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Journal articles on the topic 'Magnetic stripe'

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1

Kong, Y. H., S. Y. Chen, G. L. Zhang, and X. Fu. "A Tunable 3-Terminal GMR Device Based on a Hybrid Magnetic-Electric-Barrier Nanostructure." Journal of Nanomaterials 2013 (2013): 1–5. http://dx.doi.org/10.1155/2013/316897.

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We propose a giant magnetoresistance (GMR) device, which can be experimentally realized by depositing two ferromagnetic (FM) strips and a Schottky metal (SM) stripe in parallel configuration on top of the GaAs heterostructure. The GMR effect ascribes a significant electron transmission difference between the parallel and antiparallel magnetization configurations of two FM stripes. Moreover, the MR ratio depends strongly on the magnetic strength of the magnetic barrier (MB) and the electric barrier (EB) height induced by an applied voltage to the SM stripe. Thus, this system can be used as a GM
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2

Karlický, M., and L. Yasnov. "Estimating density and magnetic field turbulence in solar flares using radio zebra observations." Astronomy & Astrophysics 638 (June 2020): A22. http://dx.doi.org/10.1051/0004-6361/202037936.

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Context. In solar flares the presence of magnetohydrodynamic turbulence is highly probable. However, information about this turbulence, especially the magnetic field turbulence, is still very limited. Aims. In this paper we present a new method for estimating levels of the density and magnetic field turbulence in time and space during solar flares at positions of radio zebra sources. Methods. First, considering the double-plasma resonance model of zebras, we describe a new method for determining the gyro-harmonic numbers of zebra stripes based on the assumption that the ratio R = Lb/Ln (Ln and
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3

Loktev, V. M., and V. Turkowski. "On the theory of nonhomogeneous nonequilibrium superconductivity in 2D systems with massless fermions." Low Temperature Physics 48, no. 5 (2022): 371–77. http://dx.doi.org/10.1063/10.0010200.

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We analyze static and nonequilibrium superconducting properties of a 2D relativistic-like model system with local electron-electron interaction, Rashba spin-orbit interaction α R in presence of time-dependent in-plane magnetic field H( t). It is shown that similar to the 2D case with ordinary massive quasiparticle dispersion [Formula: see text] at large fields, such a system demonstrates a nonhomogeneous superconducting stripe phase with the order parameter [Formula: see text] (B is the magnetic induction, υF is the Fermi velocity, n is the normal to the plane, μ B is the Bohr magneton, and [F
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4

McCord, Jeffrey, Burak Erkartal, Thomas von Hofe, et al. "Revisiting magnetic stripe domains — anisotropy gradient and stripe asymmetry." Journal of Applied Physics 113, no. 7 (2013): 073903. http://dx.doi.org/10.1063/1.4792517.

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5

Akimov, M. L., P. A. Polyakov, A. A. Banishev, and N. N. Usmanov. "Influence of asymmetrical location of magnetic impurities on domain walls local deformation." International Journal of Modern Physics B 33, no. 14 (2019): 1950142. http://dx.doi.org/10.1142/s021797921950142x.

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Magnetic ordering in a mixed domain structure composed of a stripe domain and asymmetrically localized magnetic impurity inside the stripe domain was investigated. The analytical expression for domain walls deformation mediated by the influence of the magnetostatic stray field of the asymmetrically localized magnetic impurity was obtained. The calculations were done for the magnetic film with parameters which are typical for films used in magnetic memory. Experimental implementation of the mixed domain structure composed of the stripe domain and asymmetrically localized magnetic impurity insid
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6

Karlický, M., and L. Yasnov. "Zebra-stripe sources in the double-plasma resonance model of solar radio zebras." Astronomy & Astrophysics 624 (April 2019): A119. http://dx.doi.org/10.1051/0004-6361/201935281.

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Context. Radio bursts with fine structures are used in diagnostics of solar flare plasmas, of which zebra structures are the most important. However, there is still a debate about their origin. Aims. The most probable model of zebras is that based on double-plasma resonance (DPR) instability. The paper wants to contribute to a verification of this model. Methods. We used analytical methods. Results. We studied the DPR model in two scenarios: a model with the zebra-stripe sources in a single loop and a model with the zebra-stripe sources moving through a fan of magnetic field lines. In the firs
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7

SIRONI, LORENZO, and ANATOLY SPITKOVSKY. "PARTICLE ACCELERATION AT THE TERMINATION SHOCK OF STRIPED PULSAR WINDS." International Journal of Modern Physics: Conference Series 08 (January 2012): 144–50. http://dx.doi.org/10.1142/s2010194512004539.

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The relativistic wind of pulsars consists of toroidal stripes of opposite magnetic field polarity, separated by current sheets of hot plasma. By means of multi-dimensional particle-in-cell simulations, we investigate particle acceleration and magnetic field dissipation at the termination shock of a relativistic striped pulsar wind. At the shock, the flow compresses and the alternating fields annihilate by driven magnetic reconnection. Irrespective of the stripe wavelength λ or the wind magnetization σ (in the regime σ ≫1 of magnetically dominated flows), shock-driven reconnection transfers all
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8

Park, Sul-Ah, Young-Woo Son, and Kang-Hun Ahn. "Stripe states in photonic honeycomb ribbon." Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences 471, no. 2177 (2015): 20140765. http://dx.doi.org/10.1098/rspa.2014.0765.

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We reveal new stripe states in deformed hexagonal array of photonic wave guides when the array is terminated to have a ribbon-shaped geometry. Unlike the well-known zero energy edge modes of honeycomb ribbon, the new one-dimensional states are shown to originate from high-energy saddle-shaped photonic bands of the ribbon's two-dimensional counterpart. We find that the strain field deforming the ribbon generates pseudo-electric fields in contrast to pseudo-magnetic fields in other hexagonal crystals. Thus, the stripe states experience Bloch oscillation without any actual electric field so that
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9

WRÓBEL, PIOTR, and ROBERT EDER. "STRIPE STABILITY IN DOPED ANTIFERROMAGNETS." International Journal of Modern Physics B 14, no. 29n31 (2000): 3765–70. http://dx.doi.org/10.1142/s0217979200004325.

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In the framework of the t-Jz we discuss localized spin polarons for various original hole arrangements in different spin backgrounds. According to the so-called string picture we assume that local destruction in the magnetic structure caused by hole motion tends to localize holes and acts on them as a kind of well potential. We concentrate on the case of the hole concentration 1/8 for which stripes are experimentally observed. We explicitly take into account interaction between holes and consider several possible configurations, that represent: holes homogeneously distributed in the antiferrom
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10

Zhang, Hedong, Yasunaga Mitsuya, Natsuko Fukuoka, and Kenji Fukuzawa. "Spreading Characteristics of Monolayer Lubricant Films on Surfaces With Lube Textures." Journal of Tribology 127, no. 1 (2005): 164–70. http://dx.doi.org/10.1115/1.1843828.

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In this paper, we investigate the effect of lube textures from the viewpoint of lubricant spreading. Lube textures, designating a patterned distribution of bonding strength between lubricant molecules and disk surface, were formed by irradiating ultraviolet rays through a stripe-patterned mask onto a magnetic disk surface which was partially coated with one-monolayer film of perfluoropolyether. Surface characteristics of the lube textures were evaluated by surface energies ascertained from contact angle measurements. Spreading of the lubricant film was measured by scanning microellipsometry on
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11

Egger, J., S. Michlmayr, R. Piepgras, J. H. Espina-Hernández, and B. Zagar. "A Faraday effect magnetic stripe scanner." Journal of Physics: Conference Series 1065 (August 2018): 032013. http://dx.doi.org/10.1088/1742-6596/1065/3/032013.

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12

Klauss, H. H., W. Wagener, W. Kopmann, et al. "Magnetic stripe order in La1.8−xEu0.2SrxCuO4." Physica B: Condensed Matter 312-313 (March 2002): 71–73. http://dx.doi.org/10.1016/s0921-4526(01)01277-7.

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13

Porrati, F., H. P. Oepen, and J. Kirschner. "Magnetic configurations in anisotropic stripe systems." Journal of Magnetism and Magnetic Materials 283, no. 2-3 (2004): 133–42. http://dx.doi.org/10.1016/j.jmmm.2004.05.014.

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14

Gorkov, Dmitry, Boris P. Toperverg, and Hartmut Zabel. "Artificial Magnetic Pattern Arrays Probed by Polarized Neutron Reflectivity." Nanomaterials 10, no. 5 (2020): 851. http://dx.doi.org/10.3390/nano10050851.

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Traditionally, neutron scattering is an essential method for the analysis of spin structures and spin excitations in bulk materials. Over the last 30 years, polarized neutron scattering in terms of reflectometry has also contributed largely to the analysis of magnetic thin films and magnetic multilayers. More recently it has been shown that polarized neutron reflectivity is, in addition, a suitable tool for the study of thin films laterally patterned with magnetic stripes or islands. We provide a brief overview of the fundamental properties of polarized neutron reflectivity, considering differ
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15

Saerbeck, Thomas, Henning Huckfeldt, Boris P. Toperverg, and Arno Ehresmann. "Magnetic Structure of Ion-Beam Imprinted Stripe Domains Determined by Neutron Scattering." Nanomaterials 10, no. 4 (2020): 752. http://dx.doi.org/10.3390/nano10040752.

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We present a detailed analysis of the in-plane magnetic vector configuration in head-to-head/tail-to-tail stripe domain patterns of nominal 5 μm width. The patterns have been created by He-ion bombardment induced magnetic patterning of a CoFe/IrMn3 exchange bias thin-film system. Quantitative information about the chemical and magnetic structure is obtained from polarized neutron reflectometry (PNR) and off-specular scattering (OSS). The technique provides information on the magnetic vector orientation and magnitude along the lateral coordinate of the sample, as well as the chemical and magnet
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16

Garnier, L. C., M. Eddrief, S. Fin, et al. "Perpendicular Magnetic Anisotropy in Fe–N Thin Films: Threshold Field for Irreversible Magnetic Stripe Domain Rotation." SPIN 06, no. 04 (2016): 1640014. http://dx.doi.org/10.1142/s2010324716400142.

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The magnetic properties of an iron nitride thin film obtained by ion implantation have been investigated. N[Formula: see text] ions were implanted in a pristine iron layer epitaxially grown on ZnSe/GaAs(001). X-ray diffraction measurements revealed the formation of body-centered tetragonal N-martensite whose [Formula: see text]-axis is perpendicular to the thin film plane and [Formula: see text]-parameter is close to that of [Formula: see text]-Fe8N. Magnetic measurements disclosed a weak perpendicular magnetic anisotropy (PMA) whose energy density [Formula: see text] was assessed to about 105
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17

Sornette, D. "Stripe magnetic domains and lyotropic liquid crystals." Journal de Physique 48, no. 9 (1987): 1413–17. http://dx.doi.org/10.1051/jphys:019870048090141300.

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18

Udalov, O. G., and I. S. Beloborodov. "Stripe structures in phase separated magnetic oxides." Journal of Physics: Condensed Matter 31, no. 41 (2019): 415801. http://dx.doi.org/10.1088/1361-648x/ab2e3e.

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19

Michelena, M. D., F. Montero, P. Sánchez, E. López, M. C. Sánchez, and C. Aroca. "Piezoelectric–magnetostrictive magnetic sensor using stripe actuators." Journal of Magnetism and Magnetic Materials 242-245 (April 2002): 1160–62. http://dx.doi.org/10.1016/s0304-8853(01)01294-x.

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20

Dufva, C., J. Bengtsson, M. Svensson, and A. Nilsson. "Forensic analysis of magnetic stripe skimmer devices." Forensic Science International: Genetics Supplement Series 3, no. 1 (2011): e385-e386. http://dx.doi.org/10.1016/j.fsigss.2011.09.054.

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21

Cebers, A. "Liquid magnetic stripe patterns and undulation instabilities." Journal of Magnetism and Magnetic Materials 149, no. 1-2 (1995): 93–96. http://dx.doi.org/10.1016/0304-8853(95)00345-2.

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22

Chen, J. P., Z. Q. Wang, J. J. Gong, et al. "Stripe-vortex transitions in ultrathin magnetic nanostructures." Journal of Applied Physics 113, no. 5 (2013): 054312. http://dx.doi.org/10.1063/1.4790483.

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23

Li, Yangmu, J. Terzic, P. G. Baity, et al. "Tuning from failed superconductor to failed insulator with magnetic field." Science Advances 5, no. 6 (2019): eaav7686. http://dx.doi.org/10.1126/sciadv.aav7686.

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Do charge modulations compete with electron pairing in high-temperature copper oxide superconductors? We investigated this question by suppressing superconductivity in a stripe-ordered cuprate compound at low temperature with high magnetic fields. With increasing field, loss of three-dimensional superconducting order is followed by reentrant two-dimensional superconductivity and then an ultraquantum metal phase. Circumstantial evidence suggests that the latter state is bosonic and associated with the charge stripes. These results provide experimental support to the theoretical perspective that
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24

Nakanishi, Kanji. "Locally Induced Magnetic Anisotropy in Stripe Amorphous Soft Magnetic Film." IEEJ Transactions on Fundamentals and Materials 114, no. 11 (1994): 774–79. http://dx.doi.org/10.1541/ieejfms1990.114.11_774.

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25

Karlický, M., and L. V. Yasnov. "Spatial quasi-periodic variations of the plasma density and magnetic field in zebra radio sources." Astronomy & Astrophysics 646 (February 2021): A179. http://dx.doi.org/10.1051/0004-6361/202039850.

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Context. Radio bursts and their fine structures are an integral part of solar flares. Fine structures in particular are used for diagnostics of solar flare processes. The so-called zebras belong to the most important of such fine structures. Aims. We analyze seven zebra events in order to search for spatial variations in the plasma density and magnetic field in zebra-stripe sources. Methods. We used an improved method for estimating the gyroharmonic numbers of zebra-stripe frequencies. We compared observed zebra-stripe frequencies with those calculated in the zebra model. The differences in th
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26

Zhang, Yin Long, Wei Jiang, and Long Lin. "Composition - Property Relationships of Magnetic Inks for Screen Printing." Applied Mechanics and Materials 477-478 (December 2013): 1464–76. http://dx.doi.org/10.4028/www.scientific.net/amm.477-478.1464.

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Magnetic cards are widely used as credit cards, gift cards and VIP cards. In many industries, the principal method for producing the magnetic stripe still employs magnetic tapes. Therefore, if magnetic inks could be printed directly on the poly (vinyl chloride) (PVC) cards, then there would be the potential to improve industrial efficiency significantly. In order to apply the magnetic inks to the credit cards or other PVC cards, the Screen printing technique was chosen as a suitable printing method.In formulation 19, it is easy to mix and disperse the iron oxide powders in binder, few agglomer
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27

Zhang, Fan. "A Magnetospheric Dichotomy for Pulsars with Extreme Inclinations." Universe 7, no. 12 (2021): 455. http://dx.doi.org/10.3390/universe7120455.

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In this work, we expand on a comment by Lyne et al. (2017), that intermittent pulsars tend to congregate near a stripe in the logarithmic period versus period-derivative diagram. Such a stripe represents a small range of polar cap electric potential. Taking into account also the fact (already apparent in their Figure 7, but not explicitly stated there) that high-fraction nulling pulsars also tend to reside within this and an additional stripe, we make the observation that the two stripes further match the “death lines” for double- and single-pole interpulses, associated with nearly orthogonal
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28

LI, CHUN-SHU, YONG-HONG KONG, WEI-HUA TANG, and GUI-LIAN ZHANG. "MAGNETORESISTANCE EFFECT IN A MAGNETIC–ELECTRIC-BARRIER STRUCTURE." Surface Review and Letters 14, no. 02 (2007): 255–60. http://dx.doi.org/10.1142/s0218625x07009335.

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A Magnetoresistance device is proposed in a both magnetically and electrically modulated two-dimensional electron gas, which can be realized experimentally by the deposition, on the top and bottom of a semiconductor heterostructure, of two parallel metallic ferromagnetic strips under an applied voltage. It is shown that a considerable magnetoresistance effect can be achieved in such a device due to the significant transmission difference for electrons through parallel and antiparallel magnetization configurations. It is also shown that the magnetoresistance ratio depends strongly on the applie
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29

Freeman, P. G., S. M. Hayden, R. A. Mole, M. Enderle, D. Prabhakaran, and A. T. Boothroyd. "Evidence of Magnetic Correlations Among the Charge Stripe Electrons of Charge-Stripe Ordered La2NiO4.11." Journal of Physics: Conference Series 340 (February 8, 2012): 012060. http://dx.doi.org/10.1088/1742-6596/340/1/012060.

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30

Akimov, M. L., P. A. Polyakov, and N. E. Rusakova. "A mixed domain structure in magnetic films with large anisotropy." International Journal of Modern Physics B 32, no. 01 (2018): 1750272. http://dx.doi.org/10.1142/s0217979217502721.

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Influence of anisotropy on a bending of a magnetic stripe domain wall due to a magnetostatic stray field of a cylindrical magnetic domain (CMD) that is located within the stripe one is under investigation. It is revealed that for a specific set of physical parameters of the domain structure, energy of domain wall bending anisotropy can suppress the bending. An analytical expression for the bending shape is obtained on account of a change of both magnetostatic energy of the configuration and energy of anisotropy of the domain wall.
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31

Zablotskii, V., Andrzej Maziewski, and T. Polyakova. "Thermal-Driven Evolution of Magnetic Domain Structures in Ultrathin Films." Solid State Phenomena 112 (May 2006): 101–8. http://dx.doi.org/10.4028/www.scientific.net/ssp.112.101.

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The thermal-driven evolution of stripe domain structures in ultrathin magnetic films is analyzed with regard to temperature dependencies of the film magnetic parameters. In the vicinity of the Curie temperature or points of the spin reorientation the equilibrium stripe domain period was found to exponentially decrease with increasing temperature. It is shown that the temperature dependence of the characteristic length is the key parameter controlling the domain period changes. Irreversible and reversible changes of the domain period as well as the so-called inverse domain melting are discussed
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32

LU, MAO-WANG. "ELECTRON-SPIN POLARIZATION IN BOTH MAGNETICALLY AND ELECTRICALLY-MODULATED NANOSTRUCTURES." Surface Review and Letters 12, no. 01 (2005): 67–74. http://dx.doi.org/10.1142/s0218625x05006780.

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We theoretically investigate the spin-dependent transport properties of electrons in realistic magnetic-electric barrier nanostructures, which are produced by the deposition, on top of a heterostructure, of a metallic ferromagnetic stripe with an applied voltage. The degree of the electron-spin polarization is found to be closely associated with this voltage, although the use of applied voltage itself induces no spin polarization effect. As a positive voltage is applied to the stripe the electron-spin polarization shifts towards the low-energy region and increases; it shifts towards the high-e
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33

Fedulov, F. A., D. V. Saveliev, D. V. Chashin, V. I. Shishkin, and Yu K. Fetisov. "Magnetoelectric effects in stripe- and periodic heterostructures based on nickel–lead zirconate titanate bilayers." Russian Technological Journal 10, no. 3 (2022): 64–73. http://dx.doi.org/10.32362/2500-316x-2022-10-3-64-73.

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Objectives. A topical task in the design of magnetoelectric (ME) devices based on composite ferromagnetic– piezoelectric heterostructures involves reducing their dimensions to increase their operating frequencies and optimize their integration in modern electronics. The study set out to investigate the influence of in-plane dimensions on the characteristics of ME effects in stripe and periodic nickel–lead zirconate titanate heterostructures manufactured via electrolytic deposition.Methods. Lead zirconate titanate disks with Ag-electrodes were used for manufacturing the ME heterostructures; Ni
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34

Choe, Sug-Bong, and Sung-Chul Shin. "Stability of stripe magnetic domain in magnetic multilayers: Prediction and observation." Physical Review B 59, no. 1 (1999): 142–45. http://dx.doi.org/10.1103/physrevb.59.142.

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35

Zhu, Zengtai, Hongmei Feng, Xiaohong Cheng, Hongkang Xie, Qingfang Liu, and Jianbo Wang. "Static and dynamic magnetic properties of stripe-patterned Fe20Ni80soft magnetic films." Journal of Physics D: Applied Physics 51, no. 4 (2018): 045004. http://dx.doi.org/10.1088/1361-6463/aa9dfa.

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36

Kalyabin, D. V., A. V. Sadovnikov, E. N. Beginin, and S. A. Nikitov. "Surface spin waves propagation in tapered magnetic stripe." Journal of Applied Physics 126, no. 17 (2019): 173907. http://dx.doi.org/10.1063/1.5099358.

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37

Smith, D. F., T. Donnelly, and D. J. Mapps. "High density storage on a magnetic stripe card." IEEE Transactions on Magnetics 32, no. 5 (1996): 4025–27. http://dx.doi.org/10.1109/20.539252.

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38

Álvarez, N. R., J. E. Gómez, M. Vásquez Mansilla, et al. "Magnetic coupling of stripe domains in FePt/Ni80Fe20bilayers." Journal of Physics D: Applied Physics 50, no. 11 (2017): 115001. http://dx.doi.org/10.1088/1361-6463/aa5bce.

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39

Ghising, Pramod, Z. Hossain, and R. C. Budhani. "Stripe magnetic domains in CeY2Fe5O12 (Ce:YIG) epitaxial films." Applied Physics Letters 110, no. 1 (2017): 012406. http://dx.doi.org/10.1063/1.4973481.

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40

Szuszkiewicz, W., K. Fronc, B. Hennion, F. Ott, and M. Aleszkiewicz. "Magnetic stripe domains in Fe/Fe–N multilayers." Journal of Alloys and Compounds 423, no. 1-2 (2006): 172–75. http://dx.doi.org/10.1016/j.jallcom.2006.01.091.

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41

Christie, I. M., A. Lalakos, A. Tchekhovskoy, et al. "The role of magnetic field geometry in the evolution of neutron star merger accretion discs." Monthly Notices of the Royal Astronomical Society 490, no. 4 (2019): 4811–25. http://dx.doi.org/10.1093/mnras/stz2552.

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ABSTRACT Neutron star mergers are unique laboratories of accretion, ejection, and r-process nucleosynthesis. We used 3D general relativistic magnetohydrodynamic simulations to study the role of the post-merger magnetic geometry in the evolution of merger remnant discs around stationary Kerr black holes. Our simulations fully capture mass accretion, ejection, and jet production, owing to their exceptionally long duration exceeding 4 s. Poloidal post-merger magnetic field configurations produce jets with energies Ejet ∼ (4–30) × 1050 erg, isotropic equivalent energies Eiso ∼ (4–20) × 1052 erg, o
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42

Moshchalkov, V. V., L. Trappeniers, G. Teniers, J. Vanacken, P. Wagner, and Y. Bruynseraede. "Stripe formation and disorder induced stripe fragmentation." Physica C: Superconductivity 341-348 (November 2000): 1799–802. http://dx.doi.org/10.1016/s0921-4534(00)01087-x.

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43

CHEN, YAN, Z. D. WANG, and C. S. TING. "NOVEL VORTEX STRIPE PHASE UNDER STRONG MAGNETIC FIELD IN HIGH TEMPERATURE SUPERCONDUCTORS." International Journal of Modern Physics B 19, no. 01n03 (2005): 9–12. http://dx.doi.org/10.1142/s021797920502786x.

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The nature of vortex structure in the mixed state of high-temperature superconductors (HTS) is investigated by solving the Bogoliubov-de Gennes equations with consideration of competition between antiferromagnetic (AF) and d-wave superconductivity (DSC) orders. By varying the applied magnetic field and temperature, the geometry of vortex structure can take two different forms: conventional vortex lattice (triangular or square), or vortex stripe phases where all the order parameters including spin density wave, charge density wave and superconducting order exhibit stripe-like behavior. This nov
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44

Gavrichkov, Vladimir A., and Semyon I. Polukeev. "Magnetic Interaction in Doped 2D Perovskite Cuprates with Nanoscale Inhomogeneity: Lattice Nonlocal Effects vs. Superexchange." Condensed Matter 7, no. 4 (2022): 57. http://dx.doi.org/10.3390/condmat7040057.

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We have studied the superexchange interaction Jij in doped 2D cuprates. The AFM interaction strongly depends on the state of the lattice of a CuO2 layer surrounded by two LaO rock salt layers. In a static U and D stripe nanostructure, the homogeneous AFM interaction is impossible due to the U/D/U… periodic stripe sequence and TN=0. In a dynamic stripe nanostructure, the ideal CuO2 layer with nonlocal effects and the homogeneous AFM interaction are restored. However, the interaction Jij decreases by the exponential factor due to partial dynamic quenching. The meaning of the transition from the
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45

MIKHAILOV, S. A., and N. A. SAVOSTIANOVA. "MICROWAVE RESPONSE OF A TWO-DIMENSIONAL ELECTRON STRIPE: ELECTRODYNAMIC EFFECTS AND THE INFLUENCE OF CONTACTS." International Journal of Modern Physics B 21, no. 08n09 (2007): 1497–501. http://dx.doi.org/10.1142/s0217979207043087.

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Microwave response of a two-dimensional (2D) electron stripe, supplied by two semi-infinite side contacts, is theoretically studied taking into account retardation and radiative effects. Absorption spectra of the stripe are calculated as a function of the microwave frequency ω, magnetic field B, parameters of the 2D electron gas and of the contacts. It is shown that the contacts substantially modify the position, the linewidth and the strength of the absorption resonances, leading for instance to the inversion of the ab-sorption maxima of the right and left circularly polarized radiation in ma
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46

Roussigné, Y., S. M. Chérif, and P. Moch. "Spin waves in a magnetic stripe submitted to a perpendicular magnetic field." Journal of Magnetism and Magnetic Materials 268, no. 1-2 (2004): 89–94. http://dx.doi.org/10.1016/s0304-8853(03)00477-3.

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Bauer, Andreas, Gereon Meyer, Tristan Crecelius, Irene Mauch, and Günter Kaindl. "Magnetic stripe domains in ultrathin films and their transformation in magnetic fields." Journal of Magnetism and Magnetic Materials 282 (November 2004): 252–55. http://dx.doi.org/10.1016/j.jmmm.2004.04.057.

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FU, Qin-wei, Xuan DU, Yan ZHANG, Na LÜ, Wei TAO, and Hui ZHAO. "Extraction of laser stripe center on translucent glue strip surface." Optics and Precision Engineering 29, no. 4 (2021): 701–9. http://dx.doi.org/10.37188/ope.20212904.0701.

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Zhang, Junjie, Yu-Sheng Chen, D. Phelan, Hong Zheng, M. R. Norman, and J. F. Mitchell. "Stacked charge stripes in the quasi-2D trilayer nickelate La4Ni3O8." Proceedings of the National Academy of Sciences 113, no. 32 (2016): 8945–50. http://dx.doi.org/10.1073/pnas.1606637113.

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Abstract:
The quasi-2D nickelate La4Ni3O8 (La-438), consisting of trilayer networks of square planar Ni ions, is a member of the so-called T′ family, which is derived from the Ruddlesden–Popper (R-P) parent compound La4Ni3O10−x by removing two oxygen atoms and rearranging the rock salt layers to fluorite-type layers. Although previous studies on polycrystalline samples have identified a 105-K phase transition with a pronounced electronic and magnetic response but weak lattice character, no consensus on the origin of this transition has been reached. Here, we show using synchrotron X-ray diffraction on h
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Bisero, Diego. "A first-principle model of the magnetic contrast in ultrathin films with perpendicular magnetization." Modern Physics Letters B 31, no. 09 (2017): 1750088. http://dx.doi.org/10.1142/s0217984917500889.

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Abstract:
In ultrathin films, the energy competition between the perpendicular magnetic anisotropy and the in-plane magnetostatic coupling can originate stripe domains. In such systems, the perpendicular magnetization component has a periodic modulation, pointing alternately upwards and downwards as the stripes are crossed. A measurement technique that is widely used to study these kind of domains is the magnetic force microscopy (MFM). As known, the MFM signal cannot be related immediately to the sample magnetization and the interpretation of the results is not always straightforward. Therefore, the ac
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