atomic nuclei, Phys. Rev. Lett. 126, 022501 (2021)
work page 2021
-
[47]
W. G. Jiang, A. Ekström, C. Forssén, G. Hagen, G. R. Jansen, and T. Papenbrock, Accurate bulk properties of nuclei from A = 2 to ∞ from potentials with ∆ isobars, Phys. Rev. C 102, 054301 (2020)
work page 2020
- [48]
-
[49]
T. Miyagi, NuHamil: A numerical code to generate nu- clear two- and three-body matrix elements from chiral effective field theory, Eur. Phys. J. A 59, 150 (2023)
work page 2023
- [50]
-
[51]
National Nuclear Data Center, https://www.nndc.bnl.gov
-
[52]
M. Wang, W. Huang, F. Kondev, G. Audi, and S. Naimi, The AME 2020 atomic mass evaluation (II). Tables, graphs and references, Chinese Phys. C 45, 030003 (2021)
work page 2020
- [53]
- [54]
-
[55]
T. D. Morris, N. M. Parzuchowski, and S. K. Bogner, Magnus expansion and in-medium similarity renormal- ization group, Phys. Rev. C 92, 034331 (2015)
work page 2015
-
[56]
D. Gloeckner and R. Lawson, Spurious center-of-mass motion, Phys. Lett. B 53, 313 (1974)
work page 1974
-
[57]
W. C. Haxton, K. M. Nollett, and K. M. Zurek, Piecewise moments method: Generalized Lanczos technique for nu- clear response surfaces, Phys. Rev. C 72, 065501 (2005)
work page 2005
-
[58]
E. Caurier, G. Martínez-Pinedo, F. Nowacki, A. Poves, and A. P. Zuker, The shell model as a unified view of nuclear structure, Rev. Mod. Phys. 77, 427 (2005)
work page 2005
-
[59]
S. R. Stroberg, https://github.com/ragnarstroberg/imsrg
-
[60]
N. Shimizu, T. Mizusaki, Y. Utsuno, and Y. Tsunoda, Thick-restart block lanczos method for large-scale shell-model calculations, Comput. Phys. Commun. 244, 372 (2019)
work page 2019
-
[61]
R. Taniuchi, C. Santamaria, P. Doornenbal, A. Obertelli, K. Yoneda, G. Authelet, H. Baba, D. Calvet, F. Château, A. Corsi, A. Delbart, J.-M. Gheller, A. Gillibert, J. D. Holt, T. Isobe, V. Lapoux, M. Matsushita, J. Menéndez, S. Momiyama, T. Motobayashi, M. Niikura, F. Nowacki, K. Ogata, H. Otsu, T. Otsuka, C. Péron, S. Péru, A. Peyaud, E. C. Pollacco, A. ...
work page 2019
- [62]
-
[63]
J. Menéndez, D. Gazit, and A. Schwenk, Chi- ral two-body currents in nuclei: Gamow-teller transitions and neutrinoless double-beta decay, Phys. Rev. Lett. 107, 062501 (2011)
work page 2011
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.