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Journal articles on the topic 'Magnetoelectric and gravitational effects'

Author: Grafiati

Published: 4 June 2025

Last updated: 1 August 2025

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1

Zakharenko, Aleksey Anatolievich. "On separation of exchange terms for four-potential acoustic SH-wave case with dependence on gravitational parameters." Hadronic Journal 41, no. 4 (2018): 349–70. https://doi.org/10.5281/zenodo.2842082.

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One of major achievements in modern physics is investigations of complex systems consisting of mechanical, electrical, magnetic, gravitational, and cogravitational subsystems. The recently developed theory provides the coupling coefficient among these subsystems. It is called the coefficient of the electromagnetogravitocogravitomechanical coupling (CEMGCMC) . This coupling coefficient is one of the very important characteristics of a studied solid material and all the four-potential shear-horizontal acoustic waves depend on this coefficient. This report analytically studies the CEMGCMC concern

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2

Aleksey, Anatolievich Zakharenko. "The problem of finding of eigenvectors for 4P-SH-SAW propagation in 6 mm media." Canadian Journal of Pure and Applied Sciences 11, no. 1 (2017): 4103–19. https://doi.org/10.5281/zenodo.1301202.

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This theoretical report is pertinent to the mathematical problem of finding of all the possible eigenvectors for the four-potential shear-horizontal surface acoustic wave (4P-SH-SAW) propagation in suitable solids. In this case, the wave propagation is coupled with the four potentials, i.e. the electrical, magnetic, gravitational, and cogravitational ones. The taking into account these four potentials results in significant difficulties to find any eigenvector because the mathematical method is significantly complicated. To find all suitable eigenvectors is very important here because it will

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3

Aleksey, Anatolievich Zakharenko. "On new interfacial four-potential acoustic SH-wave in dissimilar media pertaining to transversely isotropic class 6 mm." Canadian Journal of Pure and Applied Sciences 11, no. 3 (2017): 4321–28. https://doi.org/10.5281/zenodo.1301215.

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This theoretical work documents one new interfacial shear-horizontal (SH) acoustic wave, the propagation of which is supported by the common interface between two dissimilar solid materials. For the treated case, four potentials (4P) such as the electric, magnetic, gravitational, and cogravitational potentials contribute in the wave motion in both dissimilar media pertaining to the transversely isotropic class 6 mm. This new interfacial acoustic SH-wave is guided by the perfectly bonded interface between two dissimilar solid continua. It was mathematically found the explicit form for calculati

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4

Aleksey, Anatolievich Zakharenko. "On piezogravitocogravitoelectromagnetic shear-horizontal acoustic waves." Canadian Journal of Pure and Applied Sciences 10, no. 3 (2016): 4011–28. https://doi.org/10.5281/zenodo.1301184.

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This paper relates to the first centenary of the prediction of the existence of gravitational waves by Albert Einstein in 1916. This work develops the theory of the wave propagation in the solids possessing the piezoelectric, piezomagnetic, and magnetoelectric effects as well as the piezogravitic, piezocogravitic, and gravitocogravitic effects, and the other exchange coeffects. Exploiting the quasi-static approximation in the theory of electromagnetism and gravitoelectromagnetism, the thermodynamics and the coupled equations of motion are developed in the common form. To simplify the problem o

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Aleksey, Anatolievich Zakharenko. "ON EXISTENCE OF NEW DISPERSIVE FOUR-POTENTIAL SH-WAVES IN 6 mm PLATES FOR NEW COMMUNICATION ERA BASED ON GRAVITATIONAL PHENOMENA." Canadian Journal of Pure and Applied Sciences 12, no. 3 (2018): 4585–91. https://doi.org/10.5281/zenodo.1471100.

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One of the possible ways to further miniaturize technical devices is the utilization of the two-dimensional structures such as plates. The acoustic wave propagation is one of the important characteristics. This theoretical work provides two new shear-horizontal (SH) dispersive acoustic waves. The SH-wave dispersion relations are obtained in explicit forms for the case of the transversely isotropic (6 <em>mm</em>) plates. In the plate, the propagation of either new SH-wave is coupled with the electrical, magnetic, gravitational, and cogravitational potentials. Using the obtained SH-waves, it is

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6

Zakharenko, Aleksey Anatolievich. "Relative material parameters αE, αH, ϑG, ϑF, ξE, ξF, βH, βG, ζE, ζG, λH, and λF for magnetoelectroelastics to model acoustic wave propagation incorporating gravitational phenomena". Hadronic Journal 43, № 2 (2020): 171–86. https://doi.org/10.5281/zenodo.3987732.

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Regarding solid materials of symmetry class 6 <em>mm</em>, it is natural to deal with mechanical, electrical, magnetic, gravitational, and cogravitational properties. In addition to the electromagnetic <em>α</em> and gravitocogravitic<em> &thetasym;</em> constants, the incorporation of gravitational phenomena for these smart magnetoelectroelastics adds the gravitoelectric <em>ζ</em>, cogravitoelectric <em>ξ</em>, gravitomagnetic <em>β</em>, and cogravitomagnetic<em> λ</em> constants. All of them contribute to the value of the coefficient of the electromagnetogravitoco

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7

Zakharenko. "On Discovery of the Twelfth and Thirteenth New Nondispersive SH-SAWs in 6 mm Magnetoelectroelastics." Acoustics 1, no. 4 (2019): 749–62. http://dx.doi.org/10.3390/acoustics1040044.

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This report acquaints the reader with an extra two new shear-horizontal surface acoustic waves (SH-SAWs). These new SH-SAWs can propagate along the free surface of the transversely isotropic (6 mm) magnetoelectroelastic materials. These (composite) materials can simultaneously possess the piezoelectric, piezomagnetic, and magnetoelectric effects. Some competition among these effects can lead to suitable solutions found for the following three possible coupling mechanisms: eα – hε, eµ – hα, εµ – α2. Here, the mechanically free interface between the solid and a vacuum was considered. This report

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8

Zakharenko, Aleksey Anatolievich. "DEVELOPMENT OF INTERACTIVE SOFTWARE FOR SIMULATION OF MATERIAL AND WAVE PROPERTIES OF PIEZOELECTROMAGNETICS INCORPORATING GRAVITATIONAL PHENOMENA." Canadian Journal of Pure and Applied Sciences 14, no. 2 (2020): 4993–99. https://doi.org/10.5281/zenodo.3921977.

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This short report acquaints the reader with the developed software that can work with pure piezoelectrics, pure piezomagnetics, pure piezoelectromagnetics (PEMs), and the PEMs with incorporation of gravitational phenomena, i.e. piezo gravito torsiono electromagnetic (PGTEM) materials. This software can calculate the material properties and wave characteristics in all the aforementioned continuous media. Also, it allows the PEM and PGTEM composite creation from the material parameters of both piezoelectrics and piezomagnetics that present in the software database or can be loaded from a file. T

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9

Gibbons, Gary, and Marcus Werner. "The Gravitational Magnetoelectric Effect." Universe 5, no. 4 (2019): 88. http://dx.doi.org/10.3390/universe5040088.

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Electromagnetism in spacetime can be treated in terms of an analogue linear dielectric medium. In this paper, we discuss the gravitational analogue of the linear magnetoelectric effect, which can be found in multiferroic materials. While this is known to occur for metrics with non-zero mixed components, we show how it depends on the choice of spatial formalism for the electromagnetic fields, including differences in tensor weight, and also on the choice of coordinate chart. This is illustrated for Langevin–Minkowski, four charts of Schwarzschild spacetime, and two charts of pp gravitational wa

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10

Gareeva Z. V., Zvezdin A. K., Shulga N. V., Gareev T. T., and Chen X. M. "Mechanisms of magnetoelectric effects in oxide multiferroics with a perovskite praphase." Physics of the Solid State 64, no. 9 (2022): 1324. http://dx.doi.org/10.21883/pss.2022.09.54175.43hh.

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Magnetoelectric effects are discussed in multiferroics with the perovskite structure: bismuth ferrite, rare-earth orthochromites, and Ruddlesden--Popper structures belonging to the trigonal, orthorhombic, and tetragonal syngonies. The influence of structural distortions on magnetic and ferroelectric properties is studied, possible magnetoelectric effects (linear, quadratic, inhomogeneous) in these materials are determined, and expressions for the linear magnetoelectric effect tensor are given. Macroscopic manifestations of the inhomogeneous magnetoelectric effect in multiferroic nanoelements a

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11

Cheng, Ji-Hua, Yin-Gang Wang, and Dan Xie. "Interface Effects on the Magnetoelectric Properties of Magnetoelectric Multilayer Composites." Chinese Physics Letters 32, no. 1 (2015): 017503. http://dx.doi.org/10.1088/0256-307x/32/1/017503.

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12

Fiebig, M., Th Lottermoser, Th Lonkai, A. V. Goltsev, and R. V. Pisarev. "Magnetoelectric effects in multiferroic manganites." Journal of Magnetism and Magnetic Materials 290-291 (April 2005): 883–90. http://dx.doi.org/10.1016/j.jmmm.2004.11.282.

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13

Brik, A. B. "Magnetoelectric tunnel effects in paramagnets." Ferroelectrics 161, no. 1 (1994): 59–63. http://dx.doi.org/10.1080/00150199408213353.

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14

Wen, Dandan, Xia Chen, Fuchao Huang, et al. "Piezoelectric and Magnetoelectric Effects of Flexible Magnetoelectric Heterostructure PVDF-TrFE/FeCoSiB." International Journal of Molecular Sciences 23, no. 24 (2022): 15992. http://dx.doi.org/10.3390/ijms232415992.

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Flexible polymer-based magnetoelectric (ME) materials have broad application prospects and are considered as a new research field. In this article, FeCoSiB thin films were deposited on poly(vinylidene fluoride-co-trifluoroethylene) (PVDF-TrFE) substrate by DC magnetron sputtering. The structure of PVDF-TrFE/FeCoSiB heterostructure thin films was similar to 2-2. Under a bias magnetic field of 70 Oe, the composites have a dramatically increased ME voltage coefficient as high as 111 V/cm⋅Oe at a frequency of about 85 kHz. The piezoelectric coefficient of PVDF-TrFE thin films is 34.87 pC/N. The su

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15

Zhou, Yuan, Chee-Sung Park, Mitsuhiro Murayama, and Shashank Priya. "Interfacial effects in magnetoelectric thin/thick composite films." Additional Conferences (Device Packaging, HiTEC, HiTEN, and CICMT) 2013, CICMT (2013): 000199–204. http://dx.doi.org/10.4071/cicmt-2013-tha13.

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This study reports the effect of interfacial structure on the magnetoelectric and ferroelectric characteristics in magnetoelectric laminate thin/thick films. Both bilayer and trilayer magnetoelectric heterostructures were deposited on a Pt/Ti/SiO2/Si substrate using pulsed laser deposition (PLD) and sol-gel deposition (SGD) respectively. BaTiO3 [BTO] / Pb(Zr0.6Ti0.4)O3 [PZT] and CoFe2O4 [CFO] were used as piezoelectric and magnetostrictive materials. The interface between CFO/PZT and CFO/BTO films was found to exhibit excellent interface without any cracks or delamination. PLD grown BTO on CFO

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16

Glinchuk, M. D., and V. V. Khist. "Renovation of Interest in the Magnetoelectric Effect in Nanoferroics." Ukrainian Journal of Physics 63, no. 11 (2018): 1006. http://dx.doi.org/10.15407/ujpe63.11.1006.

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Recent theoretical studies of the influence of the magnetoelectric effect on the physical properties of nanosized ferroics and multiferroics have been reviewed. Special attention is focused on the description of piezomagnetic, piezoelectric, and linear magnetoelectric effects near the ferroid surface in the framework of the Landau–Ginzburg–Devonshire phenomenological theory, where they are considered to be a result of the spontaneous surface-induced symmetry reduction. Therefore, nanosized particles and thin films can manifest pronounced piezomagnetic, piezoelectric, and magnetoelectric proper

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17

Gareeva, Zukhra, Anatoly Zvezdin, Konstantin Zvezdin, and Xiangming Chen. "Symmetry Analysis of Magnetoelectric Effects in Perovskite-Based Multiferroics." Materials 15, no. 2 (2022): 574. http://dx.doi.org/10.3390/ma15020574.

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In this article, we performed symmetry analysis of perovskite-based multiferroics: bismuth ferrite (BiFeO3)-like, orthochromites (RCrO3), and Ruddlesden–Popper perovskites (Ca3Mn2O7-like), being the typical representatives of multiferroics of the trigonal, orthorhombic, and tetragonal crystal families, and we explored the effect of crystallographic distortions on magnetoelectric properties. We determined the principal order parameters for each of the considered structures and obtained their invariant combinations consistent with the particular symmetry. This approach allowed us to analyze the

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18

Гареева, З. В., А. К. Звездин, Н. В. Шульга, Т. Т. Гареев та С. М. Чен. "Механизмы магнитоэлектрических эффектов в оксидных мультиферроиках с прафазой перовскита". Физика твердого тела 64, № 9 (2022): 1338. http://dx.doi.org/10.21883/ftt.2022.09.52830.43hh.

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Magnetoelectric effects are discussed in multiferroics with the perovskite structure: bismuth ferrite, rare-earth orthochromites, and Ruddlesden - Popper structures belonging to the trigonal, orthorhombic, and tetragonal syngonies. The influence of structural distortions on magnetic and ferroelectric properties is studied, possible magnetoelectric effects (linear, quadratic, inhomogeneous) in these materials are determined, and expressions for the linear magnetoelectric effect tensor are given. Macroscopic manifestations of the inhomogeneous magnetoelectric effect in multiferroic nanoelements

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19

GAREEVA, Z. V., A. M. TROCHINA, and SH T. GAREEV. "MAGNETOELECTRIC EFFECTS AND NEW SPINTRONICS LOGIC DEVICES." Izvestia Ufimskogo Nauchnogo Tsentra RAN, no. 1 (March 31, 2023): 65–70. http://dx.doi.org/10.31040/2222-8349-2023-0-1-65-70.

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The paper discusses new logic spintronic devices and the prospects for the use of perovskite-type multiferroics as working elements of magnetoelectric components. The principle of operation of the considered logical devices is based on the use of two components - a magnetoelectric, in which the magnetic state is recorded due to energy-efficient magnetoelectric interaction, and a spin-orbital component, in which information is read out based on the conversion of spin into charge due to the spin-orbital interaction of electrons; both components are interconnected by a nanoelectrode. When designi

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20

Li, Jun, Dongpeng Zhao, Han Bai, Zhi Yuan, and Zhongxiang Zhou. "Low magnetic-field induced high temperature dynamic magnetoelectric coupling performances in Z-type Sr₃Co₂Fe₂₄O₄₁." Journal of Physics: Condensed Matter 34, no. 10 (2021): 105803. http://dx.doi.org/10.1088/1361-648x/ac40ae.

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Abstract Magnetic-field induced dynamic magnetoelectric coupling effects and polarization performance of Z-type Sr3Co2Fe24O41 (SCFO) ceramic has been investigated. Results found that SCFO’s transverse tapered magnetic structure can induce electric polarization, and its electric polarization direction will not change under external magnetic effects. First-order dynamic magnetoelectric coupling coefficient (α) and second-order dynamic magnetoelectric coupling coefficient (β) of SCFO exhibited strong response main in magnetic structural phase transition region. The magnetoelectric structural phas

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21

Henrichs, Leonard F., Xiaoke Mu, Torsten Scherer, et al. "First-time synthesis of a magnetoelectric core–shell composite via conventional solid-state reaction." Nanoscale 12, no. 29 (2020): 15677–86. http://dx.doi.org/10.1039/d0nr02475a.

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Novel magnetoelectric core–shell ceramics exhibit characteristics of several traditional magnetoelectric composites and combine exceptional magnetoelectric coupling with low leakage current, high density and absence of substrate clamping effects.

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22

Chupis, I. E. "Spontaneous magnetoelectric effects in cubic ferromagnetoelectrics." Soviet Journal of Low Temperature Physics 11, no. 9 (1985): 529–32. https://doi.org/10.1063/10.0031357.

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The interrelationship between the orientations of the spontaneous polarization and spontaneous magnetization in ferro(ferri)magnetoelectric crystals with a centrosymmetric cubic paraelectric phase whose ferroelectric transition temperature is lower than the critical temperature for the magnetic ordering is studied. Exact solutions are obtained for the equilibrium moments for any values of the energy parameters. It is shown that the magnetoelectric interaction determines the direction of the electric polarization in a magnetic domain. At lower temperatures first- or second-order phase transitio

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23

Kimura, Tsuyoshi. "Current Progress of Research on Magnetically-induced Ferroelectrics." Acta Crystallographica Section A Foundations and Advances 70, a1 (2014): C6. http://dx.doi.org/10.1107/s2053273314099938.

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Among several different types of magnetoelectric multiferroics, "magnetically-induced ferroelectrics" in which ferroelectricity is induced by complex spin orders, such as spiral orders, exhibit giant direct magnetoelectric effects, i.e., remarkable changes in electric polarization in response to a magnetic field. Not a few spin-driven ferroelectrics showing the magnetoelectric effects have been found in the past decade.[1] However, their induced ferroelectric polarization is much smaller than that in conventional ferroelectrics and mostly develops only at temperatures much lower than room temp

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24

Zhang, C. L., J. S. Yang, and W. Q. Chen. "Magnetoelectric effects in laminated multiferroic shells." International Journal of Applied Electromagnetics and Mechanics 28, no. 4 (2008): 441–54. http://dx.doi.org/10.3233/jae-2008-996.

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25

Tokura, Yoshinori, and Noriaki Kida. "Dynamical magnetoelectric effects in multiferroic oxides." Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 369, no. 1951 (2011): 3679–94. http://dx.doi.org/10.1098/rsta.2011.0150.

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Multiferroics with coexistent ferroelectric and magnetic orders can provide an interesting laboratory to test unprecedented magnetoelectric (ME) responses and their possible applications. One such example is the dynamical and/or resonant coupling between magnetic and electric dipoles in a solid. As examples of such dynamical ME effects, (i) the multiferroic domain wall dynamics and (ii) the electric dipole active magnetic responses are discussed with an overview of recent experimental observations.

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26

Clin, Martial, Jean-Pierre Rivera, and Hans Schmid. "Low temperature magnetoelectric effects on Co3B7O13I." Ferroelectrics 108, no. 1 (1990): 213–18. http://dx.doi.org/10.1080/00150199008018759.

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27

Chupis, I. E. "TfP255. Magnetoelectric effects in ferroelectromagnetic films." Ferroelectrics 134, no. 1 (1992): 337–42. http://dx.doi.org/10.1080/00150199208015609.

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28

Ghidini, M., S. S. Dhesi, and N. D. Mathur. "Nanoscale magnetoelectric effects revealed by imaging." Journal of Magnetism and Magnetic Materials 520 (February 2021): 167016. http://dx.doi.org/10.1016/j.jmmm.2020.167016.

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29

Fetisov, Y. K., A. A. Bush, K. E. Kamentsev, and G. Srinivasan. "Pyroelectric effects in magnetoelectric multilayer composites." Solid State Communications 132, no. 5 (2004): 319–24. http://dx.doi.org/10.1016/j.ssc.2004.07.070.

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30

Gorbatsevich, A. A., O. V. Krivitsky, and S. V. Zaykov. "Magnetoelectric effects in correlated electronic systems." Ferroelectrics 161, no. 1 (1994): 343–48. http://dx.doi.org/10.1080/00150199408213383.

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31

Smirnov, A. I. "Microwave magnetoelectric effects in antiferromagnet Nd2CuO4." Ferroelectrics 162, no. 1 (1994): 355–61. http://dx.doi.org/10.1080/00150199408245123.

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32

Chupis, I. E. "High-frequency magnetoelectric effects in ferroelectrics." Ferroelectrics 204, no. 1 (1997): 173–80. http://dx.doi.org/10.1080/00150199708222197.

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33

Hu, Zhi-Ming, Yu Su, and Jackie Li. "Nonlinear magnetoelectric effects of multiferroic composites." International Journal of Solids and Structures 212 (March 2021): 96–106. http://dx.doi.org/10.1016/j.ijsolstr.2020.12.008.

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34

Petrov, V. M., and M. I. Bichurin. "ChemInform Abstract: Magnetoelectric Effects in Nanocomposites." ChemInform 43, no. 32 (2012): no. http://dx.doi.org/10.1002/chin.201232228.

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35

Chanda, Sumanto, G. W. Gibbons, Partha Guha, Paolo Maraner, and Marcus C. Werner. "Jacobi-Maupertuis Randers-Finsler metric for curved spaces and the gravitational magnetoelectric effect." Journal of Mathematical Physics 60, no. 12 (2019): 122501. http://dx.doi.org/10.1063/1.5098869.

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36

Kaplan, Michael. "Magnetoelectricity in Jahn–Teller Elastics." Magnetochemistry 7, no. 7 (2021): 95. http://dx.doi.org/10.3390/magnetochemistry7070095.

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The magnetoelectric effects in Jahn–Teller crystals are discussed on the basis of phenomenology and microscopic theory. New magnetoelectric effects—metamagnetoelectricity—are analyzed. Formation of multiferroic crystal states as the consequence of the cooperative Jahn–Teller effect is discussed.

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37

Lee, Eun Gu, Jong Kook Lee, Woo Yang Jang, Sun Jae Kim, and Jae Gab Lee. "Magnetoelectric Effects in (Bi,La)FeO3-PbTiO3Ceramics." Korean Journal of Materials Research 15, no. 2 (2005): 121–25. http://dx.doi.org/10.3740/mrsk.2005.15.2.121.

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38

Chang, Sou-Chi, Sasikanth Manipatruni, Dmitri E. Nikonov, and IAN A. Young. "Clocked Domain Wall Logic Using Magnetoelectric Effects." IEEE Journal on Exploratory Solid-State Computational Devices and Circuits 2 (December 2016): 1–9. http://dx.doi.org/10.1109/jxcdc.2016.2515120.

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39

Fetisov, Y. K., D. V. Chashin, A. G. Segalla, and G. Srinivasan. "Resonance magnetoelectric effects in a piezoelectric bimorph." Journal of Applied Physics 110, no. 6 (2011): 066101. http://dx.doi.org/10.1063/1.3633222.

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40

SRINIVASAN, G., and Y. K. FETISOV. "MICROWAVE MAGNETOELECTRIC EFFECTS AND SIGNAL PROCESSING DEVICES." Integrated Ferroelectrics 83, no. 1 (2006): 89–98. http://dx.doi.org/10.1080/10584580600949105.

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41

Wang, Fen, Tao Zou, Yi Liu, Li-Qin Yan, and Young Sun. "Persistent multiferroicity without magnetoelectric effects in CuO." Journal of Applied Physics 110, no. 5 (2011): 054106. http://dx.doi.org/10.1063/1.3636106.

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42

Smirnov, A. I. "New magnetoelectric effects in the antiferromagnet Gd2CuO4." Czechoslovak Journal of Physics 46, S4 (1996): 2139–40. http://dx.doi.org/10.1007/bf02571061.

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43

Zhang, C. L., W. Q. Chen, and Ch Zhang. "Magnetoelectric effects in functionally graded multiferroic bilayers." Journal of Applied Physics 113, no. 8 (2013): 084502. http://dx.doi.org/10.1063/1.4792657.

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44

Ngo, Anh T., Javier Rodriguez-Laguna, Sergio E. Ulloa, and Eugene H. Kim. "Quantum Manipulation via Atomic-Scale Magnetoelectric Effects." Nano Letters 12, no. 1 (2011): 13–16. http://dx.doi.org/10.1021/nl2025807.

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45

Zhang, C. L., W. Q. Chen, S. H. Xie, J. S. Yang, and J. Y. Li. "The magnetoelectric effects in multiferroic composite nanofibers." Applied Physics Letters 94, no. 10 (2009): 102907. http://dx.doi.org/10.1063/1.3095596.

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46

Chavan, Pradeep, L. R. Naik, P. B. Belavi, et al. "Temperature Dependent Electric Properties and Magnetoelectric Effects in Ferroelectric rich Ni0.8Mg0.2Fe2O4 + BaZr0.2Ti0.8O3 Magnetoelectric Composites." Journal of Alloys and Compounds 777 (March 2019): 1258–64. http://dx.doi.org/10.1016/j.jallcom.2018.10.157.

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47

Hayes, T. J., S. R. Valluri, and L. Mansinha. "Gravitational effects from earthquakes." Canadian Journal of Physics 82, no. 12 (2004): 1027–40. http://dx.doi.org/10.1139/p04-068.

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Two types of propagating gravitational effects, from the mass redistribution within the Earth due to a large earthquake, are investigated: (i) the velocity of the change of the Newtonian potential field; and (ii) the gravitational luminosity of the seismic source. The mass redistribution caused by an earthquake and the resulting change in the gravitational potential field is computed through application of geophysical dislocation theory. The global mass redistribution is postulated to be progressive, starting at the instant (and location) of the nucleation of the earthquake fault rupture, and

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48

Briskman, V. A. "Gravitational effects in polymerization." Advances in Space Research 24, no. 10 (1999): 1199–210. http://dx.doi.org/10.1016/s0273-1177(99)00720-6.

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49

Ren, Zhenqiu, and Yi Lin. "Post‐Einstein gravitational effects." Kybernetes 30, no. 4 (2001): 433–48. http://dx.doi.org/10.1108/03684920110386937.

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Gusev, A. V., V. N. Rudenko, I. V. Tsybankov, and V. D. Yushkin. "Detection of gravitational geodynamic effects with gravitational-wave interferometers." Gravitation and Cosmology 17, no. 1 (2011): 76–79. http://dx.doi.org/10.1134/s0202289311010105.

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