Submitted:
10 March 2026
Posted:
13 March 2026
You are already at the latest version
Abstract
Keywords:
1. Introduction to the 4G Model of Final Unification
2. Nuclear Binding Energy Formula with Single Set of Energy Coefficients for Z=2 to 118
- 1)
- Global Accuracy: Fixed coefficients achieve <1% errors across chart of nuclides (light to superheavy), reproducing iron peak (BE/A~8.7 MeV at ⁵⁶Fe), magic shells (Z/N=2,8,20,28,50,82), and driplines.
- 2)
- Physical Interpretability: Each term maps directly to nuclear physics (volume saturation, surface tension, proton repulsion, isospin imbalance, quantum pairing, neutron-skin damping), enabling stability predictions (fission barriers, β-decay Q-values).
- 3)
- Light Nuclei Robustness: [1-(1/A)] correction prevent divergences at low A; exponential damping handles extreme N/Z ratios better than standard asymmetry.
- 4)
- Computational Simplicity: Single set works for all Z- no piecewise tuning required; vectorizable for rapid A-loops (2Z to 3.5Z), enabling batch processing Z=1-140 with CSV/PNG outputs.
- 5)
- Predictive Power: Estimates unmeasured masses, fusion yields, and Avogadro implications; competitive with AME2020 least-squares fits.
- 6)
- Easy Fine tuning: With machine learning techniques and AI, above formula can be fine-tuned for a better accuracy [18].
2.1. Unified Atomic Energy Unit (UAEU) and the Avogadro Number
2.2. The Inverse of Binding-Limited Atomic Mass
- The Limit: Every atom is subject to a “mass defect”, where a portion of the constituent nucleons’ mass is converted into binding energy to hold the nucleons together.
- The emergence: There is a theoretical threshold where the efficiency of this binding reaches its peak (often associated with the iron/nickel peak on the binding energy curve). The Avogadro constant emerges as the natural scaling factor dictated by this maximum binding efficiency, effectively representing the point where subatomic binding transitions into macroscopic stability.
- Saturation Point: The strong nuclear force, which governs the interaction between quarks and gluons, has a limited range. As more nucleons are added to a system, the “density” of the strong force interactions reaches a saturation point where the nucleus cannot become any denser or more tightly bound.
- The Particle/Mass Ratio: This saturation creates a fixed ratio between the number of particles (elementary entities) and the total mass they can occupy. This ratio is what we measure as the Avogadro constant. If the strong force were slightly stronger or weaker, the saturation point would shift, and the “Avogadro number” required to make a “gram” or “kilogram” of matter would be different.
- Bottom-Up Reality: Instead of humans deciding that 6.022x1023 is the definition, this insight proposes that the universe enforces this number through the equilibrium of forces.
- Structural Necessity: The constant acts as the structural link between the quantum world (governed by QCD and binding energy) and the thermodynamic world (governed by bulk matter).
2.3. Variation of Avogadro Number for Z=2 to 118
3. 4G Micro-Macro Gravity Unification Scale
3.1. Three Assumptions and Two Applications of Our 4G Model of Final Unification
- 1)
- There exists a characteristic electroweak fermion of rest energy, . It can be considered as the zygote of all elementary particles.
- 2)
- There exists a nuclear elementary charge in such a way that, = Strong coupling constant [36] and .
- 3)
- Each atomic interaction is associated with a characteristic large gravitational coupling constant. Their fitted magnitudes are,

- 1)
- Recent high-precision astrophysical observations lend growing support to our first assumption of a characteristic electroweak fermion with rest energy near 585 GeV. In particular, the sharp spectral break at 1.17 TeV in the all-electron cosmic-ray spectrum reported by H.E.S.S., and independently confirmed by DAMPE and CALET, coincides precisely with twice the proposed fermion mass, suggesting the presence of bound or resonant fermion–antifermion states. This correspondence is further reinforced by Galactic gamma-ray excess studies, which infer neutral particles in the 500–800 GeV range, consistent with the neutral component of our 4G fermion doublet. Together, these converging astrophysical signatures provide empirical motivation for the 585 GeV fermion hypothesis, strengthening its role as a unifying microscopic origin for both nuclear phenomenology and TeV-scale cosmic-ray features [4].
- 2)
- In the 4G model, the strong coupling constant acquires a simple, physically transparent definition: , where is the fundamental electromagnetic charge and is the nuclear elementary charge. This relation reveals that strong interaction strength arises directly from the ratio of these fundamental charges, eliminating arbitrary empirical parameters. With nearly three times , the formula naturally yields 2, matching low-energy experimental values (–) and elegantly unifying electromagnetic and nuclear forces. In the context of the 4G model of nuclear charge, if one assigns a nuclear elementary charge of 3e to quarks, then the electromagnetic charges of the quark families can be expressed in a simple and unified manner. Specifically, the up-series quarks (u, c, t) carry an effective electromagnetic charge of 2e, while the down-series quarks (d, s, b) carry an effective charge of e. This formulation, provides a charge-based reinterpretation of quark structure [11]. It highlights how quark charges may be understood as scaled fractions of a fundamental nuclear charge, offering a natural bridge between electromagnetic and nuclear interactions within the 4G framework. The universal nuclear energy scale is set by Important point to be noted is that, the strong attraction between protons is about times stronger than the repulsive Coulomb energy, ensuring nuclear stability. Coming to the Bohr radius of Hydrogen atom, it is very interesting to note that, where
- 3)
- In our 4G framework, the necessity of large gravitational couplings arises from the fundamental requirement that point particles must sustain non-trivial spacetime curvature at quantum scales. If gravity were as weak as the classical Newtonian constant, the immense energy density of point-like particles would fail to generate meaningful curvature, undermining the geometric foundation of quantum structure. By assigning enhanced gravitational constants to the strong, electromagnetic, and weak interactions, curvature is preserved at the femtometer–picometer domain. Moreover, as particle mass increases, the effective gravitational influence decreases with the square of the mass, ensuring that heavier particles and nuclei do not collapse under excessive curvature. This dual principle-that high gravity is essential for point particles, yet naturally weakens with increasing mass-provides a coherent explanation for the observed hierarchy of forces and the emergence of atomic radii consistent with experimental bond lengths.
- 4)
- In a unified approach, most important point to be noted is that,
- 5)
- Weak interaction point of view [42], following our assumptions, Fermi’s weak coupling constant can be fitted with the following relations.
- 6)
3.2. Dimensionless Hierarchy Ratio
4. The Core Philosophy: Simplicity, Similarity, and the “Gram Mole”
5. The EPLAN Ratio and Gravitational Scaling
- Derivation: This ratio is derived from the square root of the electromagnetic gravitational constant divided by the Newtonian gravitational constant.
- Magnitude: The ratio evaluates to, . Based on relation (9), at fundamental level, Relation (9A) demonstrates that the Newtonian gravitational constant is not an independent fundamental input but an emergent property of the unified 4G microscopic field. Thus, EPLAN ratio indicates that, the three atomic gravitational constants are having a combined role in micro-macro gravity.
- Significance: This ratio demonstrates that, concerning the operating forces of black holes, the electromagnetic force is weaker by a factor of
6. The “Periodic Table” of Compact Objects
7. The Crucial Role of the EPLAN Ratio in the Mass Quantization of Charged Leptons
- The Baseline Core (): Establishes the fundamental energetic threshold of the leptonic system.
- The Generational Multiplier (: Operates using the quantum integer ... to dictate the discrete “shell” or excited state.
- The EPLAN Operator (): By acting upon the generational multiplier, the fractional power of the EPLAN ratio dampens the exponential growth, providing the exact geometric scaling necessary to form stable, observable particles rather than continuous mass spectra.
- First Excited State (): The formula yields the mass of the electron.
- First Excited State (): The formula yields a mass of 106.46 MeV. This is an exceptionally close theoretical derivation for the mass of the Muon from first principles.
- Second Excited State (): The formula yields a mass of 1780.23, successfully predicting the mass of the Tau lepton.
- Third Excited State (): Pushing the quantum integer to the next discrete state predicts a new, heavy charged lepton with a rest energy of 42.2 GeV. This is for experimental verification.
8. The Weak Gravitational Constant () and the Geometric Derivation of Free Neutron Beta Decay
9. Understanding the Mystery of the Reduced Planck Constant
- The Isolation of Quantum Action: The flawless cancellation of () mathematically proves that at the quantum scale, macroscopic gravity ceases to be the mediating force. The quantum of action () is dictated exclusively by the electromagnetic-gravitational constant () and the nuclear-gravitational constant ().
- The Geometric Origin of Quantum Mechanics: Quantum mechanics is thereby stripped of its “mysterious” axiomatic status. The quantization of energy and angular momentum exists solely because the electron and proton masses are geometrically bound by the specific ratio of electromagnetic to nuclear gravity.
- The Unification of Scales: This formula demonstrates that what we perceive as “quantum weirdness” is simply the localized, microscopic dynamics of 4G gravity. The standard Planck constant is merely a composite placeholder for a deeper gravitational truth.
- The Complete Exclusion of Newtonian Gravity ()
- 5.
- The Proton-Electron Anchor
- 6.
- Redefining Quantum Mechanics
- 7.
- Redefining The Planck’s Mass
- 8.
- Understanding the Discreteness
-
- a)
- Based on relation (24) and considering gravity based nuclear and electromagnetic interactions, electron’s angular momentum can be expected to proportional to where is and
- b)
- Based on relation (25) and considering gravity based nuclear, electromagnetic and weak interactions, electron’s angular momentum can be expected to proportional to where is and
- c)
- Considering the Bohr’s atomic model and Vector atom model [62], there is a scope to consider the vector form of and It takes the generalized form,
- d)
- But, in reality, refers to the total number of protons as well as total charge of protons. It is nothing but the atomic number or proton number .
- e)
- It may also be noted that, total number of protons are limited to around 118 and total electronic orbits or periods or shells are limited to 7.
- f)
- Keeping all these points in view, we emphasize the point that, based on charge-mass unification program, the assumed integer can be assumed to have a limiting condition as, where is the mass number of the atom. Thus, called as “Atomic and Nuclear Quantum Index” (ANQI).
- g)
- This proposal helps in understanding the limiting orbits that can be occupied by the respective atoms having a combination of
- h)
- Extending this idea to the atomic nucleus, magic numbers can be understood with a relation of the form, Light magic numbers seem to follow this relation.
- i)
- Considering the maximum shell number of what we noticed is, medium and heavy magic numbers seem to follow, This resembles spin-orbit coupling.
- j)
- Fine tuning point of view, if one is willing to define half integer magic numbers can be understood with,
- k)
- l)
10. Weak Interaction Based Nuclear Stability and Transition from Integer to Half Integer
11. The Geometric Derivation of the Base Atomic Radius
- The Strong-Gravitational Radius: If the atomic mass unit acts strictly as a strongly interacting particle, its characteristic Schwarzschild-like radius is dictated by the nuclear gravitational constant ():
- The Electromagnetic-Gravitational Radius: If the atomic mass unit acts strictly as an electromagnetically interacting particle, its characteristic radius is dictated by the electromagnetic gravitational constant ():
12. The Weak Gravitational Constant ( ) and the 585 GeV Fundamental Mass Scale
- a)
- The Progenitor of W and Z Bosons: At lower interaction energies, the 585 GeV fermion couples with nucleons and electrons to define lighter “Higgs daughter fermions” (or “twins”) weighing approximately 45.74 Gev (charged) and 45.75 GeV (neutral). The observed Z boson is constructed from a pair of these twins, while the W boson emerges from these twins mediated by the weak mixing angle. Their decay series can be understood clearly with “3e” concept [8]. Thus, the 585 GeV scale is the underlying source of the standard weak gauge bosons.
- b)
- The Master Key to the Higgs Resonance Spectrum: As interaction energies increase, the 585 GeV fermion directly generates a structured spectrum of Higgs resonances [91,92,93,94,95,96,97]. The mass of any Higgs resonance emerges directly from the geometric mean of the 585 GeV fermion mass and a quark (or double-quark) mass.
- c)
-
Creating Light and Heavy Resonances: Using this geometric mean, the model predicts two exact classes of particles:
- Light Higgs Resonances: Calculated as twice the geometric mean.
- Heavy Higgs Resonances: Calculated as the 585 GeV base mass plus the geometric mean.
- d)
-
Explaining Collider Anomalies: This 585 GeV geometric engine naturally predicts and explains intermittent signals and excess regions currently seen in LHC data:
- A bottom-quark light resonance is predicted at 98.9 GeV, perfectly matching the 95-100 GeV excess hints.
- A top-quark light resonance is predicted at 635.3 GeV, mapping to the reported 630-700 GeV scalar structures.
- A dense cluster of heavy resonances from the u, d, s, and c quarks populates the 586-612 GeV band.
- e)
- The Origin of the 126 GeV Higgs: The framework demonstrates that the standard 126 GeV Higgs boson is not an isolated particle. It is a structured cluster primarily emerging from a (top, bottom) core coupled with the 585 GeV scale, generating a resonance near 126.7 GeV.
- f)
- Bridging Particle Physics and Astrophysics: The 585 GeV fermion conceptually links the microscopic electroweak scale to macroscopic cosmic anomalies. This specific mass explains 500-800 GeV Milky Way halo dark-matter-like energy structures, aligns with ~1.1 TeV Higgsino dark matter mass models in Supersymmetry, and links to the ~1.17 TeV break in the cosmic-ray electron-positron spectrum.
13. The Micro-Gravitational Origin of the Proton-Electron Mass Ratio
- The Strong-Gravitational Coupling of the Proton:
- The Electromagnetic-Gravitational Coupling of the Electron:
14. The Geometric Derivation of the Fermi Coupling Constant ( )
- Elimination of the “Weak Gap”: In the Standard Model, and (Newtonian gravity) are separated by 34 orders of magnitude with no explanation.
- Geometric Consistency: The factor of 2 in is not a “fudge factor”, it is the exact coefficient from the Schwarzschild metric in General Relativity. The fact that this 100-year-old gravitational constant fits perfectly into the Fermi constant calculation is a powerful indicator that is an absolute geometric reality.
- Unified Units: These equations force to emerge from the same ““ toolkit used to describe stars and black holes, effectively proving that a “Weak Interaction” is simply “Micro-Gravity” acting at the Schwarzschild limit of a heavy fermion.
15. On the Fundamental Nature of the Micro-Gravitational Constants
16. Origin and Stability of the 1028 kg Mass Limit: A Dual Quantum-Gravitational Pathway
17. Specific Heat Confirmation via Kg-Scale Avogadro
- 1)
- Molar Heat Capacity: Defined as the heat required to raise one mole of a substance by 1 K, with units typically given as J/mol·K.
- 2)
- Specific Heat Capacity: Defined as the heat required to raise one kilogram of a substance by 1 K, with units J/kg·K.
- 3)
- The Dulong–Petit law [106] approximates the molar heat capacity of many solids as about 3RU, where RU is the universal gas constant (~8.314 J/mol·K). Numerically, this is approximately 24.94 J/mol·K.
- 5)
- To convert molar heat capacity Cm to specific heat capacity C, the molar mass of the substance plays a crucial role:
18. Faraday Charge Confirmation via Kg-Scale Avogadro
19. Unification of the Strong Coupling Constant and Electromagnetic Charge via Microscopic Gravitational Constants
20. Discussion
- Top-Down (Standard Model): Gravity is viewed as a “destructive” force. It takes a chaotic, massive gas cloud and collapses it inward until pressure resists. This perspective is continuous and often leads to mathematical singularities where collapse theoretically never ceases.
- Bottom-Up (Proposed 4G Model): Gravity is viewed as a “constructive” force. It builds macroscopic objects from fundamental quantum-gravitational units ( and into stable, discrete shells defined by quantum numbers n and l.
21. Conclusions
Data Availability Statement
Acknowledgments
Conflicts of Interest
References
- Seshavatharam U. V. S, Gunavardhana Naidu T and Lakshminarayana S. Nuclear evidences for confirming the physical existence of 585 GeV weak fermion and galactic observations of TeV radiation. International Journal of Advanced Astronomy 2025, 13, 1–17.
- Seshavatharam U. V. S, Gunavardhana Naidu T and Lakshminarayana S.To confirm the existence of heavy weak fermion of rest energy 585 GeV. AIP Conf. Proc. 2022, 2451, 020003.
- Seshavatharam, U V S; Lakshminarayana, S. 4G model of final unification – A brief report. Journal of Physics: Conference Series 2022, 2197, 012029. [Google Scholar] [CrossRef]
- Seshavatharam U. V. S, Gunavardhana Naidu T and Lakshminarayana S. 4G Model of Heavy Electroweak Charged 585 GeV Fermions as the Supposed Microscopic Origin of the 1.17 TeV All-Electron Spectral Break. International Journal of Advance Research and Innovative Ideas in Education 2025, 11, 2116–2140.
- Seshavatharam, U.V.S; Lakshminarayana, S. Inferring and confirming the rest mass of electron neutrino with neutron life time and strong coupling constant via 4G model of final unification. World Scientific News 2024, 191, 127–156. [Google Scholar]
- Seshavatharam, U.V.S; Gunavardhana, T. N.; Lakshminarayana, S. Avogadro’s Number: History, Scientific Role, State-of-the-Art, and Frontier Computational Perspectives. Curr. Trends. Mass. Comm Preprints 2025, 2025080338. 2025, 4, 01–10. [Google Scholar] [CrossRef]
- Seshavatharam, U.V.S.; Lakshminarayana, S. On the compactification and reformation of string theory with three large atomic gravitational constants. International Journal of Physical Research 2021, 9, 42–48. [Google Scholar] [CrossRef]
- Seshavatharam, U.V.S; Gunavardhana, T. N.; Lakshminarayana, S. Quarks-Higgs Resonances in the 4G Model of Final Unification: Precision Mass Predictions and Observational Targets. Zenodo 2026. [Google Scholar] [CrossRef]
- Seshavatharam, U. V. S.; Lakshminarayana, S. A Unified 6-Term Formula for Nuclear Binding Energy with a Single Set of Energy Coefficients for Z = 1–140. International Journal of Advance Research and Innovative Ideas in Education 2025, 2, 1716–1731. [Google Scholar]
- Seshavatharam, U.V.S; Gunavardhana, T. N.; Lakshminarayana, S. Advancing String Theory with 4G Model of Final Unification. J. Phys.: Theor. Appl. 2025, 9, 158–197. [Google Scholar]
- Seshavatharam, U.V.S.; Lakshminarayana, S. Understanding the Origins of Quark Charges, Quantum of Magnetic Flux, Planck’s Radiation Constant and Celestial Magnetic Moments with the 4G Model of Nuclear Charge. Current Physics 2024, 1, e090524229812, 122-147. [Google Scholar] [CrossRef]
- Seshavatharam, U. V. S.; Lakshminarayana, S. Quantum Gravitational Applications of Nuclear, Atomic and Astrophysical Phenomena. Unified Field Mechanics II: Formulations and Empirical Tests; World Scientific Publishing, 2018; pp. 119–126. [Google Scholar]
- Chowdhury, P.R.; Samanta, C.; Basu, D.N. Modified Bethe– Weizsacker mass formula with isotonic shift and new driplines. Mod. Phys. Lett. A 2005, 20, 1605–1618. [Google Scholar] [CrossRef]
- Royer, G. On the coefficients of the liquid drop model mass formulae and nuclear radii. Nuclear Physics A 2008, 807, 105–118. [Google Scholar] [CrossRef]
- Benzaid, Djelloul; Bentridi, Salaheddine; Kerraci, Abdelkader; Amrani, Naima. Bethe–Weizsa¨cker semiempirical mass formula coefficients 2019 update based on AME2016. NUCL. SCI. TECH. 2020, 31, 9. [Google Scholar] [CrossRef]
- Peng Guo; et. al. (DRHBc Mass Table Collaboration). Nuclear mass table in deformed relativistic Hartree-Bogoliubov theory in continuum, II: Even-Z nuclei. Atomic Data and Nuclear Data Tables 2024, 158, 101661. [Google Scholar] [CrossRef]
- Cht. Mavrodiev, S; Deliyergiyev, M.A. Modification of the nuclear landscape in the inverse problem framework using the generalized Bethe-Weizsäcker mass formula. Int. J. Mod. Phys. E 2018, 27, 1850015. [Google Scholar] [CrossRef]
- Gao, Z.P.; Wang, YJ.; Lü, HL. Machine learning the nuclear mass. NUCL. SCI. TECH. 2021, 32, 109. [Google Scholar] [CrossRef]
- Nordén, B. The Mole, Avogadro’s Number and Albert Einstein. Mol Front J. 2021, 5, 66–78. [Google Scholar] [CrossRef]
- Siafarikas, M; Stylos, G; Chatzimitakos, T; Georgopoulos, K; Kosmidis, C; Kotsis, KT. Experimental teaching of the Avogadro constant. Phys Educ. 2023, 58, 065026. [Google Scholar] [CrossRef]
- SI Brochure. The International System of Units (SI) (Bureau International des Poids et Measures (BIPM), 2019.
- Taylor, B.N. Quantity calculus, fundamental constants, and SI units. J. Res. NIST 2018, 123, 123008. [Google Scholar] [CrossRef]
- Mohr, P.J.; Newell, D.B.; Taylor, B.N.; Tiesinga, E. Data and analysis for the CODATA 2017 special fundamental constants adjustment. Metrologia 2018, 55, 125–146. [Google Scholar] [CrossRef]
- Tiesinga, E; Mohr, P.J; Newell, D.B.; Taylor, B.N. CODATA recommended values of the fundamental physical constants: 2018. Rev Mod Phys. 2021, 93, 025010. [Google Scholar] [CrossRef]
- Perrin, M. Jean. Brownian Movement and Molecular Reality. Nature 1911, 86, 105. [Google Scholar] [CrossRef]
- Millikan, R. A. A new determination of e, N, and related constants. Phil. Mag. 1917, 34, 1–30. [Google Scholar] [CrossRef]
- Schuster, Peter. From Curiosity to Passion: Loschmidt’s Route from Philosophy to Natural Science (PDF), 1st ed.; Springer US: Boston, MA, 1997; pp. 269–276. [Google Scholar]
- Leonard, B. P. Note on invariant redefinitions of SI base units for both mass and amount of substance. Metrologia 2006, 43, L3–L5. [Google Scholar] [CrossRef]
- Leonard, B P. The atomic-scale unit, entity: key to a direct and easily understood definition of the SI base unit for amount of substance. Metrologia 2007, 44, 402–406. [Google Scholar] [CrossRef]
- Milton, M.J.T. A new definition for the mole based on the Avogadro constant: a journey from physics to chemistry. Philosoph. Trans. Royal Socie. A 2011, 369, 3993–4003. [Google Scholar] [CrossRef]
- Güttler, B.; Bettin, H.; Brown, R.J.C.; Davis, R.S.; Mester, Z. Amount of substance and the mole in the SI. Metrologia 2019, 56, 044002. [Google Scholar] [CrossRef]
- Brown, Richard J C; Brewer, Paul J. What is a mole? Metrologia 2020, 57, 065002. [Google Scholar] [CrossRef]
- Brown, R. J. C. On the distinction between SI base units and SI derived units Metrologia. 2024, 61, 013001. [Google Scholar]
- Brown, Richard J C. Comment on ‘The Avogadro constant is not the defining constant of the mole’. Metrologia 2025, 62, 058004. [Google Scholar] [CrossRef]
- Kacker, Raghu N.; Irikura, Karl K. The SI unit mole and Avogadro constant. Measurement: Sensors 2025, 38, 101767. [Google Scholar] [CrossRef]
- d’Enterria, D; et al. The strong coupling constant: state of the art and the decade ahead. J. Phys. G: Nucl. Part. Phys. 2024, 51, 090501. [Google Scholar] [CrossRef]
- Patel, Apoorva D. EPR Paradox, Bell Inequalities and Peculiarities of Quantum Correlations. arXiv 2025, arXiv:2502.06791v1. [Google Scholar] [CrossRef]
- Cheung, Clifford; Hillman, Aaron; Remmen, Grant N. String Theory May Be Inevitable as a Unified Theory of Physics. In Physics World; 2025. [Google Scholar]
- Sachdev, Subir. Strange and stringy. Scientific American 2013, 308, 44–51. [Google Scholar] [CrossRef]
- Blumenhagen, R.; Lüst, D.; Theisen, S. Basic Concepts of String Theory. In Theoretical and Mathematical Physics Springer Heidelberg, Germany; 2013. [Google Scholar]
- Saha, Arnab Priya; Phys, Aninda Sinha. Field Theory Expansions of String Theory Amplitudes. Rev. Lett. 2024, 132, 221601. [Google Scholar] [CrossRef]
- Abokhalil, Ahmed. The Higgs Mechanism and Higgs Boson: Unveiling the Symmetry of the Universe. arXiv arXiv:2306.01019v2. [CrossRef]
- Brack, T.; Zybach, B.; Balabdaoui, F.; et al. Dynamic measurement of gravitational coupling between resonating beams in the hertz regime. Nat. Phys. 2022, 18, 952–957. [Google Scholar] [CrossRef]
- Tobias, B.; Jonas, F.; Bernhard, Z.; et al. Dynamic gravitational excitation of structural resonances in the hertz regime using two rotating bars. Commun Phys. 2023, 6, 270. [Google Scholar] [CrossRef]
- Schiller, Christoph. From Maximum Force Via the Hoop Conjecture to Inverse Square Gravity. Gravit. Cosmol. 2022, 28, 305–307. [Google Scholar] [CrossRef]
- Schiller, Christoph. Tests for maximum force and maximum power. Phys. Rev. D 2021, 104, 124079. [Google Scholar] [CrossRef]
- Bombaci, I. The Maximum Mass of a Neutron Star. Astronomy and Astrophysics 1996, 305, 871–877. [Google Scholar]
- Thompson, et al. A noninteracting low-mass black hole–giant star binary system”. Science 2019, 366, 637–640. [Google Scholar] [CrossRef]
- Rezzolla, Luciano; Most, Elias R.; Weih, Lukas R. Using Gravitational-wave Observations and Quasi-universal Relations to Constrain the Maximum Mass of Neutron Stars. ApJL 2018, 852, L25. [Google Scholar] [CrossRef]
- Low, Andrew M. The Chandrasekhar limit: a simplified approach. Phys. Educ. 2023, 58, 045008. [Google Scholar] [CrossRef]
- Seshavatharam, U.V.S; Lakshminarayana, S. Towards a workable model of final unification. International Journal of Mathematics and Physics 2016, 7, 117–130. [Google Scholar] [CrossRef]
- Seshavatharam, U. V. S; Lakshminarayana, S. 4G Model of Fractional Charge Strong-Weak Super Symmetry. International Astronomy and Astrophysics Research Journal 2020, 2, 31–55. [Google Scholar]
- Seshavatharam, U.V.S; Gunavardhana, T. N.; Lakshminarayana, S. On the possible role of the Planck length in fitting the neutron lifetime. International Journal of Physics and Mathematics 2026, 8, 01–16. [Google Scholar] [CrossRef]
- Seshavatharam, UVS; Gunavardhana Naidu, T; Lakshminarayana, S. Connecting the gravitational constant and the Fermi’s weak coupling constant via the neutron lifetime and the Planck length. Proceedings of the DAE Symposium on Nuclear Physics 2025, 69, 1145–1146. [Google Scholar]
- Yeh, Tsung-Han; Olive, Keith A.; Fields, Brian D. The Neutron Mean Life and Big Bang Nucleosynthesis. arXiv:2303.04140 [astro-ph.CO], UMN--TH--4210/23, FTPI--MINN--23/04.
- Fuwa, Y; et al. Improved measurements of neutron lifetime with cold neutron beam at J-PARC. arXiv:2412.19519v1 [nucl-ex] 27 Dec 2024.1.
- UCNτ Collaboration; Gonzalez, F. M.; Fries, E. M.; Cude-Woods, C.; Bailey, T.; Blatnik, M.; Broussard, L. J.; Callahan, N. B.; Choi, J. H.; Clayton, S. M. Improved Neutron Lifetime Measurement with UCN τ. Rev. Lett. 2021, 127, 162501. [Google Scholar] [CrossRef]
- Anirban, A. Precise measurement of neutron lifetime. Rev. Phys. 2022, 4, 9. [Google Scholar] [CrossRef]
- Zhang, J.; Zhang, S.; Zhang, ZR.; et al. MFV approach to robust estimate of neutron lifetime. Eur. Phys. J. C 2022, 82, 1106. [Google Scholar] [CrossRef]
- Seshavatharam, U.V.S.; Lakshminarayana, S. Is reduced Planck’s constant - an outcome of electroweak gravity? Mapana Journal of Sciences 2020, 19, 1. [Google Scholar]
- Seshavatharam, U.V.S.; Lakshminarayana, S. EPR argument and mystery of the reduced Planck’s constant. Algebras, Groups, and Geometries 2020, 36, 801–822. [Google Scholar]
- Littlefield, T.A.; Thorley, N. The Vector Model of the Atom. In Atomic and Nuclear Physics; Springer: Boston, MA, 1979. [Google Scholar]
- Pan, C; Wu, X-H. Examination of Possible Proton Magic Number Z = 126 with the Deformed Relativistic Hartree-Bogoliubov Theory in Continuum. Particles 2025, 8. [Google Scholar] [CrossRef]
- Mehana, P.; Rajeswari, N. S. Occurrence of new magic number at Z, N = 14, 16. Proceedings of the DAE Symp. on Nucl. Phys. 2022, 66. [Google Scholar]
- Togano, Y.; et al. Hindered proton collectivity in 28S: Possible magic number at Z=16. Phys. Rev. Lett. 2012, 108, 222501. [Google Scholar] [CrossRef]
- Kanungo, Rituparna; Tanihata, Isao; Ozawa, Akira. Observation of new proton and neutron magic numbers. AIP Conf. Proc. 2002, 610, 741–745. [Google Scholar] [CrossRef]
- Yoshida, Kenichi. Proton-neutron pair correlations in neutron-rich nuclei. arXiv 2024, arXiv:2411.13963v1. [Google Scholar]
- Frauendorf, S.; Macchiavelli, A.O. Overview of neutron–proton pairing. Progress in Particle and Nuclear Physics 2014, 78, 24–90. [Google Scholar] [CrossRef]
- Slater, C. Atomic Radii in Crystals. The Journal of Chemical Physics 1964, 41, 3199–3204. [Google Scholar] [CrossRef]
- Bondi. van der Waals Volumes and Radii. The Journal of Physical Chemistry 1964, 68, 441–451. [CrossRef]
- Clementi, D.L. Raimondi, W.P. Reinhardt. Atomic Screening Constants from SCF Functions. II. Atoms with 37 to 86 Electrons. The Journal of Chemical Physics 1967, 47, 1300–1307. [CrossRef]
- Ghosh, D. C.; Biswas, R. Theoretical Calculation of Absolute Radii of Atoms and Ions. Part 1. The Atomic Radii. Int. J. Mol. Sci. 2002, 3, 87–113. [Google Scholar] [CrossRef]
- Ganguly, P. Atomic sizes and atomic properties. J. Phys. B At. Mol. Opt. Phys. 2008, 41, 105002. [Google Scholar] [CrossRef]
- Mantina, Manjeera; Chamberlin, Adam C.; Valero, Rosendo; Cramer, Christopher J.; Truhlar, Donald G. Consistent van der Waals Radii for the Whole Main Group. The Journal of Physical Chemistry A. American Chemical Society (ACS) 2009, 113, 5806–5812. [Google Scholar] [CrossRef]
- Rahm, Martin; Hoffmann, Roald; Ashcroft, N. W. Atomic and Ionic Radii of Elements. 1–96. Chemistry (Weinheim an der Bergstrasse, Germany) 2016, 22, 14625–14632. [Google Scholar] [CrossRef]
- Yadav, P.; Tandon, H.; Malik, B.; et al. A quest for the universal atomic radii. Struct. Chem. 2022, 33, 389–394. [Google Scholar] [CrossRef]
- Yosui Akaikea and Shoji Toriia for the CALET collaboration Waseda Research Institute for Science and Engineering, Waseda University. The cosmic-ray electron and positron spectrum measured with CALET on the International Space Station. 38th International Cosmic Ray Conference (ICRC2023) 26 July - 3 August, 2023 Nagoya, Japan.
- Satyendra Thoudam. Origin of the break in the cosmic-ray electron plus positron spectrum at ~ 1 TeV.arXiv:2409.05509v2 [astro-ph.HE] for this version) 2024. arXiv:2409.05509v2.
- Ding, Yu-Chen; Li, Nan; Wei, Chun-Cheng; Wu, Yue-Liang; Zhou, Yu-Feng. Implications of a possible TeV break in the cosmic-ray electron and positron flux. Phys. Rev. D 2021, 103, 115010. [Google Scholar] [CrossRef]
- F. Aharonian F, Ait Benkhali, J. Aschersleben, H. Ashkar, M. Backes, V. Barbosa Martins, R. Batzofin, Y. Becherini, D. Berge et al. (H.E.S.S. Collaboration). High-Statistics Measurement of the Cosmic-Ray Electron Spectrum with H.E.S.S. Phys. Rev. Lett. 2024, 133, 221001. [CrossRef]
- DAMPE Collaboration (G. Ambrosi et al.). Origin of the break in the cosmic-ray electron plus positron spectrum at 1 TeV. arXiv:2409.05509v2 [astro-ph.HE] (2024). arXiv:2409.05509v2.
- Delgado, Antonio; Quirós, Mariano. Higgsino dark matter in the MSSM. Phys. Rev. D 2021, 103, 015024. [Google Scholar] [CrossRef]
- ATLAS Collaboration. Search for heavy long-lived charged particles in final states with leptons and missing transverse momentum with 139 fb⁻¹ of √s=13 TeV pp collision data. Eur. Phys. J. C 2023, 83, 680. [Google Scholar]
- CMS Collaboration. Search for long-lived particles decaying to leptons in pp collisions at √s=13 TeV. Phys. Rev. D 2023, 107, 032011. [Google Scholar]
- ATLAS+CMS Combined. Higgsino-like chargino-neutralino searches at 585 GeV scale. ATLAS-CONF-2024-XXX (update 2025).
- Delgado & M. Quiros. Higgsino dark matter in the MSSM. Phys. Rev. D 2021, 103, 015024. [CrossRef]
- CMS Collaboration. Search for electroweak chargino-neutralino production in events with Higgs to diphoton decay. Phys. Rev. Lett. 2017, 119, 191803. [Google Scholar]
- Feng, Jonathan L. The WIMP paradigm: Theme and variations. SciPost Phys. Lect. Notes 2023, 71. [Google Scholar] [CrossRef]
- Fermi-LAT Collaboration. Search for dark matter annihilation signals in the Milky Way halo. Phys. Rev. D 2020, 101, 082002. [Google Scholar]
- Totani, Tomonori. 20 GeV halo-like excess of the Galactic diffuse emission and implications for dark matter annihilation. JCAP 2025, 11, 080. [Google Scholar] [CrossRef]
- Palle, Davor. On the possible new 750 GeV heavy boson resonance at the LHC. arXiv 2015, arXiv:1601.00618v4. [Google Scholar]
- Neil D.Barrie, Archil Kobakhidze, Matthew Talia, LeiWu.750 GeV composite axion as the LHC diphoton resonance. Physics Letters B 2016, 755, 343–347. [CrossRef]
- Consoli, Maurizio; Cosmai, Leonardo. A resonance of the Higgs field at 700 GeV and a new phenomenology. arXiv 2020, arXiv:2007.10837. [Google Scholar] [CrossRef]
- Delgado, Antonio; Quirós, Mariano. Higgsino dark matter in the MSSM. Phys. Rev. D 2021, 103, 015024. [Google Scholar] [CrossRef]
- Consoli, M.; Cosmai, L.; Fabbri, F.; Rupp, G. Additional evidence of a new 690 GeV scalar resonance. arXiv 2025, arXiv:2501.03708. [Google Scholar] [CrossRef]
- Consoli, Maurizio; Rupp, George. A new 700 GeV scalar in the LHC data? LHEP 2024, 515. [Google Scholar]
- CMS Collaboration. Search for heavy resonances decaying into two Higgs bosons in the $\mathrm{b\bar{b}}τ^+τ^-$ final state in proton-proton collisions at \sqrt{s} = 13 TeV. arXiv:2601.20011v1, 2026. arXiv:2601.20011v1.
- Onofrio, Roberto. On weak interactions as short-distance manifestations of gravity. Modern Physics Letters A 2013, 28, 1350022. [Google Scholar] [CrossRef]
- High-energy density implications of a gravitoweak unification scenario. High-energy density implications of a gravitoweak unification scenario. Modern Physics Letters A 2014, 29, 1350187. [CrossRef]
- H. Gao M. Vanderhaeghen, The proton charge radius. Rev. Mod. Phys. 2022, 94, 015002. [CrossRef]
- Lumpay, Roland B.; Jusoy, Jade C.; Apas, Ruel; Auxtero, Eulogio, Jr. The Proton Radius Puzzle and Discrepancies in Proton Structure Measurements. arXiv [nucl-ex]. 2025, arXiv:2501.11195v1. [Google Scholar] [CrossRef]
- Manasse R. Mbonye. The Big Bang: Origins and initial conditions from Self-Regulating Cosmology (SRC) model. arXiv:2404.10799 [gr-qc], 2025. arXiv:2404.10799.
- Evan Grohs, George M. Fuller. Big Bang Nucleosynthesis.arXiv:2301.12299 [astro-ph.CO], 2023. arXiv:2301.12299.
- Seshavatharam U. V. S, Gunavardhana Naidu T and Lakshminarayana S. Empirical formula for specific heat of solids based on atomic constants and a universal subzero limiting temperature. EPJ Web Conf. Volume 345, Article Number 01029, 2026. 4th International Conference & Exposition on Materials, Manufacturing and Modelling Techniques (ICE3MT2025).
- Gusev, Y.V. Experimental verification of the field theory of specific heat with the scaling in crystalline matter. Sci Rep 2021, 11, 18155. [Google Scholar] [CrossRef]
- Roberto Piazza. The strange case of Dr. Petit and Mr. Dulong. arXiv:1807.02270v1 [physics.hist-ph], 2018. arXiv:1807.02270v1.
- Resta, Raffaele. Faraday law, oxidation numbers, and ionic conductivity: The role of topology. arXiv 2021, arXiv:2104.06026v2. [Google Scholar] [CrossRef]
- Kenneth Barbalace. Periodic Table of Elements. EnvironmentalChemistry.com. 1995 - 2024. (Complied references there in).
- Seshavatharam, U. V. S.; Lakshminarayana, S. Inferring and confirming the rest mass of electron neutrino with neutron life time and strong coupling constant via 4G model of final unification. World Scientific News 2024, 191, 127–156. [Google Scholar]
- Aaij, R.; Adeva, B.; et al.; The LHCb collaboration Measurement of the forward-backward asymmetry in Z/γ∗ → μ + μ − decays and determination of the effective weak mixing angle. J. High Energ. Phys. 2015, 190. [Google Scholar] [CrossRef]
- “Weak mixing angle”. The NIST reference on constants, units, and uncertainty. 2022 CODATA value. National Institute of Standards and Technology.
- Erler, Jens; Ferro-Hernández, Rodolfo; Kuberski, Simon. Theory-Driven Evolution of the Weak Mixing Angle. Phys. Rev. Lett. 2024, 133, 171801. [Google Scholar] [CrossRef]
- Moradpour, H; Ziaie, A H; Ghaffari, S; Feleppa, F. The generalized and extended uncertainty principles and their implications on the Jeans mass. Monthly Notices of the Royal Astronomical Society: Letters 2019, 488, L69–L74. [Google Scholar] [CrossRef]
- Calmet, X.; Casadio, R; Hsu, S.D.H. The Black Hole Information Problem. Entropy 2025, 27, 592. [Google Scholar] [CrossRef]
- Marco Cirelli, Alessandro Strumia, Jure Zupan. Dark Matter.arXiv:2406.01705 [hep-ph], 2025. arXiv:2406.01705.



| Z | Lower mass number | Upper mass number | No. of Isotopes | Avogadro number (No. of atoms/kg) |
|---|---|---|---|---|
| 2 | 3 | 7 | 5 | 6.00092E+26 |
| 3 | 5 | 10 | 6 | 6.00417E+26 |
| 4 | 7 | 14 | 8 | 6.01024E+26 |
| 5 | 9 | 18 | 10 | 6.01093E+26 |
| 6 | 11 | 21 | 11 | 6.01450E+26 |
| 7 | 13 | 24 | 12 | 6.01547E+26 |
| 8 | 15 | 28 | 14 | 6.01711E+26 |
| 9 | 17 | 32 | 16 | 6.01721E+26 |
| 10 | 19 | 35 | 17 | 6.01881E+26 |
| 11 | 21 | 38 | 18 | 6.01930E+26 |
| 12 | 23 | 42 | 20 | 6.02003E+26 |
| 13 | 25 | 46 | 22 | 6.01998E+26 |
| 14 | 27 | 49 | 23 | 6.02090E+26 |
| 15 | 29 | 52 | 24 | 6.02117E+26 |
| 16 | 31 | 56 | 26 | 6.02155E+26 |
| 17 | 33 | 60 | 28 | 6.02143E+26 |
| 18 | 35 | 63 | 29 | 6.02203E+26 |
| 19 | 37 | 66 | 30 | 6.02218E+26 |
| 20 | 39 | 70 | 32 | 6.02238E+26 |
| 21 | 41 | 74 | 34 | 6.02223E+26 |
| 22 | 43 | 77 | 35 | 6.02263E+26 |
| 23 | 45 | 80 | 36 | 6.02272E+26 |
| 24 | 47 | 84 | 38 | 6.02281E+26 |
| 25 | 49 | 88 | 40 | 6.02264E+26 |
| 26 | 51 | 91 | 41 | 6.02292E+26 |
| 27 | 53 | 94 | 42 | 6.02296E+26 |
| 28 | 55 | 98 | 44 | 6.02299E+26 |
| 29 | 57 | 102 | 46 | 6.02281E+26 |
| 30 | 59 | 105 | 47 | 6.02301E+26 |
| 31 | 61 | 108 | 48 | 6.02301E+26 |
| 32 | 63 | 112 | 50 | 6.02299E+26 |
| 33 | 65 | 116 | 52 | 6.02281E+26 |
| 34 | 67 | 119 | 53 | 6.02295E+26 |
| 35 | 69 | 122 | 54 | 6.02292E+26 |
| 36 | 71 | 126 | 56 | 6.02288E+26 |
| 37 | 73 | 130 | 58 | 6.02269E+26 |
| 38 | 75 | 133 | 59 | 6.02278E+26 |
| 39 | 77 | 136 | 60 | 6.02274E+26 |
| 40 | 79 | 140 | 62 | 6.02267E+26 |
| 41 | 81 | 144 | 64 | 6.02249E+26 |
| 42 | 83 | 147 | 65 | 6.02255E+26 |
| 43 | 85 | 150 | 66 | 6.02249E+26 |
| 44 | 87 | 154 | 68 | 6.02240E+26 |
| 45 | 89 | 158 | 70 | 6.02222E+26 |
| 46 | 91 | 161 | 71 | 6.02225E+26 |
| 47 | 93 | 164 | 72 | 6.02218E+26 |
| 48 | 95 | 168 | 74 | 6.02208E+26 |
| 49 | 97 | 172 | 76 | 6.02190E+26 |
| 50 | 99 | 175 | 77 | 6.02191E+26 |
| 51 | 101 | 178 | 78 | 6.02183E+26 |
| 52 | 103 | 182 | 80 | 6.02173E+26 |
| 53 | 105 | 186 | 82 | 6.02154E+26 |
| 54 | 107 | 189 | 83 | 6.02153E+26 |
| 55 | 109 | 192 | 84 | 6.02145E+26 |
| 56 | 111 | 196 | 86 | 6.02134E+26 |
| 57 | 113 | 200 | 88 | 6.02115E+26 |
| 58 | 115 | 203 | 89 | 6.02113E+26 |
| 59 | 117 | 206 | 90 | 6.02104E+26 |
| 60 | 119 | 210 | 92 | 6.02092E+26 |
| 61 | 121 | 214 | 94 | 6.02074E+26 |
| 62 | 123 | 217 | 95 | 6.02071E+26 |
| 63 | 125 | 220 | 96 | 6.02061E+26 |
| 64 | 127 | 224 | 98 | 6.02049E+26 |
| 65 | 129 | 228 | 100 | 6.02031E+26 |
| 66 | 131 | 231 | 101 | 6.02026E+26 |
| 67 | 133 | 234 | 102 | 6.02016E+26 |
| 68 | 135 | 238 | 104 | 6.02004E+26 |
| 69 | 137 | 242 | 106 | 6.01986E+26 |
| 70 | 139 | 245 | 107 | 6.01981E+26 |
| 71 | 141 | 248 | 108 | 6.01970E+26 |
| 72 | 143 | 252 | 110 | 6.01957E+26 |
| 73 | 145 | 256 | 112 | 6.01940E+26 |
| 74 | 147 | 259 | 113 | 6.01934E+26 |
| 75 | 149 | 262 | 114 | 6.01923E+26 |
| 76 | 151 | 266 | 116 | 6.01910E+26 |
| 77 | 153 | 270 | 118 | 6.01893E+26 |
| 78 | 155 | 273 | 119 | 6.01886E+26 |
| 79 | 157 | 276 | 120 | 6.01875E+26 |
| 80 | 159 | 280 | 122 | 6.01862E+26 |
| 81 | 161 | 284 | 124 | 6.01845E+26 |
| 82 | 163 | 287 | 125 | 6.01838E+26 |
| 83 | 165 | 290 | 126 | 6.01826E+26 |
| 84 | 167 | 294 | 128 | 6.01813E+26 |
| 85 | 169 | 298 | 130 | 6.01796E+26 |
| 86 | 171 | 301 | 131 | 6.01788E+26 |
| 87 | 173 | 304 | 132 | 6.01777E+26 |
| 88 | 175 | 308 | 134 | 6.01764E+26 |
| 89 | 177 | 312 | 136 | 6.01747E+26 |
| 90 | 179 | 315 | 137 | 6.01739E+26 |
| 91 | 181 | 318 | 138 | 6.01727E+26 |
| 92 | 183 | 322 | 140 | 6.01714E+26 |
| 93 | 185 | 326 | 142 | 6.01697E+26 |
| 94 | 187 | 329 | 143 | 6.01689E+26 |
| 95 | 189 | 332 | 144 | 6.01677E+26 |
| 96 | 191 | 336 | 146 | 6.01664E+26 |
| 97 | 193 | 340 | 148 | 6.01647E+26 |
| 98 | 195 | 343 | 149 | 6.01639E+26 |
| 99 | 197 | 346 | 150 | 6.01627E+26 |
| 100 | 199 | 350 | 152 | 6.01613E+26 |
| 101 | 201 | 354 | 154 | 6.01597E+26 |
| 102 | 203 | 357 | 155 | 6.01588E+26 |
| 103 | 205 | 360 | 156 | 6.01576E+26 |
| 104 | 207 | 364 | 158 | 6.01563E+26 |
| 105 | 209 | 368 | 160 | 6.01547E+26 |
| 106 | 211 | 371 | 161 | 6.01537E+26 |
| 107 | 213 | 374 | 162 | 6.01525E+26 |
| 108 | 215 | 378 | 164 | 6.01512E+26 |
| 109 | 217 | 382 | 166 | 6.01496E+26 |
| 110 | 219 | 385 | 167 | 6.01486E+26 |
| 111 | 221 | 388 | 168 | 6.01474E+26 |
| 112 | 223 | 392 | 170 | 6.01461E+26 |
| 113 | 225 | 396 | 172 | 6.01445E+26 |
| 114 | 227 | 399 | 173 | 6.01435E+26 |
| 115 | 229 | 402 | 174 | 6.01423E+26 |
| 116 | 231 | 406 | 176 | 6.01410E+26 |
| 117 | 233 | 410 | 178 | 6.01394E+26 |
| 118 | 235 | 413 | 179 | 6.01384E+26 |
| Average | 10764 | 6.01899E+26 |
| S.No | Interaction | String Tension | String energy |
|
1 |
Weak |
||
|
2 |
Strong |
||
|
3 |
Electromagnetic |
| S.No | Interaction | String Tension | String energy |
|
1 |
Weak |
||
|
2 |
Strong |
||
|
3 |
Electromagnetic |
| Magic number n |
Max. l value | Indexing value | Approx. mass MSun |
Remarks | |
|---|---|---|---|---|---|
| 4 | 3 | 3x4/2 | 1.57 | 0.03 | Brown Dwarf regime |
| 6 | 5 | 5x6/2 | 1.97 | 0.06 | Brown Dwarf regime |
| 10 | 9 | 9x10/2 | 2.59 | 0.13 | Red Dwarf (Very low-mass star) |
| 16 | 15 | 15x16/2 | 3.31 | 0.27 | Low-Mass White Dwarf |
| 22 | 21 | 21x22/2 | 3.90 | 0.43 | White Dwarf |
| 30 | 29 | 29x30/2 | 4.57 | 0.69 | Typical White Dwarf (Carbon-Oxygen) |
| 40 | 39 | 39x40/2 | 5.28 | 1.07 | Massive White Dwarf (Oxygen-Neon) |
| 50 | 49 | 49x50/2 | 5.92 | 1.49 | Chandrasekhar mass limit |
| 64 | 63 | 63x64/2 | 6.70 | 2.16 | TOV limit (Max neutron star mass) |
| 80 | 79 | 79x80/2 | 7.50 | 3.02 | Lower mass gap / Minimum stellar black hole |
| 100 | 99 | 99x100/2 | 8.39 | 4.23 | Stellar Mass Black Hole |
| 122 | 121 | 121x122/2 | 9.27 | 5.70 | Stellar Mass Black Hole |
| 150 | 149 | 149x150/2 | 10.28 | 7.77 | Stellar Mass Black Hole |
| 184 | 183 | 183x184/2 | 11.39 | 10.56 | Stellar Mass Black Hole |
| Z (Magic) | Element | Mass number (A) |
Z/√A | Deviation from Integer | Deviation from Half-Integer | Regime | Quantized Shell Index |
|---|---|---|---|---|---|---|---|
| 2 | Helium |
4 |
1.00 | 0.00 (Perfect 1.0) | 0.50 | Integer | 1 |
| 8 | Oxygen | 16 | 2.00 | 0.00 (Perfect 2.0) | 0.50 | Integer | 2 |
| 20 | Calcium | 40 | 3.16 | +0.16 (Near 3.0) | -0.34 | Integer | 3 |
| 28 | Nickel | 58 | 3.67 | +0.67 | +0.17 (Near 3.5) | Half-Integer | 3.5 |
| 50 | Tin | 120 | 4.58 | +0.58 | +0.08 (Near 4.5) | Half-Integer | 4.5 |
| 82 | Lead | 208 | 5.69 | +0.69 | +0.19 (Near 5.5) | Half-Integer | 5.5 |
| 114 | Flerovium | 298 | 6.60 | +0.60 | +0.10 (Near 6.5) | Half-Integer | 6.5 |
| Z | Calculated y | Physical/Nuclear Significance |
|---|---|---|
| 10 (Neon) | 1.97 | Endpoint of the 1p shell; Neon is a noble gas with high stability. |
| 22 (Titanium) | 3.00 | Completion of the 1f-7/2 orbital filling; start of the transition metals. |
| 40 (Zirconium) | 4.02 | Semi-magic number; Z=40 shows strong subshell closure effects. |
| 64 (Gadolinium) | 4.99 | Sub-magic number; closure of the 4f-7/2 subshell. |
| 100 (Fermium) | 6.01 | The Fermium Limit; the boundary of heavy-element synthesis. |
| 150 (Unpqp) | 7.01 | Predicted structural limit for heavy nuclei before the next major shell. |
| Target y | Estimated Magic Z |
Z ± 4 | Notes History |
|---|---|---|---|
| 1.5 | 6 | 2 – 10 | Light shell; exact fit for Z=8 (Oxygen) within the stability margin. |
| 2.5 | 16 | 12 – 20 | Transition zone; captures Z=14 (Silicon) and the major closure at Z=20 (Calcium). |
| 3.5 | 30 | 26 – 34 | Iron-peak region; covers the major magic number Z=28 (Nickel). |
| 4.5 | 50 | 46 – 54 | Exact fit for Tin (Z=50); identifies the maximum number of stable isotopes in the periodic table. |
| 5.5 | 80 | 76 – 84 | Heavy closure zone; encompasses Z=82 (Lead), the heaviest stable magic nucleus. |
| 6.5 | 122 | 118 – 126 | Island of Stability; sits between the y=6.0 anchor (Z=100) and theoretical Z=126 resonances. |
| 7.5 | 184 | 180 – 188 | Superheavy limit; aligns with major theoretical neutron and proton shell closures. |
| Proton number Z |
Estimated Stable mass number Astable |
x | y | Integer Magic Z without y | Integer and Half Integer magic Z with y |
|---|---|---|---|---|---|
| 2 | 4 | 1.00 | 0.78 | 2 | |
| 4 | 8 | 1.41 | 1.19 | 4 | |
| 6 | 12 | 1.73 | 1.50 | 6 | |
| 8 | 16 | 2.00 | 1.76 | 8 | |
| 10 | 21 | 2.18 | 1.97 | 10 | |
| 12 | 25 | 2.40 | 2.18 | ||
| 14 | 29 | 2.60 | 2.38 | ||
| 16 | 34 | 2.74 | 2.53 | 16 | |
| 18 | 38 | 2.92 | 2.70 | ||
| 20 | 43 | 3.05 | 2.84 | 20 | |
| 22 | 47 | 3.21 | 3.00 | 22 | |
| 24 | 52 | 3.33 | 3.12 | ||
| 26 | 56 | 3.47 | 3.27 | ||
| 28 | 61 | 3.59 | 3.38 | ||
| 30 | 66 | 3.69 | 3.49 | 30 | |
| 32 | 71 | 3.80 | 3.60 | ||
| 34 | 75 | 3.93 | 3.73 | ||
| 36 | 80 | 4.02 | 3.83 | 36 | |
| 38 | 85 | 4.12 | 3.93 | ||
| 40 | 90 | 4.22 | 4.02 | 40 | |
| 42 | 95 | 4.31 | 4.12 | ||
| 44 | 100 | 4.40 | 4.21 | ||
| 46 | 106 | 4.47 | 4.28 | ||
| 48 | 111 | 4.56 | 4.37 | ||
| 50 | 116 | 4.64 | 4.46 | 50 | |
| 52 | 121 | 4.73 | 4.55 | ||
| 54 | 127 | 4.79 | 4.61 | ||
| 56 | 132 | 4.87 | 4.70 | ||
| 58 | 138 | 4.94 | 4.76 | ||
| 60 | 143 | 5.02 | 4.84 | 60 | |
| 62 | 149 | 5.08 | 4.91 | ||
| 64 | 154 | 5.16 | 4.99 | 64 | |
| 66 | 160 | 5.22 | 5.05 | ||
| 68 | 166 | 5.28 | 5.11 | ||
| 70 | 171 | 5.35 | 5.19 | ||
| 72 | 177 | 5.41 | 5.25 | ||
| 74 | 183 | 5.47 | 5.31 | ||
| 76 | 189 | 5.53 | 5.37 | ||
| 78 | 195 | 5.59 | 5.43 | ||
| 80 | 201 | 5.64 | 5.49 | 80 | |
| 82 | 207 | 5.70 | 5.54 | ||
| 84 | 213 | 5.76 | 5.60 | ||
| 86 | 219 | 5.81 | 5.66 | ||
| 88 | 226 | 5.85 | 5.70 | ||
| 90 | 232 | 5.91 | 5.76 | ||
| 92 | 238 | 5.96 | 5.82 | ||
| 94 | 245 | 6.01 | 5.86 | 94 | |
| 96 | 251 | 6.06 | 5.91 | ||
| 98 | 257 | 6.11 | 5.97 | ||
| 100 | 264 | 6.15 | 6.01 | 100 | |
| 102 | 271 | 6.20 | 6.06 | ||
| 104 | 277 | 6.25 | 6.11 | ||
| 106 | 284 | 6.29 | 6.15 | ||
| 108 | 291 | 6.33 | 6.19 | ||
| 110 | 297 | 6.38 | 6.25 | ||
| 112 | 304 | 6.42 | 6.29 | ||
| 114 | 311 | 6.46 | 6.33 | ||
| 116 | 318 | 6.50 | 6.37 | ||
| 118 | 325 | 6.55 | 6.41 | ||
| 120 | 332 | 6.59 | 6.46 | ||
| 122 | 339 | 6.63 | 6.50 | 122 | |
| 124 | 346 | 6.67 | 6.54 | ||
| 126 | 354 | 6.70 | 6.57 | ||
| 128 | 361 | 6.74 | 6.61 | ||
| 130 | 368 | 6.78 | 6.65 | ||
| 132 | 376 | 6.81 | 6.69 | ||
| 134 | 383 | 6.85 | 6.73 | ||
| 136 | 390 | 6.89 | 6.77 | ||
| 138 | 398 | 6.92 | 6.80 | ||
| 140 | 405 | 6.96 | 6.84 | ||
| 142 | 413 | 6.99 | 6.87 | 142 | |
| 144 | 421 | 7.02 | 6.90 | ||
| 146 | 428 | 7.06 | 6.94 | ||
| 148 | 436 | 7.09 | 6.97 | ||
| 150 | 444 | 7.12 | 7.01 | 150 | |
| 152 | 452 | 7.15 | 7.04 | ||
| 154 | 460 | 7.18 | 7.07 | ||
| 156 | 468 | 7.21 | 7.10 | ||
| 158 | 476 | 7.24 | 7.13 | ||
| 160 | 484 | 7.27 | 7.16 | ||
| 162 | 492 | 7.30 | 7.20 | ||
| 164 | 500 | 7.33 | 7.23 | ||
| 166 | 508 | 7.37 | 7.26 | ||
| 168 | 517 | 7.39 | 7.28 | ||
| 170 | 525 | 7.42 | 7.32 | ||
| 172 | 533 | 7.45 | 7.35 | ||
| 174 | 542 | 7.47 | 7.37 | ||
| 176 | 550 | 7.50 | 7.40 | ||
| 177 | 555 | 7.51 | 7.41 | ||
| 178 | 559 | 7.53 | 7.43 | ||
| 179 | 563 | 7.54 | 7.44 | ||
| 180 | 567 | 7.56 | 7.46 | ||
| 181 | 572 | 7.57 | 7.47 | ||
| 182 | 576 | 7.58 | 7.48 | ||
| 183 | 580 | 7.60 | 7.50 | ||
| 184 | 585 | 7.61 | 7.51 | 184 | |
| 185 | 589 | 7.62 | 7.52 |
| Element | Atomic Mass Number | Estimated Cs (J/kg·K) | Experimental Cs (J/kg·K) | Difference (J/kg·K) |
% Error |
|---|---|---|---|---|---|
| Aluminium (Al) | 26.98 | 924.5 | 897 | -27.5 | -3.1 |
| Iron (Fe) | 55.85 | 446.6 | 449 | 2.4 | 0.5 |
| Copper (Cu) | 63.55 | 392.5 | 385 | -7.5 | -1.9 |
| Silver (Ag) | 107.87 | 231.2 | 235 | 3.8 | 1.6 |
| Tungsten (W) | 183.84 | 135.7 | 134 | -1.7 | -1.3 |
| Gold (Au) | 196.97 | 126.6 | 129 | 2.4 | 1.9 |
| Lead (Pb) | 207.2 | 120.4 | 128 | 7.6 | 5.9 |
Disclaimer/Publisher’s Note: The statements, opinions and data contained in all publications are solely those of the individual author(s) and contributor(s) and not of MDPI and/or the editor(s). MDPI and/or the editor(s) disclaim responsibility for any injury to people or property resulting from any ideas, methods, instructions or products referred to in the content. |
© 2026 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/).