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Journal articles on the topic 'Electric susceptibility'

Author: Grafiati
Published: 4 June 2021
Last updated: 6 February 2022

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1

Khare, Avinash, and Trilochan Pradhan. "Magneto-electric susceptibility of the vacuum." Physics Letters B 231, no. 1-2 (November 1989): 178–80. http://dx.doi.org/10.1016/0370-2693(89)90135-4.

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2

Gunawan, Vincensius, Ngurah Ayu Ketut Umiati, and Agus Subagio. "The Electric Susceptibility of Bi-Layers Ferroelectrics." Journal of Physics and Its Applications 1, no. 2 (June 20, 2019): 53. http://dx.doi.org/10.14710/jpa.v1i2.4860.

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In order to enhance insight of layered structure, we perform numerical calculation to obtain the dynamic electric susceptibility in bi-layers ferroelectrics. Since susceptibility is a parameter which gives response to the external field, then determination of this parameter is important. A lattice model is employed to slice bilayer structure into several lattices. Then, Landau-Khalatnikov equation of motion is used in each lattice to construct a matrix equation of equation of motion. The solution is obtained by applying entire-cell effective medium. We find that the homogeneity of dynamic polarization is different from homogeneity of the single individual layer due to the existence of interlayer interaction. As a result, the electric susceptibility is also altered. It is also noticed that there is a relation between the homogeneity of dynamic polarization and the value of electric susceptibility near resonant frequency. The higher the homogeneity, the bigger the values of susceptibility will be.
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3

ARDELEAN, I., P. PĂŞCUŢĂ, and V. IONCU. "MAGNETIC AND ELECTRIC BEHAVIOR OF IRON IONS IN THE 3B2O3·CAO GLASS MATRIX." Modern Physics Letters B 15, no. 30 (December 30, 2001): 1445–53. http://dx.doi.org/10.1142/s0217984901003378.

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Magnetic susceptibility and electric resistivity measurements have been performed on x Fe 2 O 3 · (100-x)[3 B 2 O 3· CaO ] glasses with 0 <x≤ 50 mol%. Magnetic susceptibility data suggest that for x>5 mol% the iron ions participate in the negative superexchange interaction. From Curie constant values we have established that in these glasses both Fe 2+ and Fe 3+ ions are present, which explains their magnetic and electric behavior. The electrical resistivity and the conductivity activation energy decreases with the Fe 2 O 3 content. In order to analyze the electrical data, we have considered, in these glasses, a polaronic model for conduction.
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4

MOTA, F. DE BRITO, and A. FERREIRA DA SILVA. "ENHANCED DONOR ELECTRIC SUSCEPTIBILITY IN SEMICONDUCTOR SYSTEMS." Modern Physics Letters B 06, no. 30 (December 30, 1992): 1943–49. http://dx.doi.org/10.1142/s0217984992001654.

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The electric susceptibility due to interacting donor-pair molecules are presented for a random distribution of uncompensated phosphorus-doped silicon at T=0 K. The results yield a critical exponent and susceptibility enhancement observed in optical measurements.
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5

Sullivan, Neil, Jaha Hamida, Khandker Muttalib, Subrahmanyam Pilla, and Edgar Genio. "Orientational Glasses: NMR and Electric Susceptibility Studies." Magnetochemistry 3, no. 4 (November 1, 2017): 33. http://dx.doi.org/10.3390/magnetochemistry3040033.

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6

Antoine, Rodolphe, Isabelle Compagnon, Driss Rayane, Michel Broyer, Philippe Dugourd, Gary Breaux, Frederick C. Hagemeister, David Pippen, Robert R. Hudgins, and Martin F. Jarrold. "Electric Susceptibility of Unsolvated Glycine-Based Peptides." Journal of the American Chemical Society 124, no. 23 (June 2002): 6737–41. http://dx.doi.org/10.1021/ja012656d.

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7

Panigrahi, N., T. Sahu, and P. K. Misra. "Theory of electric susceptibility of tetrahedral semiconductors." Journal of Physics C: Solid State Physics 18, no. 8 (March 20, 1985): L169—L173. http://dx.doi.org/10.1088/0022-3719/18/8/001.

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8

Castles, Flynn, Julian A. J. Fells, Dmitry Isakov, Stephen M. Morris, Andrew A. R. Watt, and Patrick S. Grant. "Active Metamaterials with Negative Static Electric Susceptibility." Advanced Materials 32, no. 9 (January 27, 2020): 1904863. http://dx.doi.org/10.1002/adma.201904863.

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9

Fuse, Takahiro, and Takashi Hotta. "Electric dipolar susceptibility of the Anderson-Holstein model." Journal of the Korean Physical Society 62, no. 12 (June 2013): 1874–78. http://dx.doi.org/10.3938/jkps.62.1874.

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10

Fukushima, Kenji, Dmitri E. Kharzeev, and Harmen J. Warringa. "Electric-current susceptibility and the Chiral Magnetic Effect." Nuclear Physics A 836, no. 3-4 (May 2010): 311–36. http://dx.doi.org/10.1016/j.nuclphysa.2010.02.003.

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11

Kliem, H., and B. Schumacher. "Time-Dependent Dielectric Susceptibility in High Electric Fields." IEEE Transactions on Electrical Insulation EI-22, no. 2 (April 1987): 219–24. http://dx.doi.org/10.1109/tei.1987.298886.

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12

M. Stadnik, Z., G. Stroink, G. Lamarche, and A. Inoue. "Electric Quadrupole Interactionsand Magnetic Susceptibility of Icosahedral Al70Fe20Ta10." Journal of the Physical Society of Japan 60, no. 11 (November 15, 1991): 3829–36. http://dx.doi.org/10.1143/jpsj.60.3829.

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13

Ribić-Zelenović, L., R. Simeunović, A. Maričić, and M. Spasojević. "The Effect of Temperature on the Magnetic Properties of the Electrochemically Obtained Ni92.8 Mo7.2 Powder Pressed at Different Pressures." Materials Science Forum 555 (September 2007): 539–43. http://dx.doi.org/10.4028/www.scientific.net/msf.555.539.

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The Ni92.8Mo7.2 alloy powder was obtained by electrochemical codeposition from an ammonium solution of NiSO4 and (NH4)6 Mo7O24 at j = 100 mA m-2, on a titanium cathode. DSC measurements and determination of the dependence of electrical resistivity on temperature did not reveal any changes in powder structure in the temperature range from 293 to 460 K. Therefore, in this range, there was no significant change in magnetic susceptibility either. Structural relaxation took place in the temperature interval from 460 to 560 K causing an increase in magnetic susceptibility. At temperatures higher than 570 K, magnetic susceptibility rapidly decreased. The Curie temperature of the powder was 660 K. With the increasing powder pressing pressure the magnetic susceptibility increased while the electric resistivity decreased. With the pressing pressure increase, the pore size was decreased and a better contact between powder particles was established. This caused electrical resistivity decrease and magnetic susceptibility increase.
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14

Nogi, Yasuyuki, Kiyomitsu Suzuki, and Yasunori Ohkuma. "Measurement of electric fields and estimation of dielectric susceptibility." American Journal of Physics 81, no. 5 (May 2013): 359–65. http://dx.doi.org/10.1119/1.4793439.

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15

Eilmes, A., R. W. Munn, V. G. Mavrantzas, D. N. Theodorou, and A. Góra. "Microscopic calculation of the static electric susceptibility of polyethylene." Journal of Chemical Physics 119, no. 21 (December 2003): 11458–66. http://dx.doi.org/10.1063/1.1623181.

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16

Hemberger, J., P. Lunkenheimer, R. Viana, R. Böhmer, and A. Loidl. "Electric-field-dependent dielectric constant and nonlinear susceptibility inSrTiO3." Physical Review B 52, no. 18 (November 1, 1995): 13159–62. http://dx.doi.org/10.1103/physrevb.52.13159.

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17

Rayane, D., A. R. Allouche, R. Antoine, I. Compagnon, M. Broyer, and Ph Dugourd. "Susceptibility and electric dipole in metal C 60 compounds." European Physical Journal D - Atomic, Molecular and Optical Physics 24, no. 1-3 (June 1, 2003): 9–13. http://dx.doi.org/10.1140/epjd/e2003-00134-5.

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18

Aiello, Orazio. "Electromagnetic Susceptibility of Battery Management Systems’ ICs for Electric Vehicles: Experimental Study." Electronics 9, no. 3 (March 19, 2020): 510. http://dx.doi.org/10.3390/electronics9030510.

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The paper deals with the susceptibility to electromagnetic interference (EMI) of battery management systems (BMSs) for Li-ion and lithium-polymer (LiPo) battery packs employed in emerging electric and hybrid electric vehicles. A specific test board was developed to experimentally assess the EMI susceptibility of a BMS front-end integrated circuit by direct power injection (DPI) and radiated susceptibility measurements in an anechoic chamber. Experimental results are discussed in reference to the different setup, highlighting the related EMI-induced failure mechanisms observed during the tests.
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19

Bodea, D., and A. Würger. "Magnetic-Field Dependence of the Static Electric Susceptibility of Glasses." Journal of Low Temperature Physics 136, no. 1/2 (July 2004): 39–56. http://dx.doi.org/10.1023/b:jolt.0000035370.58870.d4.

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20

Carrera, Álvaro, Marcos Mobbili, and Ernesto Marceca. "Electric Susceptibility of Sodium-Doped Water Clusters by Beam Deflection." Journal of Physical Chemistry A 113, no. 12 (March 26, 2009): 2711–14. http://dx.doi.org/10.1021/jp809411p.

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21

Kawamori, E. "Electric susceptibility of a magnetized plasma under electromagnetically induced transparency." Plasma Physics and Controlled Fusion 53, no. 8 (June 16, 2011): 085015. http://dx.doi.org/10.1088/0741-3335/53/8/085015.

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22

Phillips, Philip. "Magnetic susceptibility of hopping electrons in a strong electric field." Physical Review B 49, no. 6 (February 1, 1994): 4303–4. http://dx.doi.org/10.1103/physrevb.49.4303.

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23

Kahle, H. G., S. Bluck, and A. Kasten. "Simultaneous measurement of magnetic and magneto-electric susceptibility in TbPO4." Journal of Magnetism and Magnetic Materials 54-57 (February 1986): 1327–28. http://dx.doi.org/10.1016/0304-8853(86)90840-1.

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24

BÖHM, A., A. GRAUEL, N. SATO, C. SCHANK, C. GEIBEL, T. KOMATSUBARA, G. WEBER, and F. STEGLICH. "CRYSTALLINE ELECTRIC FIELD EFFECTS IN UPd2Al3." International Journal of Modern Physics B 07, no. 01n03 (January 1993): 34–37. http://dx.doi.org/10.1142/s0217979293000093.

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The temperature dependencies of the specific heat and the anisotropic magnetic susceptibility of the heavy-fermion superconductor UPd 2 Al 3 show distinct anomalies which can be described by a crystalline electric field (CEF) model for Uranium with hexagonal site symmetry. We find that a CEF-level scheme for the 3 H 4 multiplet ( 5f 2 configuration) implying two low lying singlets surprisingly well fits the experimental results.
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25

Krause, H., and D. H. Sutter. "The Molecular Zeeman Effect of Imines. I. Methanimine, its Molecular g-Tensor, its Magnetic Susceptibility Anisotropies, its Molecular Electric Quadrupole Moment, its Electric Field Gradient at the Nitrogen Nucleus, and its Nitrogen Spin-Rotation Coupling." Zeitschrift für Naturforschung A 44, no. 11 (November 1, 1989): 1063–78. http://dx.doi.org/10.1515/zna-1989-1106.

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Abstract The rotational Zeeman effect has been observed in methanimine which was produced from ethylenediamine by flash pyrolysis. The observed vibronic ground state expectation values of the molecular g-values, the magnetic susceptibility anisotropies and the molecular electric quadrupole moments are: gaa = -1.27099(22), gbb= -0.18975(7), gcc= -0.03440(8), 2ξaa-ξbb-ξcc = 12.49(19) · 10-6 ergG-2mol-1, 2ξbb-ξcc-ξaa = 5.22(11) · 10-6 ergG-2 mol-1 Qaa = 0.43(17) · 10-26esu cm2, Qbb= 1.08(10) · 10-26 esu cm2, and Qcc= -1.51 (26) . 10-26 esu cm2. With the TZVP ab initio value for the out-off plane electronic second moment as additional input, reliable values can be given also for the individual components of the magnetic susceptibility tensor and for the bulk susceptibility:ξ = (ξaa + ξbb + ξcc)/3=-13.13(88) · 10-6 erg G -2 mol-1. From low-J a-and b-type zero field transitions the spin-rotation coupling constants and the 14N nuclear quadrupole coupling constants could be redetermined with improved accuracy. These data are compared with our new theoretical results.
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26

ISRAELOFF, N. E., P. S. CRIDER, and M. E. MAJEWSKI. "SPATIO-TEMPORAL THERMAL FLUCTUATIONS AND LOCAL SUSCEPTIBILITY IN DISORDERED POLYMERS." Fluctuation and Noise Letters 07, no. 03 (September 2007): L239—L247. http://dx.doi.org/10.1142/s0219477507003891.

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Spatial and temporal fluctuations of the electric polarization were imaged in polymer thin films near the glass transition using electric force microscopy. Below the glass transition the fluctuations are quasi-static and spatial fluctuations were found to quantitatively agree with predictions for thermal fluctuations. Temporal fluctuations appear near the glass transition. Images of the space-time nanoscale dynamics near the glass transition are produced and analyzed. Local, complex dielectric susceptibility was also studied, and shows that dynamics on the free-surface are faster relative to the bulk.
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27

Mohammadi, Aliasghar, and Reghan J. Hill. "Steady electrical and micro-rheological response functions for uncharged colloidal inclusions in polyelectrolyte hydrogels." Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences 466, no. 2113 (October 7, 2009): 213–35. http://dx.doi.org/10.1098/rspa.2009.0286.

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The electric-field-induced response of an uncharged colloidal sphere embedded in a quenched polyelectrolyte hydrogel is calculated from a model where the polymer network is treated as an elastic, porous skeleton saturated with an aqueous electrolyte. We present exact analytical solutions for the steady response to a uniform electric field, as well as the steady susceptibility, defined as the ratio of the particle displacement to the strength of an optical or magnetic force. Even though the particle is uncharged, it attains a finite electric-field-induced displacement owing to hydrodynamic coupling with electroosmotic flow. The steady susceptibility decreases with increasing charge and decreasing electrolyte concentration; in general, charge imparts a small correction to the classical theory for an uncharged linearly elastic continuum.
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28

Yang, Chun, Yukihiko Shirayama, Ji-Chun Zhang, Qian Ren, and Kenji Hashimoto. "Peripheral interleukin-6 promotes resilience versus susceptibility to inescapable electric stress." Acta Neuropsychiatrica 27, no. 5 (May 28, 2015): 312–16. http://dx.doi.org/10.1017/neu.2015.36.

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ObjectiveAccumulating evidences suggest that pro-inflammatory cytokines such as interleukin-6 (IL-6) play a role in the pathophysiology of depression. In the learned helplessness (LH) paradigm, ~35% rats are resilient to inescapable stress.MethodsLevels of IL-6 in the serum and medial prefrontal cortex (mPFC) of LH rats (susceptible) and non-LH rats (resilience) were measured using enzyme-linked immunosorbent assay and western blot analysis, respectively.ResultsSerum levels of IL-6 in the LH rats were significantly higher than those of control and non-LH rats. In contrast, tissue levels of IL-6 in the mPFC were not different among three groups.ConclusionThe results suggest that peripheral IL-6 may contribute to resilience versus susceptibility to inescapable stress.
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29

Kishida, H., T. Hasegawa, Y. Iwasa, T. Koda, and Y. Tokura. "Dispersion relation in the third-order electric susceptibility for polysilane film." Physical Review Letters 70, no. 24 (June 14, 1993): 3724–27. http://dx.doi.org/10.1103/physrevlett.70.3724.

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30

Koo, Je Huan. "Negative electric susceptibility and magnetism from translational invariance and rotational invariance." Journal of Magnetism and Magnetic Materials 375 (February 2015): 106–10. http://dx.doi.org/10.1016/j.jmmm.2014.10.009.

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31

Mitra, B., A. Ghoshal, and K. P. Ghatak. "On the Electric Susceptibility Mass in Bi under Arbitrary Magnetic Quantization." physica status solidi (b) 155, no. 1 (September 1, 1989): K23—K27. http://dx.doi.org/10.1002/pssb.2221550140.

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32

Rajňák, M., B. Dolník, J. Kováč, K. Paulovičová, Z. Mitróová, J. Kurimský, R. Cimbala, P. Kopčanský, and M. Timko. "AC Magnetic Susceptibility of Ferrofluids Exposed to an External Electric Field." Acta Physica Polonica A 131, no. 4 (April 2017): 887–89. http://dx.doi.org/10.12693/aphyspola.131.887.

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33

Lim, Kok-Geng, Khian-Hooi Chew, Lye-Hock Ong, and Makoto Iwata. "Modulated internal electric field, dielectric susceptibility and polarization in ferroelectric superlattices." Ceramics International 39 (May 2013): S307—S310. http://dx.doi.org/10.1016/j.ceramint.2012.10.083.

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34

Czajkowski, G. "Excitonic susceptibility of semiconducting crystals influenced by a uniform electric field." Il Nuovo Cimento D 9, no. 12 (December 1987): 1545–49. http://dx.doi.org/10.1007/bf02451135.

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35

Huang, Bo-Jie, and Chyh-Hong Chern. "Deconfinement of electric charges in hydrogen-bonded ferroelectrics." International Journal of Modern Physics B 31, no. 20 (August 10, 2017): 1750130. http://dx.doi.org/10.1142/s0217979217501302.

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In addition to the gauge charges, a new charge degree of freedom is identified in the deconfined phase in the lattice Ising gauge theory. While applying to the hydrogen-bonded ferroelectrics, the new charge is essentially the electric charge, leading to the divergent dielectric susceptibility. The new degree of freedom paves an experimentally accessible way to identify the deconfined phase in the lattice Ising gauge theory.
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36

Webb, J. F. "A General Approach to Perturbation Theoretic Analysis in Nonlinear Optics and its Application to Ferroelectrics and Antiferroelectrics." International Journal of Modern Physics B 17, no. 22n24 (September 30, 2003): 4355–60. http://dx.doi.org/10.1142/s0217979203022441.

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Perturbation analysis in which the time variation of an electric field applied to a dielectric is treated as inducing a weakly nonlinear response expressed as a Taylor series expansion, is a standard technique for deriving the nonlinear susceptibility coefficients that relate the applied electric field to the polarization in the dielectric. In this paper a generalized method incorporating Fourier analysis is employed to treat a one-dimensional dynamical system subject to a time dependent driving force consisting of a superposition of monochromatic plane waves. It is then shown how this method can be applied to the calculation of nonlinear susceptibility coefficients, of any order, in bulk ferroelectric and antiferroelectric materials.
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37

Kazemiroodsari, Hadi, Mishac K. Yegian, Akram N. Alshawabkeh, and Seda Gokyer. "Electric Conductivity Probes to Study Change in Degree of Saturation - Bench Top Laboratory Tests." E3S Web of Conferences 195 (2020): 03016. http://dx.doi.org/10.1051/e3sconf/202019503016.

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Sand characteristics such as liquefaction susceptibility can be affected as a result of change in degree of saturation of sand. New liquefaction mitigation technique by inducing partial saturation in sands is introduced by Yegian et al in 2007[1]. This technique requires to monitor changes in degree of saturation of sand. By nature, changes in degree of saturation of sand can lead in changes in its electric conductivity. Electric conductivity is the property of a material that represents its ability to conduct electric current. Fully saturated sand can conduct electric current better than sand with lower degree of saturation. Therefore, the change in measured electric conductivity can be used to calculate the change in degree of saturation of sand. In 1942, Gus Archie [2] expressed that the electric conductivity of soil is a function of its porosity, degree of saturation, tortuosity and electric conductivity of pore fluid. Using Archie’s law electrical conductivity can be related to the degree of saturation in sands. Typically, electric conductivity probes and meters are instruments which are used to measure electric conductivity. Using electrical conductivity probes, sets of bench top tests were conducted on Ottawa sand to study the relation between degree of saturation and electric conductivity in sand. Partial saturation in sands were created by pouring dry sand into sodium percarbonate solution with a known initial concentration. By nature, sodium percarbonate in water, generates oxygen gas bubbles in time. The changes in electric conductivity in the specimen were measured using electric conductivity meters and probes. In addition, changes in degree of saturation of the specimen were measured using soil phase relations equations. Measured electric conductivity data and calculated degree of saturations were correlated to explore relation between electric conductivity and degree of saturation. This paper presents results of bench top tests, and suggests a relationship between, final degree of saturation of sand and initial concentration of sodium percarbonate solution
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38

Wieczorek, Jakub, Tomasz Maciąg, Karolina Kowalczyk, and Damian Migas. "Evaluation of thermal properties of MMCp composites with silver alloy matrix." Journal of Thermal Analysis and Calorimetry 142, no. 1 (May 13, 2020): 175–82. http://dx.doi.org/10.1007/s10973-020-09741-5.

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Abstract Silver, silver alloys, and composites with silver matrix are used mainly as electric contacts, circuit-breakers, and slide bearings. Contacts working conditions require as high as possible thermal and electrical conductivity, wear resistance during electric arc work, low susceptibility to tacking, and chemical stability. Unreinforced silver alloys do not meet those expectations, hence increasing interest in metal matrix composites. Reinforcing with ceramic particles improves tribological wear resistance and minimizes formability of silver alloys. At the same time, introduction of ceramic particles decreases thermal and electrical conductivity. In this paper, manufacturing method of silver-based composites reinforced with particles Al2O3, SiC, and glassy carbon was described. Composites were subjected to differential thermal analysis. Furthermore, thermal diffusivity measurements using laser flash method, as well as measurements of linear thermal expansion coefficient using dilatometric method were performed in order to determine heat conductivity of the prepared composites.
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39

Blanc, François, René Fanguin, Gaston Raoult, Jean-Claude Labrune, Germaine Lomaglio, and Jean-Gérard Theobald. "Susceptibilité radiofréquence d'une jonction vis-à-vis d'un champ électrique parallèle au plan métallurgique." Canadian Journal of Physics 66, no. 1 (January 1, 1988): 11–16. http://dx.doi.org/10.1139/p88-003.

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When an alternating electric field is applied parallel to a junction, the radiofrequency susceptibility gives an absorption having a maximum versus the direct current polarization of the junction; the real part of the susceptibility is negative. The explanation of both features involves an internal field parallel to the alternating field. The experiment allows the measurement of the concentration of minority carriers.
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40

Klesing, Armin, and Dieter H. Sutter. "The Rotational Zeeman Effect of Carbonylselenide, OCSe, its Molecular Electric Quadrupole Moment, and the Effects of the C = Se Stretching and the Bending Vibration; A High Resolution Microwave Fourier Transform Study." Zeitschrift für Naturforschung A 48, no. 10 (October 1, 1993): 968–86. http://dx.doi.org/10.1515/zna-1993-1004.

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Abstract The results of a high resolution microwave Fourier transform study of the rotational Zeeman effect in the J' = 2￫J" = l transitions of 16O12C80Se, 16O12C78Se, and 16O12C77 Se are reported. From the observed g-values and susceptibility anisotropies, experimental values were derived for the molecular electric quadrupole moment, for the anisotropy in the second moments of the electronic charge distribution, for the paramagnetic susceptibility perpendicular to the OCSe chain, and for the sign of the electric dipole moment. From the Zeeman data observed for the /-type doublet, the paramagnetic susceptibility parallel to the OCSe-axis, which by symmetry is zero for the linear configuration, could be derived as a function of the bending angle, ß. Ab initio calculations of the molecular electric quadrupole moment were carried out. Fair agreement with the experimental value was obtained at the CID/LANLIDZ + pol level of computation.The Lorentz-Stark effect, which usually leads to perturbations in the Zeeman patterns of /-type doublet lines, vanishes if data collection starts with a delay 2 μs after the end of the exciting pulses. This finding is attributed to the short collisional lifetime of fast molecules and suggests new experiments in the field of rotational relaxation studies.
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41

KHADRE, M. A., and A. E. YOUSEF. "Susceptibility of Human Rotavirus to Ozone, High Pressure, and Pulsed Electric Field." Journal of Food Protection 65, no. 9 (September 1, 2002): 1441–46. http://dx.doi.org/10.4315/0362-028x-65.9.1441.

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The rotavirus causes a food-transmitted gastroenteritis that affects mainly children. Currently, the food industry is interested in alternative food-processing technologies, but research on the control of food-transmitted viruses by these technologies is limited. In this study, the human rotavirus was cultured on MA104 cells, and suspensions of the virus were prepared and treated with ozone, high pressure, and pulsed electric field (PEF). Virus viability was quantified as 50% tissue culture infectious doses (TCID50) per milliliter. Ozone at 25 μg/ml decreased rotavirus infectivity by 8 to 9 log10 TCID50/ml. High pressure was extremely effective against the rotavirus; treatment with 300 MPa for 2 min at 25°C inactivated ~8 log10 TCID50/ml. A small fraction of the virus population, however, remained resistant to pressure treatments of up to 800 MPa for 10 min. Viruses surviving these extreme pressures showed a cytopathic effect different from that of the untreated viruses. The rotavirus was found to be resistant to PEF treatment at 20 to 29 kV/cm, for which no appreciable reductions in virus titer were observed.
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42

Abdullah, M., Farah T. Mohammed Noori, and Amin H. Al-Khursan. "Second-order nonlinear susceptibility in quantum dot structure under applied electric field." Superlattices and Microstructures 82 (June 2015): 219–33. http://dx.doi.org/10.1016/j.spmi.2015.01.041.

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43

Umar, S. A., M. K. Halimah, K. T. Chan, and A. A. Latif. "Polarizability, optical basicity and electric susceptibility of Er3+ doped silicate borotellurite glasses." Journal of Non-Crystalline Solids 471 (September 2017): 101–9. http://dx.doi.org/10.1016/j.jnoncrysol.2017.05.018.

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Abreu Santos, H. "Second order mesoscopic electric susceptibility in Al Ga1−As/GaAs quantum wells." Microelectronic Engineering 43-44 (August 1998): 125–30. http://dx.doi.org/10.1016/s0167-9317(98)00154-3.

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Klein, Michael W. "Dielectric susceptibility and thermal conductivity of tunneling electric dipoles in alkali halides." Physical Review B 40, no. 3 (July 15, 1989): 1918–25. http://dx.doi.org/10.1103/physrevb.40.1918.

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Gluckstern, R. L., R. Li, and R. K. Cooper. "Electric polarizability and magnetic susceptibility of small holes in a thin screen." IEEE Transactions on Microwave Theory and Techniques 38, no. 2 (1990): 186–92. http://dx.doi.org/10.1109/22.46429.

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Margulis, V. A. "Magnetic susceptibility of a semiconductor superlattice under parallel electric and magnetic fields." Journal of Physics: Condensed Matter 7, no. 3 (January 16, 1995): 645–56. http://dx.doi.org/10.1088/0953-8984/7/3/018.

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Guseinov, G. G., S. S. Ragimov, J. Hasani Barbaran, and G. M. Agamirzoeva. "X-ray diffraction study, magnetic susceptibility, and electric properties of Cu3Fe0.5Se2 crystal." Crystallography Reports 55, no. 4 (July 2010): 673–75. http://dx.doi.org/10.1134/s1063774510040231.

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Dec, J., W. Kleemann, and M. Itoh. "Linear and Nonlinear Electric Susceptibility in the Quantum Domain State of SrTi18O3." Ferroelectrics 337, no. 1 (August 2006): 13–17. http://dx.doi.org/10.1080/00150190600713900.

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Hill, R. J. "Electric railway traction. Part 6: Electromagnetic compatibility disturbance - sources and equipment susceptibility." Power Engineering Journal 11, no. 1 (February 1, 1997): 31–39. http://dx.doi.org/10.1049/pe:19970107.

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