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Journal articles on the topic 'Magnetic charge'

Author: Grafiati

Published: 3 June 2025

Last updated: 31 July 2025

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1

Jeong, Eue Jin, and Dennis Edmondson. "Measurement of the Magnetic Monopole Charge, the Missing Link in Quantum Mechanics, Aether and the Dark Energy." International Journal of Fundamental Physical Sciences 12, no. 2 (2022): 19–28. http://dx.doi.org/10.14331/ijfps.2022.330152.

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Charge conservation in the theory of elementary particle physics is one of the best-established principles ‎in physics. As such, if ‎there are magnetic monopoles in the universe, the magnetic charge will most likely be a ‎conserved quantity like electric ‎charges. If neutrinos are magnetic monopoles, as physicists have reported ‎the possibility, the Earth should show signs of ‎having a magnetic monopole charge on a macroscopic scale ‎since neutrons must also have a magnetic monopole charge if ‎the general charge conservation principle is valid. ‎To test this hypothesis, experiments were perfor

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2

Akers, David. "Existence of magnetic charge." International Journal of Theoretical Physics 29, no. 10 (1990): 1091–97. http://dx.doi.org/10.1007/bf00672087.

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3

Magnon, Anne M. R. "Ratios of magnetic charge to charge and of magnetic mass to mass." International Journal of Theoretical Physics 27, no. 1 (1988): 3–7. http://dx.doi.org/10.1007/bf00672042.

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4

Deng, Yanbin, Changyu Huang, and Yong-Chang Huang. "Constraining the existence of magnetic monopoles by Dirac-dual electric charge renormalization effect under the Planck scale limit." International Journal of Modern Physics A 31, no. 24 (2016): 1650133. http://dx.doi.org/10.1142/s0217751x16501335.

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It was suggested by dimensional analysis that there exists a limit called the Planck energy scale coming close to which the gravitational effects of physical processes would inflate and struggle for equal rights so as to spoil the validity of pure nongravitational physical theories that governed well below the Planck energy. Near the Planck scale, the Planck charges, Planck currents, or Planck parameters can be defined and assigned to physical quantities such as the single particle electric charge and magnetic charge as the ceiling value obeyed by the low energy ordinary physics. The Dirac ele

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5

Evans, Timothy J., and Douglas Singleton. "Magnetic charge and photon mass: Physical string singularities, Dirac condition, and magnetic confinement." International Journal of Modern Physics A 33, no. 11 (2018): 1850064. http://dx.doi.org/10.1142/s0217751x18500641.

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We find exact, simple solutions to the Proca version of Maxwell’s equations with magnetic sources. Several properties of these solutions differ from the usual case of magnetic charge with a massless photon: (i) the string singularities of the usual 3-vector potentials become real singularities in the magnetic fields; (ii) the different 3-vector potentials become gauge inequivalent and physically distinct solutions; (iii) the magnetic field depends on r and [Formula: see text] and thus is no longer rotationally symmetric; (iv) a combined system of electric and magnetic charge carries a field an

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6

Adhikari, B. R., S. Basnet, H. P. Lamichhane, and R. Khanal. "Variation of Velocity of Ions in a Magnetized Plasma Sheath for Different Magnetic Field." Journal of Nepal Physical Society 6, no. 1 (2020): 25–29. http://dx.doi.org/10.3126/jnphyssoc.v6i1.30513.

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The kinetic trajectory simulation method has been used to study ion velocity profile in a plasma sheath for varying magnetic field at fixed obliqueness. As the electrons have higher velocity compared to that of ions the wall is charged up negatively with respect to the core plasma. The negative potential then attracts the ions and repels electrons forming a thin positive space charge region in front of the wall. This positive space charge region, known as the ‘sheath’ separates the negatively charged wall from the quasineutral ‘presheath’ plasma. The ions moving towards the wall have to satisf

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7

Jain, Vishal, Hitesh Parmar, and Ketan Dodiya. "FTIR Spectra of Magnetic Charge Transfer Complexes of TEMPO Free Radical." International Journal of Trend in Scientific Research and Development 1, no. 2 (2017): 8–13. http://dx.doi.org/10.31142/ijtsrd62.

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8

Arrott, Anthony S., and Terry L. Templeton. "Using magnetic charge to understand soft-magnetic materials." AIP Advances 8, no. 4 (2018): 047301. http://dx.doi.org/10.1063/1.4994219.

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9

Bonville, P., J. Hammann, J. A. Hodges, P. Imbert, and G. Jéhanno. "Magnetic and non-magnetic charge states in YbPd." Journal of Magnetism and Magnetic Materials 63-64 (January 1987): 621–22. http://dx.doi.org/10.1016/0304-8853(87)90685-8.

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10

Deng, Jiang Hua, Yi Ming Zheng, Chao Tang, and Yan Ran Zhan. "Analysis of Charge Circuit and Discharge Circuit in Electromagnetic Riveting." Applied Mechanics and Materials 241-244 (December 2012): 606–9. http://dx.doi.org/10.4028/www.scientific.net/amm.241-244.606.

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The analysis of charge circuit and discharge circuit is a key part in the theoretical study of electromagnetic riveting electromagnetic field. Numerical simulation was used to establish the charge circuit model and the discharge circuit model which was an electric circuit-magnetic circuit coupling process by ANSYS. The simulation of charge circuit shows that the development of the charge current over time is an exponential descending change and that of the charge voltage over time is an exponential ascending change. And, the simulation of discharge circuit indicates that the driver is mainly s

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11

LI, KANG. "COMMENTS ON THE DEPENDENCE BETWEEN ELECTRIC CHARGE AND MAGNETIC CHARGE." Modern Physics Letters A 17, no. 40 (2002): 2647–55. http://dx.doi.org/10.1142/s0217732302009350.

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By using the two four-dimensional potential formulation of electromagnetic (EM) field theory introduced in Ref. 1, we found that the SO(2) duality symmetric EM field theory can be reduced to the magnetic source-free case by a special choice of SO(2) parameter, we called this special case nature picture of the EM field theory, the reduction condition led to a result, i.e. the electric charge and magnetic charge are no longer independent. Some comments to Ref. 10 are also mentioned.

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12

Vento, Vicente. "Ions, Protons, and Photons as Signatures of Monopoles." Universe 4, no. 11 (2018): 117. http://dx.doi.org/10.3390/universe4110117.

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Magnetic monopoles have been a subject of interest since Dirac established the relationship between the existence of monopoles and charge quantization. The Dirac quantization condition bestows the monopole with a huge magnetic charge. The aim of this study was to determine whether this huge magnetic charge allows monopoles to be detected by the scattering of charged ions and protons on matter where they might be bound. We also analyze if this charge favors monopolium (monopole–antimonopole) annihilation into many photons over two photon decays.

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13

Wang, Y. L., Z. L. Xiao, A. Snezhko, et al. "Rewritable artificial magnetic charge ice." Science 352, no. 6288 (2016): 962–66. http://dx.doi.org/10.1126/science.aad8037.

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14

Freeman, P. G., S. M. Hayden, C. D. Frost, D. Prabhakaran, and A. T. Boothroyd. "Magnetic excitations of charge-ordered." Journal of Magnetism and Magnetic Materials 310, no. 2 (2007): 760–62. http://dx.doi.org/10.1016/j.jmmm.2006.10.488.

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15

Chittipeddi, Sailesh R., Arthur J. Epstein, Jian H. Zhang, et al. "Magnetic molecular charge transfer complexes." Synthetic Metals 19, no. 1-3 (1987): 731–35. http://dx.doi.org/10.1016/0379-6779(87)90444-9.

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16

Thalmeier, P., and A. N. Yaresko. "Magnetic excitations in charge ordered." European Physical Journal B 14, no. 3 (2000): 495. http://dx.doi.org/10.1007/s100510051058.

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17

Thalmeier, P., and A. N. Yaresko. "Magnetic excitations in charge ordered." European Physical Journal B 14, no. 3 (2000): 495–508. http://dx.doi.org/10.1007/pl00011054.

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18

Sinha, Aloke Kumar. "Thermal fluctuations and correlations among hairs of a stable quantum black hole: Some examples." Modern Physics Letters A 33, no. 33 (2018): 1850190. http://dx.doi.org/10.1142/s0217732318501900.

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We have already derived the criteria for thermal stability of charged rotating quantum black holes, for horizon areas that are large relative to the Planck area. The derivation is done by using results of loop quantum gravity and equilibrium statistical mechanics of the grand canonical ensemble. We have also showed that in four-dimensional spacetime, quantum AdS Kerr–Newman black hole and asymptotically AdS dyonic black hole with electric and magnetic charge are thermally stable within certain range of its parameters. In this paper, the expectation values of fluctuations and correlations among

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19

PAVLOV, V. D. "MAGNETIC FLOW AND ITS QUANTIZATION." Izvestia Ufimskogo Nauchnogo Tsentra RAN, no. 4 (December 11, 2020): 25–28. http://dx.doi.org/10.31040/2222-8349-2020-0-4-25-28.

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It is noted that the elementary electric charge is equal to e , from which fact the well-known principle of quantization of the electric charge definitely follows, namely, the electric charge is quantized and a quantum is the charge of the electron e (or positron). Or any change in the charge is equal to an integer number of electrons (or positrons). The formally identical transformation of the principle of quantization of the electric charge allows formulating the principle of quantization of the magnetic flux, namely, the quantity inverse to the magnetic flux is quantized and a quantum is th

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20

Huseynov, J., O. Hasanov, H. Adgezalova, G. Aslanov, and G. Garashova. "MAGNETORESISTANCE OF GdxSn1-xSe SYSTEM ALLOYS." Slovak international scientific journal, no. 88 (October 13, 2024): 75–80. https://doi.org/10.5281/zenodo.13926559.

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The dependence of magnetic resistance of GdxSn1-xSe solid solutions on gadolinium content, temperature and magnetic field strength is investigated. It is established that with an increase in the amount of Gd element in the composition, the absolute value of magnetic resistance increases, the inversion point in SnSe solid solutions with Gd element shifts to the region of higher temperature. The change in the sign of magnetic resistance is due to a change in the scattering mechanism due to the participation of second-order charge carriers in the charge transfer process.

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21

ZENG, XIAOXIONG. "FERMIONS TUNNELING OF DYONIC PARTICLES FROM THE CHARGED AND MAGNETIZED BLACK HOLES." Modern Physics Letters A 24, no. 20 (2009): 1605–15. http://dx.doi.org/10.1142/s0217732309029958.

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The fermions tunneling formulism of Kerner and Mann is extended to the case of black holes with electric and magnetic charges. As the electric and magnetic fields would couple with gravity field, we introduce the Dirac equation of charged and magnetized particles. We study the spin-up particles from the Reissner–Nordström black hole with magnetic charges and spin-down particles from the Kerr–Newman–Kasuya black hole and obtain the corresponding emission temperatures. In particular, we also provide a simplified method by defining an equivalent charge and gauge potential to further discuss tunne

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22

Brandão Faria, Jose A. "Magnetic charge, magnetic current, magnetic scalar potential, and electric vector potential." Microwave and Optical Technology Letters 56, no. 5 (2014): 1107–11. http://dx.doi.org/10.1002/mop.28274.

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23

Belachew, Desalegn. "A Review of Determination of Charge to Mass Ratio of an Electron by Thomson's method." j. of Physical and Chemical Sciences Volume 6, Issue 2 (2018): 01. https://doi.org/10.5281/zenodo.1195603.

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The orbit of a charged particle in a uniform and constant magnetic field is a circle when the initial velocity of the particle is perpendicular to the magnetic field. The radius of the orbit depends on the charge to mass ratio of the particle, q/m, the speed of the particle v, and the strength of the magnetic field B. When the strength of the magnetic field and the initial speed of the particle are known, a measurement of a radius of the orbit determines q/m. This principle was used by J.J. Thomson to measure the charge to mass ratio of the electron, e/m, in 1897. In this experiment I have use

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24

Thorman, Alex, Edward Litherland-Smith, Sheena Menmuir, et al. "Visible spectroscopy of highly charged tungsten ions with the JET charge exchange diagnostic." Physica Scripta 96, no. 12 (2021): 125631. http://dx.doi.org/10.1088/1402-4896/ac387b.

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Abstract Since the installation of the ITER-like wall on the JET tokamak, visible emission from a broad range of tungsten charge states has complicated plasma ion temperature and toroidal rotation measurements. A plethora of charge exchange transitions, from ions up to W56+, and 21 suspected magnetic dipole transitions have been observed. In particular W39+ and W46+ charge exchange emission contaminates the long-established carbon measurement at 529 nm. Fortunately the wavelength and relative intensity of the tungsten charge exchange lines is predictable and their influence can be mitigated wh

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25

Bashier, Louai Hassan Elzein. "Maxwell's Equations Under Lorentz Transformations: Investigating the Spontaneous Emergence of Magnetic Charge and Current Densities." مجلة العلوم الطبيعية و الحياتية والتطبيقية 9, no. 1 (2025): 38–51. https://doi.org/10.26389/ajsrp.k010125.

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The quest for magnetic monopoles has captivated theoretical physicists due to their potential to reshape our understanding of electromagnetism. Despite extensive research, definitive mathematical proof of their existence remains elusive. This paper presents a rigorous mathematical framework supporting the existence of magnetic monopoles within the covariant formulation of classical electromagnetism and special relativity. Utilizing tensor calculus and the covariance form of Maxwell's equations, we derive expressions for magnetic charge density and magnetic current density through Lorentz trans

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26

Wolf, C. "Charge screening in Born–Infeld theory by magnetic charge of another U(1) gauge group." Canadian Journal of Physics 69, no. 10 (1991): 1304–8. http://dx.doi.org/10.1139/p91-195.

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We calculate the screening of an electric charge brought about by the coupling of electromagnetism to a second gauge group carrying magnetic charge. The resultant classical calculation demonstrates that the electric charge is antiscreened by magnetic charge. The total mass of the configuration is also evaluated including that due to the coupling of electromagnetism to the magnetic charge of a second U(1) gauge group.

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27

Arrott, Anthony Schuyler. "Visualization and Interpretation of Magnetic Configurations Using Magnetic Charge." IEEE Magnetics Letters 7 (2016): 1–5. http://dx.doi.org/10.1109/lmag.2016.2631127.

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28

Penttinen, M. "Small-Angle Scattering on a System of Magnetic and Electric Charges." International Journal of Modern Physics A 12, no. 18 (1997): 3193–204. http://dx.doi.org/10.1142/s0217751x97001687.

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The generalization of the conformal scattering method for small-angle scattering processes involving magnetic monopoles and ordinary charges is constructed. Using this generalization we show that the introduction of magnetic charges corresponds to analytical continuation of the eikonal amplitude in the complex charge plane (the imaginary part is proportional to the magnetic charge). We calculate explicitly the eikonal amplitude for scattering on a dyon and two monopoles in terms of confluent hypergeometric functions. The singularities of the corresponding amplitudes (focal points) are studied

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29

Yang, Zi, Haocheng Yang, Donglu Shi, and Yilong Wang. "In-Vitro Study of Cancer Cell Binding and Photothermal Inhibition Efficiency by Gold Nanoparticles-Capped Iron Oxide Nanospheres." Nano LIFE 09, no. 01n02 (2019): 1940004. http://dx.doi.org/10.1142/s179398441940004x.

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Different from the traditional cancer cell targeting through protein biomarkers, strong negative surface charges of cancer cells over normal cells derived from the dramatic excretion of lactate acid by cancer cells due to their glycolysis have been testified as an effective cancer cell binding strategy. In our previous work, polyethylenimine (PEI)-functionalized iron oxide nanoparticles (NPs) with strong positive surface charge and good photothermal property have been applied to kill cancer cells in vitro. Considering the obvious cytotoxicity of the first generation of positively charged nanot

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30

Huang, Ranran, Hongmei Li, Mingyang Jiang, Yu Wang, and Chuntian Zhao. "Magnetic charge model of defect in magnetic flux leakage testing." International Journal of Applied Electromagnetics and Mechanics 64, no. 1-4 (2020): 1315–23. http://dx.doi.org/10.3233/jae-209450.

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The defect in structures is the major risk to the structural integrity, thus to perform the defect detections and evaluations efficiently is critical in assuring the structural safety. Magnetic flux leakage testing (MFLT) is an important non-destructive testing (NDT) method. Due to its high testing sensitivity and simple operating procedure, it has been widely used in detecting surface and near-surface defects in ferromagnetic components. To improve the accuracy of defect detection, it is necessary to find a suitable source magnetization distribution around a defect, and furthermore, to correl

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31

Igarashi, Hajime, Arnulf Kost, and Toshihisa Honma. "Reconstruction of planar magnetic charge distribution." International Journal of Applied Electromagnetics and Mechanics 15, no. 1-4 (2002): 257–60. http://dx.doi.org/10.3233/jae-2002-509.

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32

Millange, F., S. de Brion, and G. Chouteau. "Charge, orbital, and magnetic order inNd0.5Ca0.5MnO3." Physical Review B 62, no. 9 (2000): 5619–26. http://dx.doi.org/10.1103/physrevb.62.5619.

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33

Batra, S., A. Lehmann‐Szweykowski, and P. E. Wigen. "Magnetic properties of charge uncompensated CaGe:YIG." Journal of Applied Physics 61, no. 8 (1987): 3274–76. http://dx.doi.org/10.1063/1.338879.

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34

Muscia, Roberto. "Equivalent magnetic charge in helicoidal magnets." Journal of Applied Physics 104, no. 10 (2008): 103916. http://dx.doi.org/10.1063/1.2975154.

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35

Mikhailov, V. F. "Experimental detection of Dirac's magnetic charge?" Journal of Physics D: Applied Physics 29, no. 3 (1996): 801–4. http://dx.doi.org/10.1088/0022-3727/29/3/043.

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36

Enoki, Toshiaki, and Akira Miyazaki. "Magnetic TTF-Based Charge-Transfer Complexes." Chemical Reviews 104, no. 11 (2004): 5449–78. http://dx.doi.org/10.1021/cr0306438.

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37

Voit, Johannes. "Magnetic properties of charge density waves." Synthetic Metals 29, no. 2-3 (1989): 365–70. http://dx.doi.org/10.1016/0379-6779(89)90923-5.

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38

Georgi, Howard, and Lisa Randall. "Charge conjugation and neutrino magnetic moments." Physics Letters B 244, no. 2 (1990): 196–202. http://dx.doi.org/10.1016/0370-2693(90)90055-b.

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39

Hammond, Richard T. "Magnetic charge type equations from torsion." General Relativity and Gravitation 23, no. 9 (1991): 973–80. http://dx.doi.org/10.1007/bf00756860.

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40

Porforough, Milad. "Magnetic charge quantization from SYM considerations." EPL (Europhysics Letters) 127, no. 4 (2019): 41001. http://dx.doi.org/10.1209/0295-5075/127/41001.

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41

Fujita, Mitsutaka, Kazushige Machida, and Hiizu Nakanishi. "Charge Density Waves under Magnetic Fields." Journal of the Physical Society of Japan 54, no. 10 (1985): 3820–32. http://dx.doi.org/10.1143/jpsj.54.3820.

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42

Sternlieb, B. J., J. P. Hill, U. C. Wildgruber, et al. "Charge and Magnetic Order in La0.5Sr1.5MnO4." Physical Review Letters 76, no. 12 (1996): 2169–72. http://dx.doi.org/10.1103/physrevlett.76.2169.

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43

Radaelli, P. G., D. E. Cox, M. Marezio, and S.-W. Cheong. "Charge, orbital, and magnetic ordering inLa0.5Ca0.5MnO3s." Physical Review B 55, no. 5 (1997): 3015–23. http://dx.doi.org/10.1103/physrevb.55.3015.

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44

Pinto, Marc A. "Limitations of the magnetic charge formalism." Journal of Magnetism and Magnetic Materials 97, no. 1-3 (1991): 235–45. http://dx.doi.org/10.1016/0304-8853(91)90187-f.

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45

Hermosilla Palacios, Martha Alejandra, Marissa Martinez, Jeff Blackburn, and Alexander Spokoyny. "Quantifying Free Carriers in Doped SWCNTs: An Optical and Magnetic Resonance Approach." ECS Meeting Abstracts MA2023-01, no. 10 (2023): 1188. http://dx.doi.org/10.1149/ma2023-01101188mtgabs.

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Single-walled carbon nanotubes (SWCNTs) have become increasingly important for opto-electronic devices due to their strong optical absorption, tunable carrier densities, and large carrier mobilities. To produce electricity in applications like photovoltaics and sensors, after light absorption the bound exciton must be separated into free charges carriers. However, the nature of charges in s-SWCNTs is still unclear and a way to quantify them has remained elusive. To better understand free carriers in doped semiconducting SWCNTs we employ a new class of molecular charge-transfer dopants, functio

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46

Zhou, Guo-Quan. "CHARGE MOMENT TENSOR AND THE MAGNETIC MOMENT OF ROTATIONAL CHARGED BODIES." Progress In Electromagnetics Research 68 (2007): 151–60. http://dx.doi.org/10.2528/pier06080603.

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47

Chen, Peng, and You Wei Du. "Large Magnetic Entropy Change near Charge-Ordered Transition Temperature in Nd0.5Sr0.5MnO3." Journal of the Physical Society of Japan 70, no. 4 (2001): 1080–83. http://dx.doi.org/10.1143/jpsj.70.1080.

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48

Dubinov, A. E. "Transverse motion of charged particle with oscillating charge in magnetic field." Technical Physics Letters 37, no. 4 (2011): 344–46. http://dx.doi.org/10.1134/s1063785011040183.

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49

Rayimbaev, Javlon, Bakhtiyor Narzilloev, Ahmadjon Abdujabbarov, and Bobomurat Ahmedov. "Dynamics of Magnetized and Magnetically Charged Particles around Regular Nonminimal Magnetic Black Holes." Galaxies 9, no. 4 (2021): 71. http://dx.doi.org/10.3390/galaxies9040071.

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The present paper is devoted to the study of the event horizon properties of spacetime around a regular nonminimal magnetic black hole (BH), together with dynamics of magnetized and magnetically charged particles in the vicinity of the BH. It is shown that the minimum value of the outer horizon of the extreme charged BH increases with the increase in coupling parameter. It reaches its maximum value of 1.5M when q→∞, while the maximal value of the BH charge decreases and tends toward zero. We also present a detailed analysis of magnetized particles’ motion around a regular nonminimal magnetic b

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50

Navarro-Lérida, Francisco, and D. H. Tchrakian. "Electrically charged finite energy solutions of an SO(5) and an SU(3) Higgs–Chern–Simons-Yang–Mills–Higgs system in 3+1 dimensions." International Journal of Modern Physics A 30, no. 15 (2015): 1550079. http://dx.doi.org/10.1142/s0217751x15500797.

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We study spherically symmetric finite energy solutions of two Higgs–Chern–Simons-Yang–Mills–Higgs (HCS-YMH) models in 3+1 dimensions, one with gauge group SO(5) and the other with SU(3). The Chern–Simons (CS) densities are defined in terms of both the Yang–Mills (YM) and Higgs fields and the choice of the two gauge groups is made so that they do not vanish. The solutions of the SO(5) model carry only electric charge and zero magnetic charge, while the solutions of the SU(3) model are dyons carrying both electric and magnetic charges like the Julia–Zee (JZ) dyon. Unlike the latter, however, the

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