Recognition: 2 theorem links
· Lean TheoremNuclear giant resonances from first principles
Pith reviewed 2026-05-10 17:58 UTC · model grok-4.3
The pith
Ab initio many-body methods compute nuclear giant resonances from realistic interactions.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The central claim is that first-principles calculations of nuclear giant resonances are now feasible with multiple many-body techniques grounded in realistic interactions, and that their application to oxygen-16 and calcium-40 reveals both consistency among methods and connections to measured observables.
What carries the argument
The nuclear response function computed through ab initio many-body solvers applied to realistic Hamiltonians.
If this is right
- Agreement across independent methods on the same benchmark nuclei increases in the calculated response functions.
- Divergences between methods identify specific aspects of the many-body treatment that require further development.
- Direct comparison with experimental observables validates or constrains the underlying realistic nuclear interactions.
- The same frameworks can be used to predict other electromagnetic or weak response properties in these nuclei.
Where Pith is reading between the lines
- If the methods prove reliable here, they could be applied next to neighboring light nuclei to map how resonance properties change with neutron number.
- Persistent differences with data might point to the need for improved treatment of three-body forces in the response calculation.
- Consistent predictions across methods would allow theorists to use the cheapest reliable approach for systematic studies of additional observables.
Load-bearing premise
The assumption that the selected methods and the nuclei oxygen-16 and calcium-40 provide a fair test of the approaches' ability to describe giant resonances across a wider range of nuclei and observables.
What would settle it
A large mismatch between the calculated giant resonance positions, widths, or strengths and the corresponding experimental data for oxygen-16 or calcium-40 would show that the methods do not yet capture the relevant physics.
read the original abstract
This chapter presents an ab initio perspective on giant resonances in atomic nuclei and surveys the principal theoretical frameworks that aim to describe these collective excitations from first principles. While the study of nuclear giant resonances has traditionally been dominated by the energy density functional approach, recent years have witnessed the development of advanced many-body approaches grounded directly in realistic nuclear interactions, namely, Hamiltonians that reproduce nucleon-nucleon phase shifts and accurately describe the binding energies of light nuclei. Within this modern framework, we review the main many-body methods currently used to compute nuclear response functions. These include the random phase approximation, the Lorentz integral transform coupled-cluster theory, the projected generator-coordinate method, and the self-consistent Green's functions approach. After giving a general conceptual and historical overview of giant-resonance phenomena, we outline the theoretical foundations and computational implementations of each method. We conclude with a critical comparison of their predictions for selected benchmark nuclei, $^{16}$O and $^{40}$Ca, emphasizing points of agreement and divergence, while maintaining a close connection to the relevant experimental observables.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. This manuscript is a review chapter that surveys ab initio many-body methods for computing nuclear giant resonances from realistic nucleon-nucleon interactions. It covers conceptual foundations, outlines the random phase approximation (RPA), Lorentz integral transform coupled-cluster (LIT-CC), projected generator-coordinate method (PGCM), and self-consistent Green's functions (SCGF) approaches, and concludes with a comparison of their predictions for the benchmark nuclei 16O and 40Ca against experimental observables.
Significance. If the comparisons are accurate and balanced, the review would be useful for the field by synthesizing how recent ab initio frameworks grounded in realistic Hamiltonians can access response functions for collective excitations, contrasting with traditional EDF methods. It explicitly credits existing literature for methods and predictions without asserting new derivations or fits, providing a descriptive synthesis rather than novel claims.
minor comments (2)
- The abstract states that the comparison emphasizes 'points of agreement and divergence' for 16O and 40Ca; adding a summary table of key observables (e.g., centroid energies, widths) across methods would improve readability without altering the descriptive scope.
- Section on historical overview: the transition from EDF to ab initio methods is well-motivated, but a brief sentence on why closed-shell nuclei were chosen as benchmarks (computational tractability) would clarify the scope limitation noted in the reader's assessment.
Simulated Author's Rebuttal
We thank the referee for their positive assessment of our manuscript and for recommending acceptance. We are pleased that the review is viewed as a useful synthesis for the field.
Circularity Check
No significant circularity; review of established external methods
full rationale
This is a review chapter surveying established ab initio frameworks (RPA, LIT-CC, PGCM, SCGF) drawn from prior literature for computing nuclear response functions in giant resonances. The manuscript outlines conceptual foundations, historical context, and computational implementations by reference to external works, then summarizes previously published predictions for the benchmark nuclei 16O and 40Ca without performing new derivations, fits, or self-referential calculations. No equations or claims in the paper reduce by construction to its own inputs; all load-bearing content is externally sourced and independently verifiable. This satisfies the criteria for zero circularity.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Realistic nuclear interactions reproduce nucleon-nucleon phase shifts and accurately describe the binding energies of light nuclei.
Lean theorems connected to this paper
-
IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel (J(x) uniqueness) unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
Response function R(ω) = 1/(2J0+1) Σ |⟨Ψ0|O|Ψν⟩|² δ(Eν−E0−ω); linear-response polarization ΠAB(ω) with Lehmann representation; LIT L(σ,Γ) = Γ/π ∫ R(ω)/((σ−ω)²+Γ²) dω inverted numerically.
-
IndisputableMonolith/Foundation/RealityFromDistinction.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
Ab initio methods start from Schrödinger equation with χEFT Hamiltonians; no adjustable parameters tuned to finite nuclei.
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.
Reference graph
Works this paper leans on
-
[1]
On the monopole and quadrupole isoscalar giant resonances in 4 He, 16 O, 20 Ne and 40 Ca.Phys
Abgrall Y and Caurier E (1975). On the monopole and quadrupole isoscalar giant resonances in 4 He, 16 O, 20 Ne and 40 Ca.Phys. Lett. B56: 229–231. doi:10.1016/0370-2693(75)90381-0. Ahrens J (1985). The total absorption of photons by nuclei.Nuclear Physics A446 (1): 229–239. ISSN 0375-9474. doi:https://doi.org/10.1016/ 0375-9474(85)90591-3. Ahrens J, Borch...
-
[2]
Bally B, Scalesi A, Som` a V, Zurek L and Duguet T (2025)
doi:10.1140/epja/s10050-024-01271-0.2401.00941. Bally B, Scalesi A, Som` a V, Zurek L and Duguet T (2025). Mean-field approximation on steroids: exact description of the deuteron.Eur. Phys. J. A61 (6):
work page doi:10.1140/epja/s10050-024-01271-0.2401.00941 2025
-
[3]
Barbieri C and Carbone A (2017)
doi:10.1140/epja/s10050-025-01596-4.2410.03356. Barbieri C and Carbone A (2017). Self-Consistent Green’s Function Approaches, Springer International Publishing, Cham. ISBN 978-3-319-53336-0, 571–644. doi:10.1007/978-3-319-53336-0
work page doi:10.1140/epja/s10050-025-01596-4.2410.03356 2017
-
[4]
Barbieri C and Dickhoff WH (2003). Extension of the random phase approximation including the selfconsistent coupling to two phonon contributions. Phys. Rev. C68: 014311. doi:10.1103/PhysRevC.68.014311.nucl-th/0212025. Barbieri C, Raimondi F and Mcilroy C (2018). Recent Applications of Self-Consistent Green’s Function Theory to Nuclei.J. Phys. Conf. Ser.96...
work page doi:10.1103/physrevc.68.014311.nucl-th/0212025 2003
-
[5]
Gorkov algebraic diagrammatic construction formalism at third order.Phys. Rev. C105: 044330. doi: 10.1103/PhysRevC.105.044330.https://link.aps.org/doi/10.1103/PhysRevC.105.044330. Barnea N, Efros VD, Leidemann W and Orlandini G (2010). The Lorentz Integral Transform and its Inversion.Few Body Syst.47: 201–206. doi: 10.1007/s00601-009-0081-0.0906.5421. Bar...
work page doi:10.1103/physrevc.105.044330.https://link.aps.org/doi/10.1103/physrevc.105.044330 2010
-
[6]
Electric dipole polarizability of 48Caand implications for the neutron skin.Phys
Birkhan J, Miorelli M, Bacca S, Bassauer S, Bertulani CA, Hagen G, Matsubara H, von Neumann-Cosel P, Papenbrock T, Pietralla N, Ponomarev VY, Richter A, Schwenk A and Tamii A (2017), Jun. Electric dipole polarizability of 48Caand implications for the neutron skin.Phys. Rev. Lett.118: 252501. doi:10.1103/PhysRevLett.118.252501.https://link.aps.org/doi/10.1...
work page doi:10.1103/physrevlett.118.252501.https://link.aps.org/doi/10.1103/physrevlett.118.252501 2017
-
[7]
Bonaiti F, Bacca S, Hagen G and Jansen GR (2024), Oct
doi:10.1016/0370-1573(79)90079-6. Bonaiti F, Bacca S, Hagen G and Jansen GR (2024), Oct. Electromagnetic observables of open-shell nuclei from coupled-cluster theory.Phys. Rev. C 110: 044306. doi:10.1103/PhysRevC.110.044306.https://link.aps.org/doi/10.1103/PhysRevC.110.044306. Bonaiti F, Hagen G and Papenbrock T (2025),
-
[8]
Bonaiti F, Porro A, Bacca S, Schwenk A and Tichai A (2026), Feb
Structure of the doubly magic nuclei 208Pb and 266Pb from ab initio computations2508.14217. Bonaiti F, Porro A, Bacca S, Schwenk A and Tichai A (2026), Feb. Ab initio calculations of monopole sum rules: From finite nuclei to infinite nuclear matter.Phys. Rev. C113: 024333. doi:10.1103/kfdd-79g7.https://link.aps.org/doi/10.1103/kfdd-79g7. Bracco A, Lanza E...
work page doi:10.1103/kfdd-79g7.https://link.aps.org/doi/10.1103/kfdd-79g7 2026
-
[9]
Caurier E, Bourotte-Bilwes B and Abgrall Y (1973)
doi:10.1103/RevModPhys.87.1067.1412.3081. Caurier E, Bourotte-Bilwes B and Abgrall Y (1973). Microscopic treatment of the coupled monopole and quadrupole vibrations in light nuclei.Phys. Lett. B44: 411–415. doi:10.1016/0370-2693(73)90321-3. Chadwick M and et al. (2011). Endf/b-vii.1 nuclear data for science and technology: Cross sections, covariances, fis...
-
[10]
Symmetry restoration in the axially deformed proton-neutron quasiparticle random phase approximation for nuclear beta decay: The effect of angular-momentum projection2510.16313. Coello-P´ erez EA (2026), Low-energy collective excitations in atomic nuclei, Encyclopedia of Nuclear Physics, Elsevier. Col` o G (2022). Theoretical Methods for Giant Resonances....
-
[11]
doi:10.1140/epja/s10050-023-00914-y.2209.03424. Edmonds AR (1996). Angular momentum in quantum mechanics, 4, Princeton university press. Efros VD, Leidemann W and Orlandini G (1994). Response functions from integral transforms with a lorentz ker- nel.Physics Letters B338 (2): 130–133. ISSN 0370-2693. doi:https://doi.org/10.1016/0370-2693(94)91355-2. https...
work page doi:10.1140/epja/s10050-023-00914-y.2209.03424 1996
-
[12]
Accurate nuclear radii and binding energies from a chiral interaction.Phys. Rev. C91: 051301(R). doi:10.1103/PhysRevC.91.051301. https://link.aps.org/doi/10.1103/PhysRevC.91.051301. Ekstr¨ om A, Forss´ en C, Hagen G, Jansen GR, Jiang W and Papenbrock T (2023). What is ab initio in nuclear theory?Frontiers in Physics11: 1129094. doi:10.3389/fphy.2023.11290...
-
[13]
doi:10.1007/s00601-024-01918-0
Chiral symmetry and nuclear interactions.Few-Body Systems65. doi:10.1007/s00601-024-01918-0. Erler J, Kl¨ upfel P and Reinhard PG (2011). Self-consistent nuclear mean-field models: example skyrme-hartree-fock.J. Phys. G: Nucl. Part. Phys.38: 033101. doi:doi:10.1088/0954-3899/38/3/033101. And references therein. Fabrizio M (2022). Linear Response Theory, S...
-
[14]
Frosini M, Duguet T, Ebran JP, Bally B, Mongelli T, Rodr ´ ıguez TR, Roth R and Som` a V (2022b)
doi:10.1140/epja/s10050-022-00694-x.2111.01461. Frosini M, Duguet T, Ebran JP, Bally B, Mongelli T, Rodr ´ ıguez TR, Roth R and Som` a V (2022b). Multi-reference many-body perturbation theory for nuclei: II. Ab initio study of neon isotopes via PGCM and IM-NCSM calculations.Eur. Phys. J. A58 (4):
-
[15]
doi:10.1140/epja/s10050-022-00693-y. 2111.00797. Frosini M, Duguet T, Ebran JP and Som` a V (2022c). Multi-reference many-body perturbation theory for nuclei: I. Novel PGCM-PT formalism.Eur. Phys. J. A58 (4):
-
[16]
Gambacurta D and Grasso M (2016)
doi:10.1140/epja/s10050-022-00692-z.2110.15737. Gambacurta D and Grasso M (2016). Second RPA calculations with the Skyrme and Gogny interactions.Eur. Phys. J. A52 (7):
work page doi:10.1140/epja/s10050-022-00692-z.2110.15737 2016
-
[17]
Analysis of the vertexes Ξ ∗ QΞ′ QV, Σ∗ QΣQVand radiative decays Ξ ∗ Q →Ξ ′ Qγ, Σ ∗ Q →Σ Qγ
doi:10.1140/epja/ i2016-16198-6. Gambacurta D, Grasso M and Catara F (2010). Collective nuclear excitations with Skyrme-Second RPA.Phys. Rev. C81: 054312. doi:10.1103/ PhysRevC.81.054312.1002.3563. Garg U (2023). Isoscalar Giant Resonances: Experimental Studies, Springer Nature Singapore, Singapore. ISBN 978-981-19-6345-2, 631–673. doi: 10.1007/978-981-19-6345-2
-
[18]
Garg U and Col` o G (2018). The compression-mode giant resonances and nuclear incompressibility.Prog. Part. Nucl. Phys.101: 55–95. doi:10.1016/j. ppnp.2018.03.001.1801.03672. Gazit D, Barnea N, Bacca S, Leidemann W and Orlandini G (2006), Dec. Photonuclear sum rules and the tetrahedral configuration of 4He.Phys. Rev. C74: 061001. doi:10.1103/PhysRevC.74.0...
work page doi:10.1016/j 2018
-
[19]
https://doi.org/10.1140/epja/s10050-023-00931-x
ISSN 1434-601X. https://doi.org/10.1140/epja/s10050-023-00931-x. Gour JR, Piecuch P, Hjorth-Jensen M, W loch M and Dean DJ (2006), Aug. Coupled-cluster calculations for valence systems around 16O.Phys. Rev. C 74: 024310. doi:10.1103/PhysRevC.74.024310.https://link.aps.org/doi/10.1103/PhysRevC.74.024310. Griffin JJ and Wheeler JA (1957). Collective Motions...
-
[20]
A Guided Tour of ab initio Nuclear Many-Body Theory.Front
ISSN 2296-424X. doi:10.3389/fphy.2020.00379. https://www.frontiersin.org/article/10.3389/fphy.2020.00379. Hergert H (2026), What is ab initio in nuclear theory?, Encyclopedia of Nuclear Physics, Elsevier. Hergert H, Bogner SK, Morris TD, Schwenk A and Tsukiyama K (2016a). The In-Medium Similarity Renormalization Group: A Novel Ab Initio Method for Nuclei....
-
[21]
ISSN 2296-424X. doi:10.3389/fphy.2019.00251. https://www.frontiersin.org/journals/physics/articles/10.3389/fphy.2019.00251. Lazauskas R, Hiyama E and Carbonell J (2019). Ab initio calculations of 5h resonant states.Physics Letters B791: 335–341. ISSN 0370-2693. doi: https://doi.org/10.1016/j.physletb.2019.02.047.https://www.sciencedirect.com/science/artic...
-
[22]
Marino F, Bonaiti F, Bacca S, Hagen G and Jansen GR (2025b), Jul
Electromagnetic sum rules for 22O from coupled-cluster theory.arxiv:2509.160012509.16001. Marino F, Bonaiti F, Bacca S, Hagen G and Jansen GR (2025b), Jul. Structure and dynamics of open-shell nuclei from spherical coupled-cluster theory. Phys. Rev. C112: 014315. doi:10.1103/vbsk-fmqh.https://link.aps.org/doi/10.1103/vbsk-fmqh. Mart ´ ınez-Larraz J and Ro...
work page doi:10.1103/vbsk-fmqh.https://link.aps.org/doi/10.1103/vbsk-fmqh 2022
-
[23]
doi:10.5506/APhysPolB.48.537. Papenbrock T (2024). Ab initio computations of atomic nuclei. doi:https://arxiv.org/abs/2410.00843.2410.00843. Parnes E, Barnea N, Carleo G, Lovato A, Rocco N and Zhang X (2026), Jan. Nuclear responses with neural-network quantum states.Phys. Rev. Lett. 136: 032501. doi:10.1103/tlqz-nw28.https://link.aps.org/doi/10.1103/tlqz-...
-
[24]
Collective effects in inelastic scattering from nuclei.Nuclear Physics27 (2): 270–283
Pinkston WT and Satchler G (1961). Collective effects in inelastic scattering from nuclei.Nuclear Physics27 (2): 270–283. Porro A, Col` o G, Duguet T, Gambacurta D and Som` a V (2024a). Symmetry-restored Skyrme-random-phase-approximation calculations of the monopole strength in deformed nuclei.Phys. Rev. C109 (4): 044315. doi:10.1103/PhysRevC.109.044315.2...
-
[25]
doi:10.1140/epja/s10050-024-01340-4. 2402.02228. Porro A, Duguet T, Ebran JP, Frosini M, Roth R and Som` a V (2024c). Ab initio description of monopole resonances in light- and medium-mass nuclei: II. Ab initio PGCM calculations in 46Ti, 28Si and 24Mg.Eur. Phys. J. A60 (6):
-
[26]
Porro A, Duguet T, Ebran JP, Frosini M, Roth R and Som` a V (2024d)
doi:10.1140/epja/s10050-024-01341-3.2402.15901. Porro A, Duguet T, Ebran JP, Frosini M, Roth R and Som` a V (2024d). Ab initio description of monopole resonances in light- and medium-mass nuclei: III. Moments evaluation in ab initio PGCM calculations.Eur. Phys. J. A60 (7):
-
[27]
Porro A, Duguet T, Ebran JP, Frosini M, Roth R and Som` a V (2024e)
doi:10.1140/epja/s10050-024-01377-5.2404.14154. Porro A, Duguet T, Ebran JP, Frosini M, Roth R and Som` a V (2024e). Ab initio description of monopole resonances in light- and medium-mass nuclei: IV. Angular momentum projection and rotation-vibration coupling.Eur. Phys. J. A60 (11):
-
[28]
Porro A, Schwenk A and Tichai A (2025)
doi:10.1140/epja/s10050-024-01448-7.2407.01325. Porro A, Schwenk A and Tichai A (2025). Impact of ground-state correlations on the multipole response of nuclei: Ab initio calculations of moment operators.Phys. Rev. C112 (5): 054303. doi:10.1103/1ktc-lknn.2507.20665. Quaglioni S and Navratil P (2007). The 4He total photo-absorption cross section with two- ...
work page doi:10.1140/epja/s10050-024-01448-7.2407.01325 2025
-
[29]
Nuclear electromagnetic dipole response with the self-consistent green’s function formalism.Phys. Rev. C99: 054327. doi:10.1103/PhysRevC.99.054327.https://link.aps.org/doi/10.1103/PhysRevC.99.054327. Ring P and Schuck P (1980). The Nuclear Many-Body Problem, first ed., Theoretical and Mathematical Physics, Springer, New York. https://link.springer.com/boo...
work page doi:10.1103/physrevc.99.054327.https://link.aps.org/doi/10.1103/physrevc.99.054327 1980
-
[30]
doi:https://doi.org/10.1016/j.ppnp.2018.04.001
ISSN 0146-6410. doi:https://doi.org/10.1016/j.ppnp.2018.04.001. http://www.sciencedirect.com/science/article/pii/S0146641018300334. Roth R and Navr´ atil P (2007). Importance-truncated no-core shell model.Physical Review Letters99 (9): 092501. doi:10.1103/PhysRevLett.99.092501. Roth R, Langhammer J, Calci A, Binder S and Navr´ atil P (2011), Aug. Similari...
-
[31]
Many-Body Methods for Atoms, Molecules and Clusters, Lecture Notes in Physics, Springer International Publishing. ISBN 978-3-319-93601-7. doi:10.1007/978-3-319-93602-4. Schunck N (2019). Energy density functional methods for atomic nuclei, IoP Publishing. Shavitt I and Bartlett RJ (2009). Many-Body Methods in Chemistry and Physics: MBPT and Coupled-Cluste...
-
[32]
Sobczyk JE, Acharya B, Bacca S and Hagen G (2021), Aug
doi:10.1140/ epja/i2019-12825-0.1905.02055. Sobczyk JE, Acharya B, Bacca S and Hagen G (2021), Aug. Ab initio computation of the longitudinal response function in 40Ca.Phys. Rev. Lett.127: 072501. doi:10.1103/PhysRevLett.127.072501.https://link.aps.org/doi/10.1103/PhysRevLett.127.072501. Sobczyk JE, Acharya B, Bacca S and Hagen G (2024). Ca40 transverse r...
work page doi:10.1103/physrevlett.127.072501.https://link.aps.org/doi/10.1103/physrevlett.127.072501 1905
-
[33]
Ab initio self-consistent gorkov-green’s function calculations of semimagic nu- clei: Formalism at second order with a two-nucleon interaction.Phys. Rev. C84: 064317. doi:10.1103/PhysRevC.84.064317. https://link.aps.org/doi/10.1103/PhysRevC.84.064317. Som` a V, Cipollone A, Barbieri C, Navr´ atil P and Duguet T (2014). Chiral two- and three-nucleon forces...
-
[34]
Novel chiral hamiltonian and observables in light and medium-mass nuclei.Phys. Rev. C101: 014318.https://link.aps.org/doi/10.1103/PhysRevC.101.014318. Som` a V (2020). Self-consistent green’s function theory for atomic nuclei.Frontiers in Physics8:
-
[35]
ISSN 2296-424X. doi:10.3389/fphy.2020.00340. https://www.frontiersin.org/article/10.3389/fphy.2020.00340. Speth J and van der Woude A (1981). Giant resonances in nuclei.Reports on Progress in Physics44 (7):
-
[36]
Steinwedel H and Jensen JHD (1950).Z
http://stacks.iop.org/0034-4885/44/i=7/a=002. Steinwedel H and Jensen JHD (1950).Z. Naturforsch.5A:
1950
-
[37]
Electric dipole polarizabilities of hydrogen and helium isotopes.Phys
Stetcu I, Quaglioni S, Friar JL, Hayes AC and Navr´ atil P (2009), Jun. Electric dipole polarizabilities of hydrogen and helium isotopes.Phys. Rev. C79: 064001. doi:10.1103/PhysRevC.79.064001.https://link.aps.org/doi/10.1103/PhysRevC.79.064001. Stoitsov MV, Ring P and Sharma MM (1994). Generator coordinate calculations for breathing-mode giant monopole re...
work page doi:10.1103/physrevc.79.064001.https://link.aps.org/doi/10.1103/physrevc.79.064001 2009
-
[38]
doi:10.1140/epja/i2019-12781-7.http://link.springer.com/10.1140/epja/i2019-12781-7
ISSN 1434-6001. doi:10.1140/epja/i2019-12781-7.http://link.springer.com/10.1140/epja/i2019-12781-7. von Neumann-Cosel P and Tamii A (2025). Electric dipole polarizability constraints on neutron skin and sym- metry energy.Frontiers in PhysicsVolume 13 -
work page doi:10.1140/epja/i2019-12781-7.http://link.springer.com/10.1140/epja/i2019-12781-7 2025
-
[39]
ISSN 2296-424X. doi:10.3389/fphy.2025.1629987. https://www.frontiersin.org/journals/physics/articles/10.3389/fphy.2025.1629987. Walecka JD (1995). Theoretical nuclear and subnuclear physics,
-
[40]
Production review of accelerator-based medical isotopes.Molecules27 (16):
Wang Y, Chen D, dos Santos Augusto R, Liang J, Qin Z, Liu J and Liu Z (2022). Production review of accelerator-based medical isotopes.Molecules27 (16):
2022
-
[41]
Whitehead RR (1980)
ISSN 1420-3049.https://www.mdpi.com/1420-3049/27/16/5294. Whitehead RR (1980). Moment Methods and Lanczos Methods, Springer US, Boston, MA. ISBN 978-1-4613-3120-9, 235–255. doi:10.1007/ 978-1-4613-3120-9
1980
-
[42]
Wu Q, Hu BS, Xu FR, Ma YZ, Dai SJ, Sun ZH and Jansen GR (2018). Chiral NNLO sat descriptions of nuclear multipole resonances within the random phase approximation.Phys. Rev. C97 (5): 054306. doi:10.1103/PhysRevC.97.054306. Youngblood DH, Rozsa CM, Moss JM, Brown DR and Bronson JD (1977). Isoscalar giant resonance region in 40ca.Physical Review Letters39: ...
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.