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1

Ayala Rodríguez, Maribel. "La función del nombre y sus cambios en la conformación de la identidad del héroe en «Espejo de príncipes y caballeros» de Diego Ortúñez de Calahorra." Tirant: Butlletí informatiu i bibliogràfic de literatura de cavalleries, no. 23 (December 13, 2020): 151. http://dx.doi.org/10.7203/tirant.23.19116.

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En diversas obras literarias el nombre de los personajes es un repositorio de elementos importantes para el desarrollode la trama. En los libros de caballerías, además, el cambio de nombre es un recurso que destaca por su utilidad paramarcar distintas etapas o aventuras en el desarrollo de los héroes. El Espejo de príncipes y caballeros de Diego Ortúñez de Calahorra (1555) es una excepción, pues su protagonista, el Cavallero del Febo, cambia de nombre una sola vez. No obstante, en esta historia tienen lugar conflictos que en otras obras son desencadenados típicamente por los cambios de nombre. Por ello, este artículo busca exponer los rasgos particulares del nombre del Cavallero del Feboy cómo éstos se relacionan con su identidad y le permiten prescindir del cambio de nombre sin afectar el desarrollodel libro de caballerías.
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2

Ayala Rodríguez, Maribel. "La función del nombre y sus cambios en la conformación de la identidad del héroe en «Espejo de príncipes y caballeros» de Diego Ortúñez de Calahorra." Tirant: Butlletí informatiu i bibliogràfic de literatura de cavalleries, no. 23 (December 13, 2020): 151. http://dx.doi.org/10.7203/titant.23.19116.

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En diversas obras literarias el nombre de los personajes es un repositorio de elementos importantes para el desarrollode la trama. En los libros de caballerías, además, el cambio de nombre es un recurso que destaca por su utilidad paramarcar distintas etapas o aventuras en el desarrollo de los héroes. El Espejo de príncipes y caballeros de Diego Ortúñez de Calahorra (1555) es una excepción, pues su protagonista, el Cavallero del Febo, cambia de nombre una sola vez. No obstante, en esta historia tienen lugar conflictos que en otras obras son desencadenados típicamente por los cambios de nombre. Por ello, este artículo busca exponer los rasgos particulares del nombre del Cavallero del Feboy cómo éstos se relacionan con su identidad y le permiten prescindir del cambio de nombre sin afectar el desarrollodel libro de caballerías.
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3

Neumair, Stephanie C., Robert Glaum, and Hubert Huppertz. "Synthesis and Crystal Structure of the High-pressure Iron Borate β-FeB2O4." Zeitschrift für Naturforschung B 64, no. 8 (August 1, 2009): 883–90. http://dx.doi.org/10.1515/znb-2009-0802.

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The iron borate β -FeB2O4 was synthesized under high-pressure / high-temperature conditions of 8 GPa and 1030 ◦C. The structure of β -FeB2O4 is isotypic to HP-NiB2O4, representing the second example of a borate in which every BO4 tetrahedron shares a common edge with a second one. β - FeB2O4 crystallizes in the space group C2/c (Z = 4) with the parameters a = 950.0(2), b = 562.9(2), c = 443.7(1) pm, β = 108.50(3)◦, V = 0.22495(8) nm3, R1 = 0.0293, and wR2 = 0.0647 (all data). The structure consists of layers of BO4 tetrahedra, connected via strings of edge-sharing FeO6 octahedra. A ligand field splitting of Δo ≈8860 cm−1 is estimated from polarized single-crystal electronic absorption spectra of β -FeB2O4. The tetragonal distortion of the ligand field in the [FeIIO6] chromophore amounts to −(8/3)dσ ≈2900 cm−1. In the range of 16000 cm−1 ≤ṽ ≤24000 cm−1, rather strong spin-forbidden transitions within the [FeIIO6] chromophore are observed
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4

Yu, Peng, Lin Zhang, and Linxiu Du. "Atomic Simulations for Packing Changes of Nano-Sized Cu Clusters Embedded in the Febulk on Heating." Metals 11, no. 6 (June 8, 2021): 934. http://dx.doi.org/10.3390/met11060934.

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Understanding of the defect evolution mechanism under irradiation is very important for the research of pressure vessel steel embrittlement. In this paper, the embedded atom method (EAM) based canonical ensemble molecular dynamics (MD) method was used to study the evolution of the stacking structure of different nano-sized Cun (n = 13, 43 and 87) clusters in an Febulk embedded with BCC lattice structure during continuous heating. The mean square displacement, pair distribution functions and atomic structures of Cu atom clusters at the nanometer scale were calculated at different temperatures. The structural changes present apparent differences, for the Febulks contain nano-sized Cu clusters with different atom numbers during heating. For the Febulk–Cu13 system, since the ability to accommodate the atomic Cu in the Fe substrate is lesser, a small number of Cu atoms in BCC lattice positions cannot influence the whole structure of the Fe-Cu system. For the Febulk–Cu43 system, with an increase in temperature, a Cu atomic pile structural change happened, and the strain areas decreased significantly in the Febulk, but a single strain area grew large. For the Febulk–Cu87 system, when the Cu atoms are constrained by the Fe atoms in bulk, only a few of the Cu atoms adjust their positions. With the increase in temperature, strain in the Fe eased.
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5

Abrori, Syauqi Abdurrahman, Ni Luh Wulan Septiani, Nugraha, Isa Anshori, Suyatman, Veinardi Suendo, and Brian Yuliarto. "Metal-Organic-Framework FeBDC-Derived Fe3O4 for Non-Enzymatic Electrochemical Detection of Glucose." Sensors 20, no. 17 (August 29, 2020): 4891. http://dx.doi.org/10.3390/s20174891.

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Present-day science indicates that developing sensors with excellent sensitivity and selectivity for detecting early signs of diseases is highly desirable. Electrochemical sensors offer a method for detecting diseases that are simpler, faster, and more accurate than conventional laboratory analysis methods. Primarily, exploiting non-noble-metal nanomaterials with excellent conductivity and large surface area is still an area of active research due to its highly sensitive and selective catalysts for electrochemical detection in enzyme-free sensors. In this research, we successfully fabricate Metal-Organic Framework (MOF) FeBDC-derived Fe3O4 for non-enzymatic electrochemical detection of glucose. FeBDC synthesis was carried out using the solvothermal method. FeCl2.4H2O and Benzene-1,4-dicarboxylic acid (H2BDC) are used as precursors to form FeBDC. The materials were further characterized utilizing X-ray Powder Diffraction (XRD), Scanning Electron Microscopy (SEM), and Fourier-Transform Infrared Spectroscopy (FTIR). The resulting MOF yields good crystallinity and micro-rod like morphology. Electrochemical properties were tested using Cyclic Voltammetry (CV) and Differential Pulse Voltammetry (DPV) with a 0.1 M of Phosphate Buffer Saline (PBS pH 7.4) solution as the supporting electrolyte. The measurement results show the reduction and oxidation peaks in the CV curve of FeBDC, as well as Fe3O4. Pyrolysis of FeBDC to Fe3O4 increases the peak of oxidation and reduction currents. The Fe3O4 sample obtained has a sensitivity of 4.67 µA mM−1.cm−2, a linear range between 0.0 to 9.0 mM, and a glucose detection limit of 15.70 µM.
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6

Herrmann, Hartmut, and Ralf Wolke. "Introduction to FEBUKO and MODMEP." Atmospheric Environment 39, no. 23-24 (July 2005): 4167. http://dx.doi.org/10.1016/j.atmosenv.2005.02.005.

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7

Maas, Steve A., Gerard A. Ateshian, and Jeffrey A. Weiss. "FEBio: History and Advances." Annual Review of Biomedical Engineering 19, no. 1 (June 21, 2017): 279–99. http://dx.doi.org/10.1146/annurev-bioeng-071516-044738.

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8

Aslam, M., M. Tahir Soomro, Iqbal M. I. Ismail, Huda A. Qari, M. A. Gondal, and A. Hameed. "The facile synthesis, characterization and evaluation of photocatalytic activity of bimetallic FeBiO3 in natural sunlight exposure." RSC Advances 5, no. 124 (2015): 102663–73. http://dx.doi.org/10.1039/c5ra18808c.

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9

Calendron, Anne-Laure, Emma Kueny, Liwei Song, Giovanni Cirmi, Lars Bocklage, Franz X. Kärtner, and Ralf Röhlsberger. "Excitation and control of spin waves in FeBO3 by a strong-field THz pulse." EPJ Web of Conferences 205 (2019): 07008. http://dx.doi.org/10.1051/epjconf/201920507008.

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The dynamically resolved response of the canted-antiferromagnet FeBO3 excited near a magnon resonance shows fast oscillations after THz-excitation’ followed by the magnons’ intrinsic relaxation’ enabling to probe transient magnetic relaxation dynamics over large frequency range.
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10

Strugatsky, M. B., and K. M. Skibinsky. "Acoustic resonances in antiferromagnet FeBO3." Journal of Magnetism and Magnetic Materials 309, no. 1 (February 2007): 64–70. http://dx.doi.org/10.1016/j.jmmm.2006.06.028.

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11

Chzhan, A. V., G. S. Patrin, and I. N. Isaeva. "Photo-Induced Relaxation Self-Oscillations of Stripe Structures in FeBO3." Defect and Diffusion Forum 293 (August 2009): 113–17. http://dx.doi.org/10.4028/www.scientific.net/ddf.293.113.

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Photo-induced self-oscillations of stripe structures are studied in FeBO3 crystals at low temperatures. Experimental data show that the observed oscillations have a relaxational character. On the basis of the research carried out, a model for such oscillations is presented.
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12

Svistov, L. E., and H. Benner. "Magnetization of FeBO3 by microwave pumping." Journal of Experimental and Theoretical Physics 88, no. 3 (March 1999): 610–14. http://dx.doi.org/10.1134/1.558836.

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13

Mitsai, Yu N., K. M. Skibinskii, M. B. Strugatskii, and V. V. Tarakanov. "Linear magnetoacoustic birefringence effects in FeBO3." Physics of the Solid State 39, no. 5 (May 1997): 803–6. http://dx.doi.org/10.1134/1.1129973.

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14

Fedorov, Yu M., A. A. Leksikov, and O. V. Vorotynova. "Photoinduced magnetic superstructure in FeBO3:Ni." Solid State Communications 55, no. 11 (September 1985): 987–89. http://dx.doi.org/10.1016/0038-1098(85)90572-1.

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15

Wang, Baoxiang, Xiaoli Tian, Xianfen Song, Lili Ma, Shoushan Yu, Chuncheng Hao, Kezheng Chen, and Qingquan Lei. "Smart electrorheological behavior of Cr-doped multiferroelectric FeBiO3 nanoparticles." Colloids and Surfaces A: Physicochemical and Engineering Aspects 461 (November 2014): 184–94. http://dx.doi.org/10.1016/j.colsurfa.2014.07.046.

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16

Wieprecht, W., K. Acker, S. Mertes, J. Collett, W. Jaeschke, E. Brüggemann, D. Möller, and H. Herrmann. "Cloud physics and cloud water sampler comparison during FEBUKO." Atmospheric Environment 39, no. 23-24 (July 2005): 4267–77. http://dx.doi.org/10.1016/j.atmosenv.2005.02.012.

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17

Klemm, Marco, Michael Kröger, Kati Görsch, Rüdiger Lange, Gerd Hilpmann, Farzad Lali, Stefan Haase, et al. "Experimental Evaluation of a New Approach for a Two-Stage Hydrothermal Biomass Liquefaction Process." Energies 13, no. 14 (July 17, 2020): 3692. http://dx.doi.org/10.3390/en13143692.

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A new approach for biomass liquefaction was developed and evaluated in a joint research project. Focus of the project, called FEBio@H2O, lies on a two-step hydrothermal conversion. Within step 1, the input biomass is converted employing a hydrothermal degradation without added catalyst or by homogeneous catalysis. Within step 2, the hydrogen accepting products of step 1, e.g., levulinic acid (LA) are upgraded by a heterogeneously catalyzed hydrogenation with hydrogen donor substances, e.g., formic acid (FA). As a result, components with an even lower oxygen content in comparison to step 1 products are formed; as an example, γ-valerolactone (GVL) can be named. Therefore, the products are more stable and contained less oxygen as requested for a possible application as liquid fuel. As a hydrothermal process, FEBio@H2O is especially suitable for highly water-containing feedstock. The evaluation involves hydrothermal conversion tests with model substances, degradation of real biomasses, transfer hydrogenation or hydrogenation with hydrogen donor of model substances and real products of step 1, catalyst selection and further development, investigation of the influence of reactor design, the experimental test of the whole process chain, and process assessment.
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18

Ягупов, С. В., Н. И. Снегирёв, К. А. Селезнева, Е. Т. Милюкова, Ю. А. Могиленец, Ю. В. Ермолаев, and М. Б. Стругацкий. "Структурные превращения в борате железа при высокотемпературном отжиге." Журнал технической физики 89, no. 8 (2019): 1229. http://dx.doi.org/10.21883/jtf.2019.08.47896.285-18.

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Surface morphology and crystal structure of iron borate, FeBO3, annealed at different temperatures, have been studied by scanning electron microscopy and X-ray diffraction analysis. The temperature range of structurally stability of iron borate has been determined. It has been established that in the range of temperatures 800–900°C recrystallization in the iron orthoborate Fe3BO6 phase, and more than 900°C − in α-Fe2O3 phase, occurs.
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19

Safonov, V. L., P. M. Loaiza, and L. E. Svistov. "Relaxation of magnetoelastic oscillations in antiferromagnetic FeBO3." Journal of Magnetism and Magnetic Materials 173, no. 1-2 (September 1997): 43–50. http://dx.doi.org/10.1016/s0304-8853(97)00165-0.

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20

Glazkov, V. P., V. V. Kvardakov, and V. A. Somenkov. "Pressure induced spin-reorientation transition in FeBO3." High Pressure Research 17, no. 3-6 (August 2000): 179–85. http://dx.doi.org/10.1080/08957950008245905.

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21

Snegirev, N. I., I. S. Lyubutin, S. V. Yagupov, M. A. Chuev, N. K. Chumakov, O. M. Zhigalina, D. N. Khmelenin, and M. B. Strugatsky. "Size Effects in Iron Borate FeBO3 Nanoparticles." Russian Journal of Inorganic Chemistry 66, no. 8 (August 2021): 1217–22. http://dx.doi.org/10.1134/s0036023621080283.

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22

Neumair, Stephanie C., Reinhard Kaindl, and Hubert Huppertz. "Synthesis and Crystal Structure of the High-pressure Cobalt Borate HP-CoB2O4." Zeitschrift für Naturforschung B 65, no. 11 (November 1, 2010): 1311–17. http://dx.doi.org/10.1515/znb-2010-1104.

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The cobalt borate HP-CoB2O4 was synthesized from Co3O4 and B2O3 under high-pressure / high-temperature conditions of 6.5 GPa and 950 °C. The structure of HP-CoB2O4 is isotypic to HPNiB2O4 and β -FeB2O4, representing the third example of a borate, in which every BO4 tetrahedron shares a common edge with a second one. HP-CoB2O4 crystallizes in the space group C2/c (Z = 4) with the parameters a = 934.6(2), b = 562.0(2), c = 443.3(1) pm, β = 108.2(1)°, V = 0.2212(1) nm3, R1 = 0.0218, and wR2 = 0.0410 (all data). The structure consists of layers of BO4 tetrahedra, that are interconnected via strings of edge-sharing FeO6 octahedra
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23

Özkendir, Osman Murat. "Influence of Neodymium Doping on the Crystal and Electronic Properties of FeBO3 Oxide Materials." Afyon Kocatepe University Journal of Sciences and Engineering 18, no. 1 (April 1, 2018): 62–66. http://dx.doi.org/10.5578/fmbd.66458.

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24

Glazkov, V. P., S. E. Kichanov, D. P. Kozlenko, B. N. Savenko, and V. A. Somenkov. "Pressure-induced changes in magnetic structure of FeBO3." Journal of Magnetism and Magnetic Materials 258-259 (March 2003): 543–44. http://dx.doi.org/10.1016/s0304-8853(02)01137-x.

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25

Tarakanov, Valery V., Valery I. Khizhnyi, Aleksey P. Korolyuk, and Mark B. Strugatsky. "Excitation of magnetic polaritons in plates of FeBO3." Physica B: Condensed Matter 284-288 (July 2000): 1452–53. http://dx.doi.org/10.1016/s0921-4526(99)02694-0.

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26

Troyan, I. A., A. G. Gavrilyuk, S. G. Ovchinnikov, I. S. Lyubutin, and N. V. Kazak. "Electron transport in FeBO3 ferroborate at ultrahigh pressures." JETP Letters 94, no. 10 (January 2012): 748–52. http://dx.doi.org/10.1134/s0021364011220115.

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27

Sadreev, A. F., and Yu M. Fedorov. "Photoinduced superstructure in easy plane magnet FeBO3:Ni." Physics Letters A 123, no. 3 (July 1987): 148–50. http://dx.doi.org/10.1016/0375-9601(87)90296-9.

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28

Rupp, R. A., B. Sugg, H. Nürge, M. Neumann, and W. Jantz. "Holographic Recording in the Photorefractive Weak Ferromagnet FeBO3." Journal of Optics 24, no. 3 (September 1995): 125–31. http://dx.doi.org/10.1007/bf03549766.

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29

Neumair, Stephanie C., Lukas Perfler, and Hubert Huppertz. "Synthesis and Characterization of the Manganese Borate α-MnB2O4." Zeitschrift für Naturforschung B 66, no. 9 (September 1, 2011): 882–88. http://dx.doi.org/10.1515/znb-2011-0903.

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The high-pressure manganese borate α-MnB2O4 was synthesized under high-pressure/hightemperature conditions of 6.5 GPa and 1100 ◦C in a modified Walker-type multianvil apparatus. The monoclinic compound is isotypic to α-FeB2O4, CaAl2O4-II, CaGa2O4, andβ -SrGa2O4 crystallizing with eight formula units in the space group P21/c (Z = 8) with the lattice parameters a = 712.1(2), b = 747.1(2), c = 878.8(2) pm, β = 94.1(1)◦, V = 0.466(1) nm3, R1 = 0.0326, and wR2 = 0.0652 (all data). The compound is built up from layers of “sechser” rings of corner-sharing BO4 tetrahedra that are interconnected to a three-dimensional network. The manganese ions are coordinated by seven oxygen atoms and situated in channels along the a axis.
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30

Knyazev, Yurii V., Natalia V. Kazak, Vyacheslav S. Zhandun, Juan Bartolomé, Ana Arauzo, Nadejda A. Belskaya, Oleg A. Bayukov, Leonard N. Bezmaternykh, and Sergey G. Ovchinnikov. "Electronic and magnetic states of Fe ions in Co2FeBO5." Dalton Transactions 50, no. 28 (2021): 9735–45. http://dx.doi.org/10.1039/d1dt00125f.

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31

Das, Swapan K., Mahasweta Nandi, Saurav Giri, and Asim Bhaumik. "A new mesoporous FeBO3 material having dominant surface magnetism." Microporous and Mesoporous Materials 117, no. 1-2 (January 2009): 362–67. http://dx.doi.org/10.1016/j.micromeso.2008.07.010.

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32

Kamzin, A. S., B. Stahl, E. Kankeleit, R. Gellert, M. Muller, and D. B. Vcherashnii. "Critical behavior of the surface of FeBO3 single crystals." Journal of Experimental and Theoretical Physics Letters 71, no. 10 (May 2000): 442–45. http://dx.doi.org/10.1134/1.568373.

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33

Strugatsky, M. B., K. M. Skibinsky, V. V. Tarakanov, and V. I. Khizhnyi. "Frequency dependence of sound amplitude in antiferromagnetic crystal FeBO3." Journal of Magnetism and Magnetic Materials 313, no. 1 (June 2007): 84–88. http://dx.doi.org/10.1016/j.jmmm.2006.12.007.

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34

Svistov, L. E., V. L. Safonov, and K. R. Khachevatskaya. "Spin-wave resonances in nonuniformly strained films of FeBO3." Journal of Experimental and Theoretical Physics 85, no. 2 (August 1997): 307–12. http://dx.doi.org/10.1134/1.558279.

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35

Pleshakov, Ivan V., and Vladimir V. Matveev. "Nuclear magnetic resonance investigation of photomagnetic phenomena in FeBO3." Journal of Physics: Condensed Matter 16, no. 10 (March 1, 2004): 1725–31. http://dx.doi.org/10.1088/0953-8984/16/10/005.

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36

Patrin, G. S., G. A. Petrakovskii, and V. V. Rudenko. "Photoinduced change of magnetic resonance in FeBO3 single crystals." Physica Status Solidi (a) 99, no. 2 (February 16, 1987): 619–23. http://dx.doi.org/10.1002/pssa.2210990233.

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37

Dyachenko, A. A., A. O. Shorikov, and V. I. Anisimov. "Phase transitions in FeBO3 under pressure: DFT + DMFT study." JETP Letters 106, no. 5 (September 2017): 317–23. http://dx.doi.org/10.1134/s0021364017170015.

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38

Finley, Sean M., Darrel S. Brodke, Nicholas T. Spina, Christine A. DeDen, and Benjamin J. Ellis. "FEBio finite element models of the human lumbar spine." Computer Methods in Biomechanics and Biomedical Engineering 21, no. 6 (April 26, 2018): 444–52. http://dx.doi.org/10.1080/10255842.2018.1478967.

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39

Karaev, A. A., B. Yu Sokolov, and Yu M. Fedorov. "Induced magnetic superstructure in the FeBO3: Mg weak ferromagnet." Physics of the Solid State 42, no. 11 (November 2000): 2097–102. http://dx.doi.org/10.1134/1.1324046.

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40

Ovchinnikov, S. G., V. V. Rudenko, and V. I. Tugarinov. "Weak ferromagnetism along the triad axis of FeBO3 crystals." Physics of the Solid State 58, no. 10 (October 2016): 1995–98. http://dx.doi.org/10.1134/s1063783416100279.

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41

Meng, Qingen, Zhongmin Jin, John Fisher, and Ruth Wilcox. "Comparison between FEBio and Abaqus for biphasic contact problems." Proceedings of the Institution of Mechanical Engineers, Part H: Journal of Engineering in Medicine 227, no. 9 (June 26, 2013): 1009–19. http://dx.doi.org/10.1177/0954411913483537.

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42

Herron, Michael R., Jeeone Park, Andrew T. Dailey, Douglas L. Brockmeyer, and Benjamin J. Ellis. "Febio finite element models of the human cervical spine." Journal of Biomechanics 113 (December 2020): 110077. http://dx.doi.org/10.1016/j.jbiomech.2020.110077.

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43

Fedorov, Yu M., A. A. Leksikov, and O. V. Vorotynova. "Temperature behaviour of photoinduced modulated state in FeBO3:Ni." Physics Letters A 123, no. 3 (July 1987): 145–47. http://dx.doi.org/10.1016/0375-9601(87)90295-7.

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44

Knyrim, Johanna S., and Hubert Huppertz. "Synthesis and crystal structure of the high-pressure iron borate α-FeB2O4." Journal of Solid State Chemistry 181, no. 8 (August 2008): 2092–98. http://dx.doi.org/10.1016/j.jssc.2008.05.016.

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45

Valverde-Canossa, J., W. Wieprecht, K. Acker, and G. K. Moortgat. "H2O2 and organic peroxide measurements in an orographic cloud: The FEBUKO experiment." Atmospheric Environment 39, no. 23-24 (July 2005): 4279–90. http://dx.doi.org/10.1016/j.atmosenv.2005.02.040.

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46

Matsouli, Ioanna, Vladimir V. Kvardakov, and José Baruchel. "Double-crystal diffraction imaging with a small effective divergence source: application to the magneto-acoustic vibrations in FeBO3." Journal of Applied Crystallography 33, no. 4 (August 1, 2000): 1051–58. http://dx.doi.org/10.1107/s0021889800004222.

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Ultrasonic standing waves, excited in FeBO3(111) crystal plates through magneto-elastic coupling, were visualized using monochromatic Bragg diffraction imaging (topography) with synchrotron radiation. The images depend strongly on whether diffraction by the sample occurs in the same plane as in the double-crystal monochromator, or in the perpendicular plane. The observations are explained by taking into account (a) the strong spatial dispersion which prevails because of the small effective divergence (angular size of the source as seen from a point in the specimen), which is less than one microradian in this experiment, and (b) the sample vibration and curvature.
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47

Massimiliano and Doriana Fuksas, Arquitectos. "Iglesia de San Paolo Foligno, Perugia. Italia." EN BLANCO. Revista de Arquitectura 5, no. 11 (April 18, 2013): 64. http://dx.doi.org/10.4995/eb.2013.6646.

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<p>Desde un punto de vista estructural, el edifi cio de la Iglesia también se concibe como una caja que contiene otra caja. El piso terminado, a 1,5 m del nivel del suelo está construido con una losa bidireccional de hormigón armado. La losa es de 40 cm de canto en la zona central y está construida con hormigón Rck clase 350, clase de exposición XC3-XF1, tipo SCC para mejorar la planeidad y el orifi cio de llenado durante la fase de vaciado. A lo largo del perímetro el canto de la losa se eleva a 60 cm con hormigón Rck clase 500, tipo SCC, en este ámbito, la losa recibe la carga de las columnas y las ménsulas. La losa en voladizo se ve reforzada con barras y perfi les FeB44K Fe510B de acero para apoyar los esfuerzos estructurales elevados transmitidos por la estructura.</p>
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Jędrych, Karolina. "Przesunięcie centrum świata i ucieczka na wieś w Febliku i Wnuczce od orzechów Małgorzaty Musierowicz." Annales Universitatis Paedagogicae Cracoviensis. Studia Poetica 6 (November 29, 2018): 52–63. http://dx.doi.org/10.24917/23534583.6.5.

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Re-centered of the world. Escape from city to the countryside in the newest novels by Małgorzata Musierowicz In this article I analyse two newest books by Małgorzata Musierowicz from the series Jeżycjada:Wnuczka do orzechów (2014) and Feblik(2015). Action of Jeżycjadatakes place in Poznań and its surroundings. Actually in the last two books action takes place mainly in this surroundings – at the countryside. Borejko family (main characters of the series) is spending there definitely more time than in the city. Seniors decided to go out of city. The result od this decision is that the centre of characters’ life has relocated. City is described as human’s enemy and countryside as a friendly space. In my article I interpret fragments which are describing this two areas. I answer the question why characters decided to move out form Poznań and stay at the countryside and how this change affects Borejko family.
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Sokolov, B. Yu. "Modulated magnetic structure of a nonuniformly stressed FeBO3 single crystal." JETP Letters 83, no. 9 (July 2006): 372–75. http://dx.doi.org/10.1134/s0021364006090025.

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Sadykov, E. K., A. Ya Dzyublik, G. I. Petrov, V. V. Arinin, and V. Yu Spivak. "Mössbauer forward scattering on FeBO3 in the RF remagnetization regime." JETP Letters 92, no. 4 (August 2010): 250–54. http://dx.doi.org/10.1134/s0021364010160113.

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