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Journal articles on the topic 'Stripe domains'

Author: Grafiati

Published: 23 September 2022

Last updated: 28 September 2022

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1

Kong, Xiangyang, Yongqiang Zhao, Jize Xue, Jonathan Cheung-Wai Chan, and Seong G. Kong. "Global and Local Tensor Sparse Approximation Models for Hyperspectral Image Destriping." Remote Sensing 12, no. 4 (February 20, 2020): 704. http://dx.doi.org/10.3390/rs12040704.

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This paper presents a global and local tensor sparse approximation (GLTSA) model for removing the stripes in hyperspectral images (HSIs). HSIs can easily be degraded by unwanted stripes. Two intrinsic characteristics of the stripes are (1) global sparse distribution and (2) local smoothness along the stripe direction. Stripe-free hyperspectral images are smooth in spatial domain, with strong spectral correlation. Existing destriping approaches often do not fully investigate such intrinsic characteristics of the stripes in spatial and spectral domains simultaneously. Those methods may generate new artifacts in extreme areas, causing spectral distortion. The proposed GLTSA model applies two ℓ 0 -norm regularizers to the stripe components and along-stripe gradient to improve the destriping performance. Two ℓ 1 -norm regularizers are applied to the gradients of clean image in spatial and spectral domains. The double non-convex functions in GLTSA are converted to single non-convex function by mathematical program with equilibrium constraints (MPEC). Experiment results demonstrate that GLTSA is effective and outperforms existing competitive matrix-based and tensor-based destriping methods in visual, as well as quantitative, evaluation measures.

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2

Wang, Min, Ting-Zhu Huang, Xi-Le Zhao, Liang-Jian Deng, and Gang Liu. "A Unidirectional Total Variation and Second-Order Total Variation Model for Destriping of Remote Sensing Images." Mathematical Problems in Engineering 2017 (2017): 1–10. http://dx.doi.org/10.1155/2017/4397189.

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Remote sensing images often suffer from stripe noise, which greatly degrades the image quality. Destriping of remote sensing images is to recover a good image from the image containing stripe noise. Since the stripes in remote sensing images have a directional characteristic (horizontal or vertical), the unidirectional total variation has been used to consider the directional information and preserve the edges. The remote sensing image contaminated by heavy stripe noise always has large width stripes and the pixels in the stripes have low correlations with the true pixels. On this occasion, the destriping process can be viewed as inpainting the wide stripe domains. In many works, high-order total variation has been proved to be a powerful tool to inpainting wide domains. Therefore, in this paper, we propose a variational destriping model that combines unidirectional total variation and second-order total variation regularization to employ the directional information and handle the wide stripes. In particular, the split Bregman iteration method is employed to solve the proposed model. Experimental results demonstrate the effectiveness of the proposed method.

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3

Tranquada, J. M. "The stripe-liquid phase in cuprates and nickelates." Journal de Physique IV 12, no. 9 (November 2002): 239–44. http://dx.doi.org/10.1051/jp4:20020404.

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It is well established that doped 2D antiferromagnets such as layered nickelates and certain cuprates can exhibit an ordered phase in which charge carriers are segregated to periodically-spaced domain walls separating antiferromagnetic domains. An open question concerns the nature of the state that is achieved when a stripe solid melts. Recent neutron scattering experiments on nickelates and cuprates indicate that melting leads to a stripe-liquid state; these results will be presented and discussed. The existence of the stripe-liquid phase in nickelates makes it plausible to interpret the mid-infrared absorption in terms of transitions from valence to mid-gap states associated with the stripes.

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4

Ramesh, M., and P. E. Wigen. "Ferromagnetodynamics of parallel stripe domains - domain walls system." Journal of Magnetism and Magnetic Materials 74, no. 2 (September 1988): 123–33. http://dx.doi.org/10.1016/0304-8853(88)90058-3.

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5

McCord, Jeffrey, Burak Erkartal, Thomas von Hofe, Lorenz Kienle, Eckhard Quandt, Olga Roshchupkina, and Jörg Grenzer. "Revisiting magnetic stripe domains — anisotropy gradient and stripe asymmetry." Journal of Applied Physics 113, no. 7 (February 21, 2013): 073903. http://dx.doi.org/10.1063/1.4792517.

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6

Onojima, Norio, Ayato Nakamura, Hiroki Saito, and Norihiro Daicho. "Angle-Dependent Polarized Raman Spectroscopy of TIPS Pentacene Single-Crystalline Domains Deposited on Au-Striped Substrates." MRS Proceedings 1799 (2015): 1–6. http://dx.doi.org/10.1557/opl.2015.484.

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ABSTRACT6,13-bis(triisopropylsilylethynyl) pentacene (TIPS pentacene) was deposited on SiO2/Si substrates with Au stripes using electrostatic spray deposition (ESD). We observed that crystalline domains on the substrates were preferentially oriented. To elucidate this phenomenon, the correlation between the orientation direction and stripe direction was investigated by angle-dependent polarized Raman spectroscopy. Since the acene planes in TIPS pentacene take an edge-on orientation on the substrates, C-C ring stretch modes can be used to probe the in-plane orientation. We found that the long molecular axis of acene planes is inclined at about 50° or 110° from the stripe direction. This result suggests that the molecular orientation of the crystalline domains can be controlled by the stripes.

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7

Kiselev, N. S., I. E. Dragunov, U. K. Rößler, and A. N. Bogdanov. "Stripe domains in nanomagnetic superlattices." Technical Physics Letters 33, no. 12 (December 2007): 1028–31. http://dx.doi.org/10.1134/s1063785007120139.

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8

Schafer, R., N. Mattern, and G. Herzer. "Stripe domains on amorphous ribbons." IEEE Transactions on Magnetics 32, no. 5 (1996): 4809–11. http://dx.doi.org/10.1109/20.539159.

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9

WRÓBEL, PIOTR, and ROBERT EDER. "STRIPE STABILITY IN DOPED ANTIFERROMAGNETS." International Journal of Modern Physics B 14, no. 29n31 (December 20, 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 antiferromagnetic background, hole pairs (which correspond to spin bipolarons) homogeneously distributed in the antiferromagnetic background, hole pairs which form the stripe structure in the perfect antiferromagnetic background, and eventually holes in stripes which separate antiferromagnetic domains with alternating direction of the staggered magnetization. Spin polarons are constructed by means of some computer algebra. It turns out that lowest eigenenergy has a state that represents a single hole polaron at the anti-phase domain wall (ADW). On the other hand, the stripe phase is exposed to keen competition from holes binding in the antiferromagnetic background and the energy margin by which stripes win is small.

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10

Lardelli, M., and D. Ish-Horowicz. "Drosophila hairy pair-rule gene regulates embryonic patterning outside its apparent stripe domains." Development 118, no. 1 (May 1, 1993): 255–66. http://dx.doi.org/10.1242/dev.118.1.255.

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The hairy (h) segmentation gene of Drosophila regulates segmental patterning of the early embryo, and is expressed in a set of anteroposterior stripes during the blastoderm stage. We have used a set of h gene deletions to study the h promoter and the developmental requirements for individual h stripes. The results confirm upstream regulation of h striping but indicate that expression in the anterodorsal head domain depends on sequences downstream of the two transcription initiation sites. Surprisingly, the two anterior-most h domains appear to be dispensable for head development and embryonic viability. One partial promoter deletion expresses ectopic h, leading to misexpression of other segmentation genes and embryonic pattern defects. We demonstrate that h affects patterning outside its apparent stripe domains, supporting a model in which primary pair-rule genes act as concentration-dependent transcriptional regulators, i.e. as local morphogens.

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11

Zhang, J. P., Y. X. Guo, and J. S. Speck. "Magnetic Domains and Domain Wall Pinning in Nanocrystalline Ni-P." Microscopy and Microanalysis 7, S2 (August 2001): 1242–43. http://dx.doi.org/10.1017/s1431927600032281.

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Magnetic domain structures in a Ni-5at%P alloy have been examined using Lorentz microscopy in Fresnel mode in a JEOL 2010TEM. with electron diffraction and high resolution electron imaging, the Ni-P alloy material is seen to be of FCC structure and composed of nanometer-sized grains (< 4nm in diameter), which is about 2 orders less in size than that of a single magnetic domain.The TEM specimen was prepared using jet polishing method. Before introducing the specimen into the microscope, the objective lens was turned off in a free lens control mode to ensure that the domain structures in the specimen remain unaffected. The objective mini-lens was used to perform Lorentz imaging with out-focus method.Stripe domains were observed. The width of these stripes is about 0.2 micron. But the length of these domains varies, sometime up to several microns. The stripe domains are grouped, which are near parallel one to the other.

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12

Kaplan, B. "Ferromagnetic stripe domains in ultrathin films." Journal of Magnetism and Magnetic Materials 288 (March 2005): 178–82. http://dx.doi.org/10.1016/j.jmmm.2004.08.034.

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13

Labrune, M., and L. Belliard. "Stripe Domains in Multilayers: Micromagnetic Simulations." physica status solidi (a) 174, no. 2 (August 1999): 483–97. http://dx.doi.org/10.1002/(sici)1521-396x(199908)174:2<483::aid-pssa483>3.0.co;2-7.

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14

Labrune, M., and J. Miltat. "Numerical simulation of weak stripe domains." Journal of Magnetism and Magnetic Materials 104-107 (February 1992): 241–42. http://dx.doi.org/10.1016/0304-8853(92)90781-i.

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15

Denneulin, T., and A. S. Everhardt. "A transmission electron microscopy study of low-strain epitaxial BaTiO₃ grown onto NdScO₃." Journal of Physics: Condensed Matter 34, no. 23 (April 5, 2022): 235701. http://dx.doi.org/10.1088/1361-648x/ac5db3.

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Abstract Ferroelectric materials exhibit a strong coupling between strain and electrical polarization. In epitaxial thin films, the strain induced by the substrate can be used to tune the domain structure. Substrates of rare-earth scandates are sometimes selected for the growth of ferroelectric oxides because of their close lattice match, which allows the growth of low-strain dislocation-free layers. Transmission electron microscopy (TEM) is a frequently used technique for investigating ferroelectric domains at the nanometer-scale. However, it requires to thin the specimen down to electron transparency, which can modify the strain and the electrostatic boundary conditions. Here, we have investigated a 320 nm thick epitaxial layer of BaTiO3 grown onto an orthorhombic substrate of NdScO3 with interfacial lattice strains of −0.45% and −0.05% along the two in-plane directions. We show that the domain structure of the layer can be significantly altered by TEM sample preparation depending on the orientation and the geometry of the lamella. In the as-grown state, the sample shows an anisotropic a/c ferroelastic domain pattern in the direction of largest strain. If a TEM lamella is cut perpendicular to this direction so that strain is released, a new domain pattern is obtained, which consists of bundles of thin horizontal stripes parallel to the interfaces. These stripe domains correspond to a sheared crystalline structure (orthorhombic or monoclinic) with inclined polarization vectors and with at least four variants of polarization. The stripe domains are distributed in triangular-shaped 180° domains where the average polarization is parallel to the growth direction. The influence of external electric fields on this domain structure was investigated using in situ biasing and dark-field imaging in TEM.

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16

Kosman, D., and S. Small. "Concentration-dependent patterning by an ectopic expression domain of the Drosophila gap gene knirps." Development 124, no. 7 (April 1, 1997): 1343–54. http://dx.doi.org/10.1242/dev.124.7.1343.

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The asymmetric distribution of the gap gene knirps (kni) in discrete expression domains is critical for striped patterns of pair-rule gene expression in the Drosophila embryo. To test whether these domains function as sources of morphogenetic activity, the stripe 2 enhancer of the pair-rule gene even-skipped (eve) was used to express kni in an ectopic position. Manipulating the stripe 2-kni expression constructs and examining transgenic lines with different insertion sites led to the establishment of a series of independent lines that displayed consistently different levels and developmental profiles of expression. Individual lines showed specific disruptions in pair-rule patterning that were correlated with the level and timing of ectopic expression. These results suggest that the ectopic domain acts as a source for morphogenetic activity that specifies regions in the embryo where pair-rule genes can be activated or repressed. Evidence is presented that the level and timing of expression, as well as protein diffusion, are important for determining the specific responses of target genes.

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17

Vukadinovic, N., A. Serraj, H. Le Gall, and J. Ben Youssef. "Dynamic susceptibility of parallel stripe domains with flexing domain walls." Physical Review B 58, no. 1 (July 1, 1998): 385–93. http://dx.doi.org/10.1103/physrevb.58.385.

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18

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 (April 15, 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 magnetic layer structure as a function of depth. Additional sensitivity to magnetic features is obtained through a neutron wave field resonance, which is fully accounted for in the presented analysis. The scattering reveals a domain width imbalance of 5.3 to 3.7 μm of virgin and bombarded stripes, respectively. Further, we report that the magnetization in the bombarded stripe significantly deviates from the head-to-head arrangement. A domain wall of 0.6 μm with homogeneous magnetization direction is found to separate the two neighboring domains. The results contain detailed information on length scales and magnetization vectors provided by PNR and OSS in absolute units. We illustrate the complementarity of the technique to microscopy techniques for obtaining a quantitative description of imprinted magnetic domain patterns and illustrate its applicability to different sample systems.

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19

Li, Xiaolei, Hongkang Xie, Yurui Wei, Hongmei Feng, Yueyue Liu, Runliang Gao, Qingfang Liu, and Jianbo Wang. "Effect of stripe domains on magnetization reversal and domain wall motion-like boundary expansion of the stripe domain region." Journal of Physics D: Applied Physics 53, no. 28 (May 18, 2020): 285001. http://dx.doi.org/10.1088/1361-6463/ab82db.

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20

Ausanio, G., V. Iannotti, L. Lanotte, M. Carbucicchio, and M. Rateo. "Weak stripe domains in Co/Fe multilayers." Journal of Magnetism and Magnetic Materials 226-230 (May 2001): 1740–42. http://dx.doi.org/10.1016/s0304-8853(00)00878-7.

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21

Simsova, J., R. Gemperle, J. Kaczer, and J. C. Lodder. "Stripe and bubble domains in CoCr films." IEEE Transactions on Magnetics 26, no. 1 (1990): 30–32. http://dx.doi.org/10.1109/20.50480.

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22

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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23

Suzuki, T., K. Matsuyama, H. Asada, and S. Konishi. "Initiating stripe domains in Bloch line memory." IEEE Transactions on Magnetics 23, no. 5 (September 1987): 3393–95. http://dx.doi.org/10.1109/tmag.1987.1065554.

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24

Arnaud, L., and F. Boileau. "STRIPE DOMAINS STABILIZATION FOR BLOCH LINE MEMORY." Le Journal de Physique Colloques 46, no. C6 (September 1985): C6–137—C6–140. http://dx.doi.org/10.1051/jphyscol:1985624.

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25

Álvarez-Prado, Luis M. "Control of Dynamics in Weak PMA Magnets." Magnetochemistry 7, no. 3 (March 17, 2021): 43. http://dx.doi.org/10.3390/magnetochemistry7030043.

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We have recently shown that a hybrid magnetic thin film with orthogonal anisotropies presenting weak stripe domains can achieve a high degree of controllability of its ferromagnetic resonance. This work explores the origin of the reconfigurability through micromagnetic simulations. The static domain structures which control the thin film resonance can be found under a deterministic applied field protocol. In contrast to similar systems reported, our effect can be obtained under low magnetic fields. We have also found through simulations that the spin wave propagation in the hybrid is nonreciprocal: two adjacent regions emit antiparallel spin waves along the stripe domains. Both properties convert the hybrid in a candidate for future magnonic devices at the nanoscale.

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26

Takahashi, R., Ø. Dahl, E. Eberg, J. K. Grepstad, and T. Tybell. "Ferroelectric stripe domains in PbTiO3 thin films: Depolarization field and domain randomness." Journal of Applied Physics 104, no. 6 (September 15, 2008): 064109. http://dx.doi.org/10.1063/1.2978225.

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27

Fujioka, M., Y. Emi-Sarker, G. L. Yusibova, T. Goto, and J. B. Jaynes. "Analysis of an even-skipped rescue transgene reveals both composite and discrete neuronal and early blastoderm enhancers, and multi-stripe positioning by gap gene repressor gradients." Development 126, no. 11 (June 1, 1999): 2527–38. http://dx.doi.org/10.1242/dev.126.11.2527.

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The entire functional even-skipped locus of Drosophila melanogaster is contained within a 16 kilobase region. As a transgene, this region is capable of rescuing even-skipped mutant flies to fertile adulthood. Detailed analysis of the 7.7 kb of regulatory DNA 3′ of the transcription unit revealed ten novel, independently regulated patterns. Most of these patterns are driven by non-overlapping regulatory elements, including ones for syncytial blastoderm stage stripes 1 and 5, while a single element specifies both stripes 4 and 6. Expression analysis in gap gene mutants showed that stripe 5 is restricted anteriorly by Kruppel and posteriorly by giant, the same repressors that regulate stripe 2. Consistent with the coregulation of stripes 4 and 6 by a single cis-element, both the anterior border of stripe 4 and the posterior border of stripe 6 are set by zygotic hunchback, and the region between the two stripes is ‘carved out’ by knirps. Thus the boundaries of stripes 4 and 6 are set through negative regulation by the same gap gene domains that regulate stripes 3 and 7 (Small, S., Blair, A. and Levine, M. (1996) Dev. Biol. 175, 314–24), but at different concentrations. The 3′ region also contains a single element for neurogenic expression in ganglion mother cells 4–2a and 1–1a, and neurons derived from them (RP2, a/pCC), suggesting common regulators in these lineages. In contrast, separable elements were found for expression in EL neurons, U/CQ neurons and the mesoderm. The even-skipped 3′ untranslated region is required to maintain late stage protein expression in RP2 and a/pCC neurons, and appears to affect protein levels rather than mRNA levels. Additionally, a strong pairing-sensitive repression element was localized to the 3′ end of the locus, but was not found to contribute to efficient functional rescue.

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28

Talbi, Y., Y. Roussigné, P. Djemia, and M. Labrune. "Weak stripe domains vibrations description using Thiele equation." Journal of Physics: Conference Series 200, no. 4 (January 1, 2010): 042027. http://dx.doi.org/10.1088/1742-6596/200/4/042027.

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29

Tee Soh, Wee, Nguyen N. Phuoc, C. Y. Tan, and C. K. Ong. "Magnetization dynamics in permalloy films with stripe domains." Journal of Applied Physics 114, no. 5 (August 7, 2013): 053908. http://dx.doi.org/10.1063/1.4817767.

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30

Yan, M., G. Leaf, H. Kaper, V. Novosad, P. Vavassori, R. E. Camley, and M. Grimsditch. "Dynamic origin of stripe domains in cobalt bars." Journal of Magnetism and Magnetic Materials 310, no. 2 (March 2007): 1596–98. http://dx.doi.org/10.1016/j.jmmm.2006.10.1127.

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31

Donzelli, O., M. Bassani, F. Spizzo, and D. Palmeri. "Reorientational transition and stripe domains in Co films." Journal of Magnetism and Magnetic Materials 320, no. 14 (July 2008): e261-e263. http://dx.doi.org/10.1016/j.jmmm.2008.02.147.

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32

Craus, C. B., A. R. Chezan, M. H. Siekman, J. C. Lodder, D. O. Boerma, and L. Niesen. "Stripe domains in Fe–Zr–N nanocrystalline films." Journal of Magnetism and Magnetic Materials 240, no. 1-3 (February 2002): 423–26. http://dx.doi.org/10.1016/s0304-8853(01)00882-4.

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33

Ghising, Pramod, Z. Hossain, and R. C. Budhani. "Stripe magnetic domains in CeY2Fe5O12 (Ce:YIG) epitaxial films." Applied Physics Letters 110, no. 1 (January 2, 2017): 012406. http://dx.doi.org/10.1063/1.4973481.

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34

Álvarez, N. R., J. E. Gómez, M. Vásquez Mansilla, B. Pianciola, D. G. Actis, G. J. Gilardi, L. Leiva, J. Milano, and A. Butera. "Magnetic coupling of stripe domains in FePt/Ni80Fe20bilayers." Journal of Physics D: Applied Physics 50, no. 11 (February 13, 2017): 115001. http://dx.doi.org/10.1088/1361-6463/aa5bce.

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35

Theis-Bröhl, K., A. Westphalen, H. Zabel, U. Rücker, J. McCord, V. Höink, J. Schmalhorst, et al. "Hyper-domains in exchange bias micro-stripe pattern." New Journal of Physics 10, no. 9 (September 18, 2008): 093021. http://dx.doi.org/10.1088/1367-2630/10/9/093021.

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36

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 (October 2006): 172–75. http://dx.doi.org/10.1016/j.jallcom.2006.01.091.

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37

Ovadia, A., I. B. Puchalska, and J. P. Jakubovics. "Stripe domains in obliquely deposited Co-Au films." Journal of Magnetism and Magnetic Materials 54-57 (February 1986): 851–52. http://dx.doi.org/10.1016/0304-8853(86)90282-9.

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38

Dhiman, A. K., R. Gieniusz, P. Gruszecki, J. Kisielewski, M. Matczak, Z. Kurant, I. Sveklo, et al. "Magnetization statics and dynamics in (Ir/Co/Pt)₆ multilayers with Dzyaloshinskii–Moriya interaction." AIP Advances 12, no. 4 (April 1, 2022): 045007. http://dx.doi.org/10.1063/9.0000339.

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Magnetic multilayers of (Ir/Co/Pt)6 with interfacial Dzyaloshinskii-Moriya interaction (IDMI) were deposited by magnetron sputtering with Co thickness d=1.8 nm. Exploiting magneto-optical Kerr effect in longitudinal mode microscopy, magnetic force microscopy, and vibrating sample magnetometry, the magnetic field-driven evolution of domain structures and magnetization hysteresis loops have been studied. The existence of weak stripe domains structure was deduced – tens micrometers size domains with in-plane “core” magnetization modulated by hundred of nanometers domains with out-of-plane magnetization. Micromagnetic simulations interpreted such magnetization distribution. Quantitative evaluation of IDMI was carried out using Brillouin light scattering (BLS) spectroscopy as the difference between Stokes and anti-Stokes peak frequencies Δ f. Due to the additive nature of IDMI, the asymmetric combination of Ir and Pt covers led to large values of effective IDMI energy density Deff. It was found that Stokes and anti-Stokes frequencies as well as Δ f, measured as a function of in-plane applied magnetic field, show hysteresis. These results are explained under the consideration of the influence of IDMI on the dynamics of the in-plane magnetized “core” with weak stripe domains.

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39

Ebels, U., P. E. Wigen, and K. Ounadjela. "Domain FMR in epitaxial Co(0 0 0 1) films with stripe domains." Journal of Magnetism and Magnetic Materials 177-181 (January 1998): 1239–40. http://dx.doi.org/10.1016/s0304-8853(97)00309-0.

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40

Kent, A. D., U. Ruediger, J. Yu, S. Zhang, P. M. Levy, Y. Zhong, and S. S. P. Parkin. "Magnetoresistance due to domain walls in micron scale Fe wires with stripe domains." IEEE Transactions on Magnetics 34, no. 4 (July 1998): 900–902. http://dx.doi.org/10.1109/20.706305.

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41

Zhang, Haoran, Yanhui Zhang, Bin Wang, Zhiying Chen, Yaqian Zhang, Yanping Sui, Guanghui Yu, Zhi Jin, and Xinyu Liu. "Stripe distributions of graphene-coated Cu foils and their effects on the reduction of graphene wrinkles." RSC Advances 5, no. 117 (2015): 96587–92. http://dx.doi.org/10.1039/c5ra17581j.

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The wrinkle distribution of graphene domain was obtained as trenches after hydrogen etching. Parallel stripes on graphene domains are always perpendicular to these trenches, suggesting the suppressed wrinkle formation along the stripes' direction.

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42

Zheng, Luping, Jie He, Zuomei Ding, Chenlong Zhang, and Ruoxue Meng. "Identification of Functional Domain(s) of Fibrillarin Interacted with p2 of Rice stripe virus." Canadian Journal of Infectious Diseases and Medical Microbiology 2018 (2018): 1–6. http://dx.doi.org/10.1155/2018/8402839.

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p2 of Rice stripe virus may promote virus systemic infection by interacting with the full length of fibrillarin from Nicotiana benthamiana (NbFib2) in the nucleolus and cajal body (CB). NbFib2 contains three functional domains. We used yeast two-hybrid, colocalization, and bimolecular fluorescence complementation (BiFC) assays to study the interactions between p2 and the three domains of NbFib2, namely, the N-terminal fragment containing a glycine and arginine-rich (GAR) domain, the central RNA-binding domain, and the C-terminal fragment containing an α-helical domain. The results show that the N-terminal domain is indispensable for NbFib2 to localize in the nucleolus and cajal body. p2 binds all three regions of NbFib2, and they target to the nucleus but fail to the nucleolus and cajal bodies (CBs).

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43

Martin, Wayne. "Fast equi-partitioning of rectangular domains using stripe decomposition." Discrete Applied Mathematics 82, no. 1-3 (March 1998): 193–207. http://dx.doi.org/10.1016/s0166-218x(97)00122-4.

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Sparks, P. D., N. P. Stern, D. S. Snowden, B. A. Kappus, J. G. Checkelsky, S. S. Harberger, A. M. Fusello, and J. C. Eckert. "Stripe domains and magnetoresistance in thermally deposited nickel films." Journal of Magnetism and Magnetic Materials 272-276 (May 2004): E1339—E1340. http://dx.doi.org/10.1016/j.jmmm.2003.12.586.

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Wu, Dongping, Tianli Jin, Yuanfu Lou, and Fulin Wei. "Understanding the dense stripe domains in soft magnetic film." Applied Surface Science 346 (August 2015): 567–73. http://dx.doi.org/10.1016/j.apsusc.2015.04.010.

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Coïsson, Marco, Franco Vinai, Paola Tiberto, and Federica Celegato. "Magnetic properties of FeSiB thin films displaying stripe domains." Journal of Magnetism and Magnetic Materials 321, no. 7 (April 2009): 806–9. http://dx.doi.org/10.1016/j.jmmm.2008.11.072.

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Niedoba, H., and M. Labrune. "Magnetic bubbles and stripe domains in nanostructured FePd elements." Journal of Magnetism and Magnetic Materials 321, no. 14 (July 2009): 2178–86. http://dx.doi.org/10.1016/j.jmmm.2009.01.007.

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Ha, Seung-Seok, Jungbum Yoon, Sukmock Lee, Chun-Yeol You, Myung-Hwa Jung, and Young Keun Kim. "Spin wave quantization in continuous film with stripe domains." Journal of Applied Physics 105, no. 7 (April 2009): 07D544. http://dx.doi.org/10.1063/1.3072757.

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Kiselev, N. S., I. E. Dragunov, U. K. Rößler, and A. N. Bogdanov. "Exchange shift of stripe domains in antiferromagnetically coupled multilayers." Applied Physics Letters 91, no. 13 (September 24, 2007): 132507. http://dx.doi.org/10.1063/1.2793626.

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Kiselev, N. S., I. E. Dragunov, A. T. Onisan, U. K. Rößler, and A. N. Bogdanov. "Theory of stripe domains in magnetic shape memory alloys." European Physical Journal Special Topics 158, no. 1 (May 2008): 119–24. http://dx.doi.org/10.1140/epjst/e2008-00663-5.

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