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Journal articles on the topic 'Effective nuclear charge'

Author: Grafiati

Published: 5 June 2025

Last updated: 2 August 2025

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1

Robson, Fernandes de Farias. "Atomic Radii based on Effective Nuclear Charge." Chemistry Research Journal 4, no. 4 (2019): 1–6. https://doi.org/10.5281/zenodo.13310958.

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In the present work, a set of atomic radii are provided (from hydrogen to radon). Such values were calculated by using Clementi effective nuclear charges [3,4].The obtained atomic radii were compared with van der Walls atomic radii [1] as well as the Rahm-Hoffmann-Ashcroft  values [2]. The obtained results confirm a crossroad position for cerium in the periodic tableas previously proposed [6].

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2

Ohwada, Ken. "The effective nuclear charge model—IX. On the transferability of effective nuclear charges defined from homonuclear diatomic molecules." Spectrochimica Acta Part A: Molecular Spectroscopy 43, no. 9 (1987): 1147–50. http://dx.doi.org/10.1016/0584-8539(87)80032-6.

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3

Gornostaeva, O. V., R. Y. Babkin, K. V. Lamonova, S. M. Orel, and Yu G. Pashkevich. "Effective nuclear charge approximation for free rare-earth ions." Spectroscopy Letters 50, no. 9 (2017): 482–88. http://dx.doi.org/10.1080/00387010.2017.1360359.

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4

Zawischa, D., U. Regge, and R. Stapel. "Effective interaction and the staggering of nuclear charge radii." Physics Letters B 185, no. 3-4 (1987): 299–303. http://dx.doi.org/10.1016/0370-2693(87)91003-3.

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5

BARTEL, J., G. WENES, M. WAROQUIER, and J. RYCKEBUSCH. "CHARGE DENSITY DIFFERENCES AND THE NUCLEAR INCOMPRESSIBILITY." Modern Physics Letters A 01, no. 09 (1986): 509–15. http://dx.doi.org/10.1142/s0217732386000646.

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The influence of the nuclear matter compression modulus K∞ on the difference in the charge density distribution of 208 Pb −206 Pb is investigated in a self-consistent mean field approach with a variety of density dependent effective interactions of the generalized Skyrme type. It is found that in addition to a dependence on the compressibility associated with a given Skyrme force the results also depend strongly on the pairing correlations which, through the level density, are influenced by the nuclear matter effective mass.

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6

Sun, Bao-Xi, Xiao-Fu Lu, Peng-Nian Shen, and En-Guang Zhao. "Effective Photon Mass in Nuclear Matter and Finite Nuclei." Modern Physics Letters A 18, no. 21 (2003): 1485–92. http://dx.doi.org/10.1142/s0217732303011332.

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Electromagnetic field in nuclear matter and nuclei are studied. In the nuclear matter, because the expectation value of the electric charge density operator is not zero, different in vacuum, the U(1) local gauge symmetry of electric charge is spontaneously broken, and consequently, the photon gains an effective mass through the Higgs mechanism. An alternative way to study the effective mass of photon is to calculate the self-energy of photon perturbatively. It shows that the effective mass of photon is about 5.42 MeV in the symmetric nuclear matter at the saturation density ρ0 = 0.16 fm -3 and

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7

Cui, Z. F., J. L. Zhang, D. Binosi, et al. "Effective charge from lattice QCD." Chinese Physics C 44, no. 8 (2020): 083102. http://dx.doi.org/10.1088/1674-1137/44/8/083102.

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8

Khadikar, Padmaker V., and Sadhana Pandharkar. "The Edge Shift, Effective Nuclear Charge and Coordination Stoichiometry: A Novel Correlation." Japanese Journal of Applied Physics 27, Part 1, No. 12 (1988): 2183–86. http://dx.doi.org/10.1143/jjap.27.2183.

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9

Khadikar, P. V., and S. P. Pandharkar. "Co-ordination stoichiometry, edge shift and effective nuclear charge: A novel correlation." Il Nuovo Cimento D 8, no. 1 (1986): 33–38. http://dx.doi.org/10.1007/bf02450464.

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10

Rios, L. A., P. K. Shukla, and A. Serbeto. "Neutrino effective charge in a dense Fermi plasma." Physics Letters B 657, no. 1-3 (2007): 154–58. http://dx.doi.org/10.1016/j.physletb.2007.10.009.

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11

Ershov, D. K. "Dynamic Mapping of Effective Nuclear Charge for 1S1/2-Shell Electrons and Nominal Nuclear Charge for Heavy Element Atoms with 10 ≤ Z ≤ 173." Russian Physics Journal 63, no. 7 (2020): 1299–300. http://dx.doi.org/10.1007/s11182-020-02144-x.

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12

Ermakov, A. I. "Calculating the effective nuclear charge for a slater orbital from physical screening concepts." Journal of Structural Chemistry 32, no. 4 (1992): 455–61. http://dx.doi.org/10.1007/bf00753020.

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13

Peter, Th. "Scaling laws for the effective charge of heavy ions penetrating gas or plasma targets." Laser and Particle Beams 8, no. 4 (1990): 643–58. http://dx.doi.org/10.1017/s026303460000906x.

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Until now a theoretical derivation of scaling laws for the effective charge Zeff of heavy ions penetrating matter has been lacking, although for cold gaseous targets there are well-established empirical relations of the form Zeff/Zp = f (up/ZpγZtδ), where vp and Zp are, respectively, the velocity and nuclear charge of the projectile ion, Zt, is the nuclear charge of the target atoms, and γ and δ are the scaling exponents. We show that the scaling exponents may be derived from an investigation of loss and capture rates. The treatment is based on the Bohr-Lamb criterion. This very crude criterio

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14

Binosi, D., and J. Papavassiliou. "The QCD effective charge to all orders." Nuclear Physics B - Proceedings Supplements 121 (June 2003): 281–84. http://dx.doi.org/10.1016/s0920-5632(03)01862-0.

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15

Xu, Zhangbu. "High-pTidentified particle spectra—the effective color-charge factor." Journal of Physics G: Nuclear and Particle Physics 35, no. 10 (2008): 104009. http://dx.doi.org/10.1088/0954-3899/35/10/104009.

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16

Ferreira, P. M. "A full one-loop charge symmetry breaking effective potential." Physics Letters B 509, no. 1-2 (2001): 120–30. http://dx.doi.org/10.1016/s0370-2693(01)00552-4.

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17

T Whelan, Colm, HRJ Walters, J. Hansen, and RM Dreizler. "High Energy Electron Impact Ionisation of H(1s) in Coplanar Asymmetric Geometry." Australian Journal of Physics 44, no. 1 (1991): 39. http://dx.doi.org/10.1071/ph910039.

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Various effective charge approximations are explored for the high energy electron impact ionisation of H(ls) in coplanar asymmetric geometry, using a first order perturbative model. Our results are compared with other more sophisticated calculations and with experiment. It is found that effective charge prescriptions satisfying the requirement that, in the limit of zero ejection energy, the escaping electron sees the full nuclear charge while the scattered electron is totally screened, are unsuccessful. In contrast it is found that the Coulomb projected Born exchange approximation, where both

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18

Robson, Fernandes de Farias. "What is the polarizability of element 119?" Chemistry Research Journal 3, no. 1 (2018): 113–17. https://doi.org/10.5281/zenodo.13925692.

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In the present work, an extrapolation approach is employed to calculate the polarizability (10<sup>-24</sup>cm<sup>3</sup>) for element 119, from the absolute hardness for the cation 119<sup>+</sup>. The calculated value: 67.49, is in total disagreement with the value calculated by using sophisticated relativistic quantum chemical approach [7], 25.12 (or 169.7, in atomic units). It is considered here that the relativistic effects, for element 119 (of course, regarding polarizability), in such calculations [7-9], have been overestimated, and that the value obtained by extrapolation is the relia

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19

KREBS, H., E. EPELBAUM, and ULF-G. MEIßNER. "CHIRAL EFFECTIVE POTENTIAL WITH DELTA DEGREES OF FREEDOM." International Journal of Modern Physics A 24, no. 02n03 (2009): 511–14. http://dx.doi.org/10.1142/s0217751x09043961.

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Using chiral effective field theory (EFT) with explicit Δ degrees of freedom we calculated nuclear forces up to next-to-next-to-leading order (NNLO). We found much better convergence of the chiral expansion in all peripheral partial waves. We also observe strong cancellations between charge-symmetry-breaking (CSB) contributions due to nucleon- and Δ-mass splittings in the two-pion-exchange potentials. The CSB potentials appear to be weaker in the Δ-full theory.

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20

PÉREZ-GARCÍA, M. ÁNGELES. "CHARGE DISTRIBUTION AND RADII IN CLUSTERS FROM NUCLEAR PASTA MODELS." International Journal of Modern Physics E 19, no. 07 (2010): 1477–89. http://dx.doi.org/10.1142/s0218301310015886.

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We study the consistency of the description of charge distributions and radii of nuclear clusters obtained with semiclassical nuclear pasta models. These nuclei are expected to exist in the low density outer crust of neutron stars. Properties of the arising clusterized nucleon matter can be compared to realistic nuclear properties as experimentally extracted on earth. We focus on non iso-symmetric light clusters with nucleon number 8 ≤ A ≤ 30 and use Monte Carlo many-body techniques. We simulate isotopic chains for a set of selected nuclei using a model Hamiltonian consisting of the usual kine

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21

Gnech, Alex, Jordy de Vries, Sachin Shain, and Michele Viviani. "Electric dipole moment of light nuclei in chiral effective field theory." EPJ Web of Conferences 258 (2022): 06007. http://dx.doi.org/10.1051/epjconf/202225806007.

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CP-violating interactions at quark level generate CP-violating nuclear interactions and currents, which could be revealed by looking at the presence of a permanent nuclear electric dipole moment. Within the framework of chiral effective field theory, we discuss the derivation of the CP-violating nuclear potential up to next-to-next-to leading order (N2LO) and the preliminary results for the charge operator up to next-to leading order (NLO). Moreover, we introduce some renormalization argument which indicates that we need to promote the short-distance operator to the leading order (LO) in order

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22

Ohwada, Ken. "Energetic consideration of the vibrational potential function in the effective nuclear charge model. V." Journal of Chemical Physics 84, no. 3 (1986): 1670–76. http://dx.doi.org/10.1063/1.450463.

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23

Ohwada, Ken. "Energetic consideration of the vibrational potential function in the effective nuclear charge model. VI." Journal of Chemical Physics 85, no. 10 (1986): 5882–89. http://dx.doi.org/10.1063/1.451550.

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24

Ohwada, Ken. "Energetic consideration of the vibrational potential function in the effective nuclear charge model. VII." Journal of Chemical Physics 87, no. 8 (1987): 4727–35. http://dx.doi.org/10.1063/1.452837.

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25

Sala, O., Koiti Araki, and L. K. Noda. "A Procedure to Obtain the Effective Nuclear Charge from the Atomic Spectrum of Sodium." Journal of Chemical Education 76, no. 9 (1999): 1269. http://dx.doi.org/10.1021/ed076p1269.

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26

Ohwada, Ken. "Energetic consideration of the vibrational potential function in the effective nuclear charge model. IV." Journal of Chemical Physics 82, no. 2 (1985): 860–67. http://dx.doi.org/10.1063/1.448513.

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27

Zamick, L. "The average monopole polarization charge and its relation to nuclear incompressibility and effective mass." Zeitschrift f�r Physik A Atomic Nuclei 327, no. 4 (1987): 409–12. http://dx.doi.org/10.1007/bf01289566.

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28

Ohwada, Ken. "Energetic consideration of the vibrational potential function in the effective nuclear charge model—VIII." Spectrochimica Acta Part A: Molecular Spectroscopy 44, no. 8 (1988): 809–17. http://dx.doi.org/10.1016/0584-8539(88)80147-8.

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29

Cai, X., X. M. Chen, Z. Y. Liu, et al. "The effective charge effect in partially stripped ion-helium collisions." Zeitschrift für Physik A Hadrons and Nuclei 355, no. 4 (1996): 439–42. http://dx.doi.org/10.1007/s002180050135.

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30

Cai, X., X. M. Chen, Z. Y. Liu, et al. "The effective charge effect in partially stripped ion-helium collisions." Zeitschrift für Physik A: Hadrons and Nuclei 355, no. 1 (1996): 439–42. http://dx.doi.org/10.1007/bf02769721.

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31

Ojovan, Michael I., Boris E. Burakov, and William E. Lee. "Destruction of Micro-crystal Containing Wasteforms by Charge-induced Crystal Shape Change on Self-irradiation." MRS Advances 2, no. 11 (2016): 621–26. http://dx.doi.org/10.1557/adv.2016.655.

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ABSTRACTMechanical damage of non-metallic nuclear wasteforms can be caused by electrical fields induced by decaying clusters of radionuclides surrounded by an insulating matrix. We assess the electric fields near clusters with decaying radionuclides 244Cm, 241Am, 238,239Pu and 137Cs in a glass matrix determining that matrix destruction can gradually occur via electric breakdown discharges and diffusion-controlled change in form of clusters. The most important parameters that control potential matrix destruction are the radioactive cluster (inhomogeneity) size, radionuclide specific radioactivi

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32

SESHAVATHARAM, U. V. S., and S. LAKSHMINARAYANA. "SUPER SYMMETRY IN STRONG AND WEAK INTERACTIONS." International Journal of Modern Physics E 19, no. 02 (2010): 263–80. http://dx.doi.org/10.1142/s021830131001473x.

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For strong interaction two new fermion mass units 105.32 MeV and 11450 MeV are assumed. Existence of "Integral charge quark bosons", "Integral charge effective quark fermions", "Integral charge (effective) quark fermi-gluons" and "Integral charge quark boso-gluons" are assumed and their masses are estimated. It is noticed that, characteristic nuclear charged fermion is Xs · 105.32 = 938.8 MeV and corresponding charged boson is Xs(105.32/x) = 415.0 where Xs = 8.914 is the inverse of the strong coupling constant and x = 2.26234 is a new number by using which "super symmetry" can be seen in "stro

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33

Sigmund, Peter, and Andreas Schinner. "Effective charge and related/unrelated quantities in heavy-ion stopping." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 174, no. 4 (2001): 535–40. http://dx.doi.org/10.1016/s0168-583x(01)00317-2.

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34

Ho, Y. K., and C. Coceva. "Nucleon effective charge in E1 and E2 radiative transitions." Journal of Physics G: Nuclear Physics 14, S (1988): S207—S214. http://dx.doi.org/10.1088/0305-4616/14/s/022.

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35

Udema, Ikechukwu. "Fine Structure Constant is Related to Effective Nuclear Charge and Bohr’s Radius for Any Atom." Asian Journal of Physical and Chemical Sciences 3, no. 4 (2017): 1–8. http://dx.doi.org/10.9734/ajopacs/2017/36931.

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36

Babkin, R. Yu, K. V. Lamonova, S. M. Orel, and Yu G. Pashkevich. "Determination of the effective nuclear charge for free ions of transition metals from experimental spectra." Optics and Spectroscopy 107, no. 1 (2009): 9–15. http://dx.doi.org/10.1134/s0030400x09070029.

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37

Babkin, R. Yu, K. V. Lamonova, S. M. Orel, Yu G. Pashkevich, and V. F. Meshcheryakov. "Determination of the effective nuclear charge from EPR data using a modified crystal-field theory." Optics and Spectroscopy 112, no. 3 (2012): 438–42. http://dx.doi.org/10.1134/s0030400x12020051.

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38

Luna, E. G. S., A. L. dos Santos, and A. A. Natale. "QCD effective charge and the structure function F2 at small-x." Physics Letters B 698, no. 1 (2011): 52–58. http://dx.doi.org/10.1016/j.physletb.2011.02.057.

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39

Binosi, D., J. Bernabéu, and J. Papavassiliou. "The effective neutrino charge radius in the presence of fermion masses." Nuclear Physics B 716, no. 1-2 (2005): 352–72. http://dx.doi.org/10.1016/j.nuclphysb.2005.02.039.

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40

Tsvetkov, I. V., and T. Tanabe. "The effective secondary electron yield in the space-charge limited condition." Journal of Nuclear Materials 258-263 (October 1998): 927–33. http://dx.doi.org/10.1016/s0022-3115(98)00312-2.

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41

GAMBOA, J., J. LÓPEZ-SARRIÓN, M. LOEWE, and F. MÉNDEZ. "CENTRAL CHARGES AND EFFECTIVE ACTION AT FINITE TEMPERATURE AND DENSITY." Modern Physics Letters A 19, no. 03 (2004): 223–38. http://dx.doi.org/10.1142/s0217732304012952.

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The current algebra for gauge theories like QCD at finite temperature and density is studied. We start considering, the massless Thirring model at finite temperature and density, finding an explicit expression for the current algebra. The central charge only depends on the coupling constant and there are not new effects due to temperature and density. From this calculation, we argue how to compute the central charge for QCD4 and we argue why the central charge in four dimensions could be modified by finite temperature and density.

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42

FAGHIHI, F., and M. R. ESKANDARI. "NUCLEAR FUSION RATE STUDY OF A MUONIC MOLECULE VIA NUCLEAR THRESHOLD RESONANCES." International Journal of Modern Physics E 14, no. 08 (2005): 1213–21. http://dx.doi.org/10.1142/s0218301305003818.

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This work follows our previous calculations of the ground state binding energy, size, and the effective nuclear charge of the muonic T3 molecule, using the Born–Oppenheimer adiabatic approximation. In our past articles, we showed that the system possesses two minimum positions, the first one at the muonic distance and the second at the atomic distance. Also, the symmetric planner vibrational model assumed between the two minima and the approximated potential were calculated. Following from the previous studies, we now calculate the fusion rate of the T3 muonic molecule according to the overlap

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43

Choudhary, Shalini, Prabhat Ranjan, and Tanmoy Chakraborty. "Atomic polarizability: A periodic descriptor." Journal of Chemical Research 44, no. 3-4 (2019): 227–34. http://dx.doi.org/10.1177/1747519819889936.

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Atomic polarizability is an essential theoretical construct to define and correlate many physicochemical properties. It exhibits periodicity and has a relationship with other periodic descriptors. Although a number of scales are available to compute atomic polarizability, the final scale is yet to be designed. In this venture, we have invoked a new empirical approach to compute the atomic polarizability of 103 elements of the periodic table, considering the conjoint action of other periodic descriptors, namely effective nuclear charge (Zeff) and absolute radii (r). The proposed approach is [Fo

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44

DEXHEIMER, VERÔNICA A., CÉSAR A. Z. VASCONCELLOS, MOISÉS RAZEIRA, and MANFRED DILLIG. "THE ROLE OF THE NUCLEAR MATTER COMPRESSION MODULUS IN NEUTRON STARS." International Journal of Modern Physics D 13, no. 07 (2004): 1519–24. http://dx.doi.org/10.1142/s0218271804005754.

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For the nuclear many body problem at high densities, formulated in the framework of a relativistic mean-field theory, we investigate in detail the compression modulus of nuclear matter as a function of the effective nucleon mass. We include consistently in our modelling chemical equilibrium as well as baryon number and electric charge conservation and investigate properties of neutron stars. Among other predictions we focus on the dependence of the maximum mass of a sequence of neutron stars as a function of the compression modulus and the nucleon effective mass.

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45

Brown, B. Alex. "The Nuclear Shell Model towards the Drip Lines." Physics 4, no. 2 (2022): 525–47. http://dx.doi.org/10.3390/physics4020035.

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Applications of configuration-mixing methods for nuclei near the proton and neutron drip lines are discussed. A short review of magic numbers is presented. Prospects for advances in the regions of four new “outposts” are highlighted: 28O, 42Si, 60Ca and 78Ni. Topics include shell gaps, single-particle properties, islands of inversion, collectivity, neutron decay, neutron halos, two-proton decay, effective charge, and quenching in knockout reactions.

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46

Hasan, A. K., and H. H. Abed. "Study of the nuclear structure for the 18O by using NuShellX@MSU code." Nuclear Physics and Atomic Energy 24, no. 3 (2023): 219–24. http://dx.doi.org/10.15407/jnpae2023.03.219.

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In this study, the energy levels, electromagnetic transition probability, and charge density distribution of the 18O nucleus were calculated using the NuShellX@MSU code within the sdpn-shell and using the effective USDEPN and WCPN interactions. The charge density distribution values were also reasonably consistent with existing experimental data. Comparing the theoretical and experimental results indicates that applying the nuclear shell model using the USDEPN and WCPN interactions is successful within the sdpn-shell.

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47

Ochala, Isaiah. "Probing nuclear equation of state with the cdm3y version of B3y-fetal effective interaction." International Journal of Physics Research and Applications 6, no. 1 (2023): 098–114. http://dx.doi.org/10.29328/journal.ijpra.1001057.

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This paper is a study of the nuclear Equation of State (EOS) of cold nuclear matter with the B3Y-Fetal effective interaction in its CDM3Y density-dependent version within the framework of Hartree-Fock approximation. The well-known saturation properties of both symmetric and asymmetric nuclear matter are well-reproduced in this work. Using the CDM3Y-K approach, this study has evolved a new set of user interactions, some of which are CDB3Y1-, CDB3Y2-, CDB3Y3-, CDB3Y4-, CDB3Y5-, CDB3Y6-Fetal interactions with corresponding incompressibilities K0 = 188, 204, 217,228, 241 and 252 MeV respectively,

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48

Asif, M. "Theoretical Calculation of Effective Ionic Charge with Lithium Limiter on HT-7 Tokamak." Journal of Fusion Energy 33, no. 4 (2014): 444–48. http://dx.doi.org/10.1007/s10894-014-9676-7.

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49

MOUSTAKIDIS, CH C., T. S. KOSMAS, F. ŠIMKOVIC, and AMAND FAESSLER. "THE EFFECTS OF DEFORMATION AND PAIRING CORRELATIONS ON NUCLEAR CHARGE FORM FACTOR." International Journal of Modern Physics E 15, no. 03 (2006): 659–72. http://dx.doi.org/10.1142/s0218301306004570.

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A set of moderately deformed s–d shell nuclei is employed for testing the reliability of the nuclear ground state wave functions which are obtained in the context of a BCS approach and offer a simultaneous consideration of deformation and pairing correlations effects. In this method, the mean field is assumed to be an axially symmetric Woods-Saxon potential and the effective two-body interaction is a monopole pairing force. As quantities of main interest we have chosen the nuclear form factors, the occupancies of the active (surface) orbits and the Fermi sea depletion, which provide quite good

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50

Torrens Zaragozá, Francisco. "Periodic Table of the Elements, History, Education and Evaluation." Nereis. Interdisciplinary Ibero-American Journal of Methods, Modelling and Simulation., no. 13 (November 15, 2021): 147–64. http://dx.doi.org/10.46583/nereis_2021.13.808.

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The periodic tables of transition metal thiophosphates MPS3, transition metal dichalcogenides MX2 and other materials, the origin of chemical elements and toxic trace elements in dried mushrooms are provided. The effective nucleus-electron attraction is proportional to the effective nuclear charge (Zeff) and inversely proportional to the effective principal quantum number (n*). The periodic arch is one of many modern visual displays that have been developed to augment the traditional periodic table of the chemical elements. The table is related with the multiparameter optimisation of N atom, n

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