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1

Chen, Qi, Zhicheng Yan, Hao Zhang, et al. "High MB Solution Degradation Efficiency of FeSiBZr Amorphous Ribbon with Surface Tunnels." Materials 13, no. 17 (2020): 3694. http://dx.doi.org/10.3390/ma13173694.

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The as spun amorphous (Fe78Si9B13)99.5Zr0.5 (Zr0.5) and (Fe78Si9B13)99Zr1 (Zr1) ribbons having a Fenton-like reaction are proved to bear a good degradation performance in organic dye wastewater treatment for the first time by evaluating their degradation efficiency in methylene blue (MB) solution. Compared to the widely studied (Fe78Si9B13)100Zr0 (Zr0) amorphous ribbon for degradation, with increasing cZr (Zr atomic content), the as-spun Zr0, Zr0.5 and Zr1 amorphous ribbons have gradually increased degradation rate of MB solution. According to δc (characteristic distance) of as-spun Zr0, Zr0.5
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2

Zheng, Guo Tai, Zhao Hui Liu, and Da Guo Jiang. "GMI Effect of FeCoSiB Amorphous Ribbon." Advanced Materials Research 148-149 (October 2010): 644–48. http://dx.doi.org/10.4028/www.scientific.net/amr.148-149.644.

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The effects of AC frequency, magnetic field strength, ribbon length and test temperature on the Fe72Co8Si15B5 amorphous ribbon’s magnetic impedance were studied. The results showed that the resistance, reactance and impedance of amorphous ribbons increased with the increase of AC frequency, but decreased as magnetic field strength decreased; the rangeability of resistance, reactance and impedance increased as AC frequency and magnetic field strength increased; the resistance and reactance increased as ribbon length increased; the ribbon had a good temperature stability in resistance.
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3

Rapaport, David H. "Quantitative aspects of synaptic ribbon formation in the outer plexiform layer of the developing cat retina." Visual Neuroscience 3, no. 1 (1989): 21–32. http://dx.doi.org/10.1017/s0952523800012475.

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AbstractThe development of synaptic ribbons in rod and cone photoreceptor terminals of the cat retina was studied using quantitative electron microscopy. At the region of the area centralis, synaptic ribbon profiles are initially recognized at PCD (postconception day) 59. Synaptic ribbon density increases rapidly, reaching a peak of 0.55 ribbons/μm3 at PCD 68 (postnatal day 3) and maintains approximately that value for an additional 8 d. Following PCD 76, ribbon density begins to decrease, to 0.37 ribbons/μm3 at PCD 82 and 0.25 ribbons/μm3 at PCD 102. Although ribbon density drops by approxima
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4

Prusik, Krystian, Katarzyna Bałdys, Danuta Stróż, Tomasz Goryczka, and Józef Lelątko. "Microstructural Studies of NiCoMnIn Magnetic Shape Memory Ribbons." Materials Science Forum 738-739 (January 2013): 436–40. http://dx.doi.org/10.4028/www.scientific.net/msf.738-739.436.

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In present paper two ribbons of the Ni44Co6Mn36In14 (at.%) were prepared under different melt-spinning technique conditions. Microstructure of the ribbons was studied by scanning electron microscopy (SEM). Depending on the liquid ejection overpressure two types of ribbons microstructures were observed. Ribbon T1 for which ejection overpressure was 1.5 bar showed typical melt-spun ribbon microstructure consisting of a top layer of small equi-axial grains and columnar grains below. For T2 ribbon (ejection overpressure 0.2 bar) only a small fraction of the columnar grains were observed. Structure
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5

BALKEMA, GRANT W., KATHLEEN CUSICK, and TRI-HUNG NGUYEN. "Diurnal variation in synaptic ribbon length and visual threshold." Visual Neuroscience 18, no. 5 (2001): 789–97. http://dx.doi.org/10.1017/s0952523801185123.

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Previous work suggests that photoreceptor synaptic ribbon length and absolute dark-adapted threshold may vary during a 24-h diurnal cycle. To test this hypothesis, we examined the length of photoreceptor synaptic ribbons and the dark-adapted threshold in black (+/+) and albino (c2J/c2J) C57BL/6J mice at six times over a 24-h period. Testing began 2 h after light onset (ZT 2:00) and continued at successive 4-h intervals (12 h:12 h light:dark). We determined the length of the synaptic ribbons in frozen sections by labeling them with an antibody specific for synaptic ribbons. Synaptic ribbons var
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6

Yan, A.-Ru, Zhi-Gang Sun, Wen-Yong Zhang, Hong-Wei Zhang, and Bao-Gen Shen. "Magnetic properties, domain structure, and microstructure of anisotropic SmCo6.5Zr0.5 ribbons with C addition." Journal of Materials Research 16, no. 3 (2001): 629–32. http://dx.doi.org/10.1557/jmr.2001.0095.

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The magnetic properties and the domain structure of anisotropic melt-spun SmCo6.5Zr0.5 alloys with C addition was investigated by means of x-ray diffraction (XRD), magnetic measurement, and magnetic force microscopy. The XRD analyses showed that the addition of a few percent of C led to a significant increase in the coercivity and simultaneously affected the characterization of crystalline texture of the ribbons. The easy magnetization c axis changed from parallel to the ribbon plane for SmCo6.5Zr0.5 ribbons to normal to the ribbon plane for SmCo6.5Zr0.5C0.25−0.75 ribbons. An optimal coercivit
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7

He, J., L. Zhou, D. L. Zhao, and X. L. Wang. "Hysteresis loop shift behavior of CoFeSiB amorphous ribbons." Journal of Materials Research 24, no. 4 (2009): 1607–10. http://dx.doi.org/10.1557/jmr.2009.0185.

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Exchange bias phenomena of amorphous CoFeSiB ribbons have been probed at room temperature. The dramatic loop shift away from zero point occurred when the ribbons were annealed in ambient atmosphere with longitudinal field. The possible crystalline phases grown in our ribbons are discussed based on the grazing incidence diffraction and energy dispersive x-ray spectroscopy. The magnetic domain configuration of ribbon surface was also observed to make clear the dependence of bias behavior on the induced magnetic anisotropy in the ribbon. A simple phenomenological explanation was given to discuss
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8

Liu, Hao, Haiou Wang, Meng Xiong Cao, et al. "Structure and Magnetostriction of Melt-Spun Fe81-xNixGa19(x=0,5,10,15,20,25) Alloys." Applied Mechanics and Materials 372 (August 2013): 21–25. http://dx.doi.org/10.4028/www.scientific.net/amm.372.21.

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Fe81-xNixGa19(with x ranging from 0-25 at.% Ni) ribbons were made by melt spinning method. We have studied the structural (phases, texturing, and lattice parameter), magnetic (saturation magnetization and saturation magnetostriction) properties of these ribbons. The main results are as follows: (i) For x≤10, all the ribbons are A2 single phase; for x=15, the ribbon is of A2+L12+DO3+E21 phase; for x=20, the ribbon is of A2+L12+DO3+B2 phase; for x=25, only A2 and L12 phases exist. (ii) For x=5 and 15, an obvious (211) texture was detected, whereas other ribbons are (110) textured, no (100) textu
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9

Francis, Adam A., Bhupesh Mehta, and David Zenisek. "Development of new peptide-based tools for studying synaptic ribbon function." Journal of Neurophysiology 106, no. 2 (2011): 1028–37. http://dx.doi.org/10.1152/jn.00255.2011.

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Synaptic ribbons are proteinaceous specialized electron-dense presynaptic structures found in nonspiking sensory cells of the vertebrate nervous system. Understanding the function of these structures is an active area of research (reviewed in Matthews G, Fuchs P. Nat Rev Neurosci 11: 812–822, 2010). Previous work had shown that ribbons could be effectively labeled and visualized using peptides that bind to the synaptic ribbon protein RIBEYE via a PXDLS motif (Zenisek D, Horst NK, Merrifield C, Sterling P, Matthews G. J Neurosci 24: 9752–9759, 2004). Here, we expand on the previous work to deve
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10

Nguyen, Hai-Yen, Huy-Ngoc Nguyen, Xuan-Hau Kieu, et al. "Structure, magnetic properties and magnetocaloric effect of \(Fe_{81-x}Cr_{x+4}B_2Zr_{10}Nd_3\) rapidly quenched alloys." HPU2 Journal of Science: Natural Sciences and Technology 3, no. 2 (2024): 10–17. http://dx.doi.org/10.56764/hpu2.jos.2024.3.2.10-17.

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This paper presents, we present the structure, magnetic properties, and magnetocaloric effect of the Fe81-xCrx+4B2Zr10Nd3 (x = 0, 1, 2, and 3) alloy ribbons. The alloy ribbons were prepared by using the melt-spinning method. Structural analysis by X-ray diffraction shows that the obtained alloy ribbons are almost amorphous. Curie temperature of the alloy ribbons decreases from 310 to 275 K when x increases from 0 to 3. Under a magnetic field change of 12 kOe, the maximum magnetic entropy change \(|\Delta S_m|_{\text{max}}\) of the Fe80Cr5B2Zr10Nd3 alloy ribbon is found to be 1.05 J.kg-1.K-1 at
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11

Wang, Jian, Feng Luo, Can Zhu, et al. "Linear magnetoresistance in textured Bi1−xSbx ribbons prepared by melt spinning method." Journal of Applied Physics 132, no. 13 (2022): 135103. http://dx.doi.org/10.1063/5.0112457.

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Bi1− xSb x alloys with large linear magnetoresistance (LMR) are a promising candidate for magneto-electronic devices. In this work, the highly (00 l) textured Bi1− xSb x (0 ≤ x ≤ 0.04) ribbons with nano-sized lamellar grains were prepared by the melt spinning method and their magneto-transport properties were investigated. All the ribbons exhibit obvious LMR features, and the crossover magnetic field ( Bc) from quadratic to linear magnetoresistance is remarkably reduced by Sb doping. Compared with the Bc of the x = 0 ribbon (about 1.28 T at 300 K), the Bc values of the Sb doped ribbons are sig
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12

Juozapaitis, Algirdas, Giedrė Sandovič, Ronaldas Jakubovskis, and Viktor Gribniak. "Effects of Flexural Stiffness on Deformation Behaviour of Steel and FRP Stress-Ribbon Bridges." Applied Sciences 11, no. 6 (2021): 2585. http://dx.doi.org/10.3390/app11062585.

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Stress-ribbon systems develop the most flexible and slender bridges. A structural system of such elegant bridges consists of cables or ribbons and deck slabs placed to these strips to distribute the live load. Although this structural system is simple, the design of such structures is a challenging issue. Design limitations of the bridge deck slope induce considerable forces in the ribbons, which transfer the tension to massive foundations. The deformation increase under concentrated and asymmetrical loads causes another problem of stress-ribbon bridges—the kinematic component, the design obje
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13

Nguyen, Xuan Truong, Hong Ky Vu, Hung Manh Do, Van Khanh Nguyen, and Van Vuong Nguyen. "The Effect of External Magnetic Field on Microstructure and Magnetic Properties of Melt-Spun Nd-Fe-B/Fe-Co Nanocomposite Ribbons." Advances in Materials Science and Engineering 2013 (2013): 1–5. http://dx.doi.org/10.1155/2013/927356.

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The ribbons Nd2Fe14B/Fe-Co were prepared with the nominal composition Nd16Fe76B8/40% wt. Fe65Co35by the conventional and the developed magnetic field-assisted melt-spinning (MFMS) techniques. Both ribbons are nanocomposites with the smooth single-phase-like magnetization loops. The 0.32 T magnetic field perpendicular to the wheel surface and assisting the melt-spinning process reduces the grain size inside the ribbon, increases the texture of the ribbon, improves the exchange coupling, and, in sequence, increases the energy product(BH)maxof the isotropic powdered samples of MFMS ribbon in ~9%
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14

Li, Liang Feng, Tai Qiu, Jian Yang, and Yong Bao Feng. "Solidification Structure Characteristics and Mechanical Properties of (Ag-Cu28)-25Sn Alloy Ribbons Prepared by Melt Spinning Method." Materials Science Forum 682 (March 2011): 75–79. http://dx.doi.org/10.4028/www.scientific.net/msf.682.75.

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To obtain novel intermediate temperature alloy solders with melting temperature of 400~600°C, (Ag-Cu28)-25Sn alloy ribbons were prepared by high frequency induction melting and melt spinning at different quenching linear speed. The effect of the development of solidification structure on melting properties and microhardness of the ribbons were investigated. The XRD results show that the as-prepared alloy ribbons have the same phase composition as the master alloy, which consists of Ag4Sn and Cu3Sn. With the quenching linear speed increasing, the solidification structures are refined and change
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15

Ying, Weiyi, Zhengli Yang, Xiang Liu, Qingrong Yao, and Jiang Wang. "Effects of Lanthanum Element and Heat Treatment on Phase Formation and Magnetic Properties of SmFe10V2 Melt-Spun Ribbons." Materials 18, no. 10 (2025): 2322. https://doi.org/10.3390/ma18102322.

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The effects of the La element and heat treatment on the phase composition and magnetic properties of SmFe10V2 melt-spun ribbons are studied by X-ray diffraction (XRD) and vibrating sample magnetometry (VSM). The XRD results show that the Sm1−xLaxFe10V2 (x = 0, 0.2, 0.4) and SmLayFe10V2 (y = 0.1, 0.2, 0.3) melt-spun ribbons are composed of the 1:12 main phase with a ThMn12 structure, α-Fe phase and α-La phase, and the phase formation of the SmLa0.2Fe10V2 melt-spun ribbon is not changed after annealing at different temperatures (700–900 °C) and times (10–60 min). The XRD results indicate that La
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16

Dittrich, Alina, Girish Ramesh, Martin Jung та Frank Schmitz. "Rabconnectin-3α/DMXL2 Is Locally Enriched at the Synaptic Ribbon of Rod Photoreceptor Synapses". Cells 12, № 12 (2023): 1665. http://dx.doi.org/10.3390/cells12121665.

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Ribbon synapses reliably transmit synaptic signals over a broad signalling range. Rod photoreceptor ribbon synapses are capable of transmitting signals generated by the absorption of single photons. The high precision of ribbon synapses emphasizes the need for particularly efficient signalling mechanisms. Synaptic ribbons are presynaptic specializations of ribbon synapses and are anchored to the active zone. Synaptic ribbons bind many synaptic vesicles that are delivered to the active zone for continuous and faithful signalling. In the present study we demonstrate with independent antibodies a
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17

Ke, Qingjin, Feilong Dai, Shengxi Li, Maohua Rong, Qingrong Yao, and Jiang Wang. "Phase Formation, Microstructure, and Magnetic Properties of Nd14.5Fe79.3B6.2 Melt-Spun Ribbons with Different Ce and Y Substitutions." Materials 14, no. 14 (2021): 3992. http://dx.doi.org/10.3390/ma14143992.

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Phase formation and microstructure of (Nd1-2xCexYx)14.5Fe79.3B6.2 (x = 0.05, 0.10, 0.15, 0.20, 0.25) alloys were studied experimentally. The results reveal that (Nd1-2xCexYx)14.5Fe79.3B6.2 annealed alloys show (NdCeY)2Fe14B phase with the tetragonal Nd2Fe14B-typed structure (space group P42/mnm) and rich-RE (α-Nd) phase, while (Nd1-2xCexYx)14.5Fe79.3B6.2 ribbons prepared by melt-spun technology are composed of (NdCeY)2Fe14B phase, α-Nd phase and α-Fe phase, except for the ribbon with x = 0.25, which consists of additional CeFe2 phase. On the other hand, magnetic properties of (Nd1-2xCexYx)14.5
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18

Jing, Ju, Jeongwoo Lee, Mia Mancuso, et al. "Magnetic Eruption from a Three-ribbon Flare." Astrophysical Journal 972, no. 1 (2024): 110. http://dx.doi.org/10.3847/1538-4357/ad5ce3.

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Abstract We present observations and analysis of an eruptive M1.5 flare (SOL2014-08-01T18:13) in NOAA active region (AR) 12127, characterized by three flare ribbons, a confined filament between ribbons, and rotating sunspot motions as observed by the Solar Dynamics Observatory. The potential field extrapolation model shows a magnetic topology involving two intersecting quasi-separatrix layers (QSLs) forming a hyperbolic flux tube (HFT), which constitutes the fishbone structure for the three-ribbon flare. Two of the three ribbons show separation from each other, and the third ribbon is rather s
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19

Yan, A.-Ru, Zhi-Gang Sun, Baoshan Han, and Bao-Gen Shen. "Magnetic Anisotropy of Sm(Co0.68Fe0.22Cu0.08Zr0.02)7.7 Ribbons Produced by Melt Spinning." Journal of Materials Research 17, no. 3 (2002): 648–52. http://dx.doi.org/10.1557/jmr.2002.0092.

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A high degree of texture was observed in melt-spun Sm(Co0.68Fe0.22Cu0.08Zr0.02)7.7 ribbons prepared by single-roller melt spinning at low wheel speed; their easy magnetization axis was parallel to the ribbon plane. Magnetization studies showed an obvious magnetic anisotropy and a 90% higher remanance in ribbons for the field parallel to the longitudinal direction (8.5 kGs) than that for the field parallel to the wide direction (4.4 kGs); this was attributed to a dendritic structure of needle-size grains (2–3 × 10–40 μm) with their long axis parallel to the ribbon plane. This texture allowed th
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20

Huang, S. C., E. L. Hall, and M. F. X. Gigliotti. "Rapidly solidified Al3Ti-base alloys containing Ni." Journal of Materials Research 3, no. 1 (1988): 1–7. http://dx.doi.org/10.1557/jmr.1988.0001.

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Two Ni-modified Al3Ti alloys (Al65Ni10Ti25 and Al62Ni8Ti30) were rapidly solidified by melt spinning. The resulting microstructure was studied using light microscopy and analytical electron microscopy. Significant variations in the microstructure and phases were observed between the two ribbons and through the thickness of each ribbon.A single-phase γ-TiAl structure was seen near the wheel side of the Al62Ni8Ti30 ribbon, having microcrystalline grains ∼ 100 nm in diameter. Second-phase particles of Λ-AlNiTi were found in the remaining regions of that ribbon as the structure became columnar due
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21

Serra, Filipe, Ivo Costa, José A. Silva, and João M. Serra. "Optical Recrystallization of Nanocrystalline Silicon Ribbons." Metals 13, no. 3 (2023): 452. http://dx.doi.org/10.3390/met13030452.

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The Silicon on Dust Substrate (SDS) is a gas-to-wafer process that produces multicrystalline silicon ribbons directly from gaseous feedstock (silane), avoiding the standard industry steps of polysilicon deposition, crystal growth, and wafering. The SDS technique consists of three main steps: (i) micrometric-sized silicon powder production by grinding silicon chunks; (ii) chemical vapor deposition (CVD) of silicon over this silicon powder substrate; and (iii) zone-melting recrystallization (ZMR) of the nanocrystalline pre-ribbon obtained in the CVD step. Several samples were produced by this te
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22

Bailey, J. K., G. A. Pozarnsky, and M. L. Mecartney. "The direct observation of structural development during vanadium pentoxide gelation." Journal of Materials Research 7, no. 9 (1992): 2530–37. http://dx.doi.org/10.1557/jmr.1992.2530.

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The sequence of structural evolution in the gelation of vanadic acid to form vanadium pentoxide gels was studied using cryogenic transmission electron microscopy (cryo-TEM) and scanning tunneling microscopy (STM). Small whiskers form from initially homogeneous solutions, and then grow into crystalline ribbon-like colloidal particles. It is proposed that the whiskers form from polymerization of dioxovanadium cations. The ribbons then grow by continued addition of dioxovanadium cations which are supplied by the decomposition of decavanadate ions. In solution, the ribbon-like particles have dimen
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23

TIVAKORNASITHORN, K., S. NILPAIRUCH, S. VATANAYON, and I. M. TANG. "MAGNETIC PROPERTIES OF AMORPHOUS Fe40Ni38B18Mo4 RIBBONS CONTAINING NANOCRYSTALLITES." Modern Physics Letters B 19, no. 06 (2005): 295–302. http://dx.doi.org/10.1142/s0217984905008347.

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Cut Fe 40 Ni 38 B 18 Mo 4 ribbons were annealed for two hours at various temperatures Ta between 400 and 540°C. All the ribbons were subjected to XRD, VSM (vibrating sample magnetometer) and ME (Mossbauer effect spectroscopy) investigations. A differential thermal analysis scan of an as-cast ribbon showed the presence of two exothermic peaks, the first beginning at 419.9°C and peaking at 429.7°C and the second beginning at 497.3°C and ending at 546.2°C. The XRD patterns of the ribbons showed the formation of FeNi 3 nanocrystallites in the lower T'a ribbons and (Fe, Ni, Mo) 23 B 6 crystallites
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24

Nguyen, Yen, Mai Nguyen, Quang Vu, et al. "Investigation of magnetic phase transition and magnetocaloric effect of (Ni,Co)-Mn-Al melt-spun ribbons." EPJ Web of Conferences 185 (2018): 05001. http://dx.doi.org/10.1051/epjconf/201818505001.

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Magnetic phase transition, magnetocaloric effect and critical parameters of Ni50-xCoxMn50-yAly (x = 5 and 10; y = 17, 18 and 19) rapidly quenched ribbons have been studied. X-ray diffraction patterns exhibit a coexistence of the L21 and 10M crystalline phases of the ribbons. Magnetization measurements show that all the samples behave as soft magnetic materials with a low coercive force less than 60 Oe. The shape of thermomagnetization curves considerably depends on Co and Al concentrations. The Curie temperature (TC) of the alloy ribbons strongly increases with increasing the Co concentration
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25

Cai, Shuxian, Xingfang Liu, Xin Zheng, and Zhonghua Liu. "Growth of Ordered Graphene Ribbons by Sublimation Epitaxy." Crystals 8, no. 12 (2018): 449. http://dx.doi.org/10.3390/cryst8120449.

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Ordered graphene ribbons were grown on the surface of 4° off-axis 4H-SiC wafers by sublimation epitaxy, and characterized by using scanning electron microscopy (SEM), atomic force microscopy (AFM) and micro-Raman spectroscopy (μ-Raman). SEM showed that there were gray and dark ribbons on the substrate surface, and AFM further revealed that these ordered graphene ribbons had clear stepped morphologies due to surface step-bunching. It was shown by μ-Raman that the numbers of graphene layers of these two types of regions were different. The gray region was composed of mono- or bilayer ordered gra
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26

Buršík, Jiří, Vilma Buršíková, and Yvonna Jirásková. "Study of the Mechanical Properties of Single-Layered and Bilayered CoCrFeSi Ribbons Using Quasistatic and Dynamic Nanoindentation Tests." Key Engineering Materials 662 (September 2015): 91–94. http://dx.doi.org/10.4028/www.scientific.net/kem.662.91.

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In this work we have studied local mechanical properties of CoCrFeSiB ribbons prepared by planar flow casting (PFC). Recently improved PFC technology enabled us to use two melts simultaneously and to prepare a bilayered Co69Fe2Cr7Si8B14/Co59Fe12Cr7Si8B14 ribbon with a good homogeneity of the layers and well defined interface. Single-layered ribbons of the two compositions above were prepared as well. The microstructure and the composition profiles were studied by means of analytical electron microscopy. Nanoindentation tests were carried out on the cross sections of the bilayered ribbon as wel
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27

Prior, Chris, Julien Moussou, Buddhapriya Chakrabarti, Oliver E. Jensen, and Anne Juel. "Ribbon curling via stress relaxation in thin polymer films." Proceedings of the National Academy of Sciences 113, no. 7 (2016): 1719–24. http://dx.doi.org/10.1073/pnas.1514626113.

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The procedure of curling a ribbon by running it over a sharp blade is commonly used when wrapping presents. Despite its ubiquity, a quantitative explanation of this everyday phenomenon is still lacking. We address this using experiment and theory, examining the dependence of ribbon curvature on blade curvature, the longitudinal load imposed on the ribbon, and the speed of pulling. Experiments in which a ribbon is drawn steadily over a blade under a fixed load show that the ribbon curvature is generated over a restricted range of loads, the curvature/load relationship can be nonmonotonic, and f
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28

Li, Li Ya, Yi Cheng Ge, and Yuan Dong Peng. "Microstructure and Magnetic Properties of Rapidly Solidified Sm(CobalFe0.11Cu0.10Zrx)7 Alloys." Advanced Materials Research 893 (February 2014): 357–60. http://dx.doi.org/10.4028/www.scientific.net/amr.893.357.

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We reported a systematic study of the effect of Zr content on the structural and magnetic properties of rapidly quenched Sm (CobalFe0.11Cu0.10Zrx)7 alloys with x varying from 0 to 0.04. The results show that the addition of Zr greatly affected the microstructure and magnetic properties of the heat-treated ribbons. The Zr-free ribbon had crystallized as the 1:7H structure as the main phase while the ribbon with Zr addition adopted the 2:17R structure type. A Sm2Co7 phase was observed in the heat-treated ribbons when the Zr content x increased to 0.04. It is found that while the Zr content was i
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29

Saage, G., S. Roth, J. Eckert, and L. Schultz. "Extraction of boron Fe8B2 ribbons by annealing under hydrogen flow." Journal de Physique IV 120 (December 2004): 55–59. http://dx.doi.org/10.1051/jp4:2004120005.

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Transition metal alloys often are difficult to be prepared as ribbons by conventional methods. If boron is added to these alloys, amorphous ribbons may be prepared by melt spinning. These amorphous ribbons have a better workability than their crystalline counterparts. However, the composition is different from the target composition. Upon annealing treatments in flowing hydrogen the boron may be extracted and the ribbon crystallizes. Thermodynamically the extraction of boron proceeds by the reaction of hydrogen with the borides formed during the crystallization of the ribbons. In order to inve
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30

Arreguín-Hernández, M. L., A. Dzubinska, M. Reiffers, J. L. Sánchez Llamazares, C. F. Sánchez-Valdés, and R. Varga. "Magnetostructural transition and magnetocaloric effect in Mn0.5Fe0.5NiSi1−xAlx melt-spun ribbons (x = 0.055 and 0.060)." AIP Advances 13, no. 2 (2023): 025336. http://dx.doi.org/10.1063/9.0000554.

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Melt-spun ribbons samples of the multicomponent alloy Mn0.5Fe0.5NiSi0.940Al0.060 were prepared and the magnetostructural transition (MST) and related magnetocaloric properties studied for as-solidified ribbons and ribbon samples annealed between 800 and 950 °C for 4 h. The results are compared with those reported in the literature for melt-spun ribbons with an Al content x = 0.055 and bulk alloys. It is shown that all samples undergo a first-order MST from a paramagnetic Ni2In-type hexagonal structure to a ferromagnetic TiNiSi-type orthorhombic one. Ribbons show broader isothermal entropy chan
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31

Yuan, Yasheng, and Fanglu Chi. "Dynamic changes in hair cell ribbon synapse induced by loss of spiral ganglion neurons in mice." Chinese Medical Journal 127, no. 10 (2014): 1941–46. http://dx.doi.org/10.3760/cma.j.issn.0366-6999.20132520.

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Background Previous studies have suggested that primary degeneration of hair cells causes secondary degeneration of spiral ganglion neurons (SGNs), but the effect of SGN degeneration on hair cells has not been studied. In the adult mouse inner ear ouabain can selectively and permanently induce the degeneration of type 1 SGNs while leaving type 2 SGNs, efferent fibers, and sensory hair cells relatively intact. This study aimed to investigate the dynamic changes in hair cell ribbon synapse induced by loss of SGNs using ouabain application to the round window niche of adult mice. Methods In the a
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32

Hong, Juan, Yan Chen, Yanping Zhang, et al. "N-Methyl-D-Aspartate Receptors Involvement in the Gentamicin-Induced Hearing Loss and Pathological Changes of Ribbon Synapse in the Mouse Cochlear Inner Hair Cells." Neural Plasticity 2018 (July 15, 2018): 1–16. http://dx.doi.org/10.1155/2018/3989201.

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Cochlear inner hair cell (IHC) ribbon synapses play an important role in sound encoding and neurotransmitter release. Previous reports show that both noise and aminoglycoside exposures lead to reduced numbers and morphologic changes of synaptic ribbons. In this work, we determined the distribution of N-methyl-D-aspartate receptors (NMDARs) and their role in the gentamicin-induced pathological changes of cochlear IHC ribbon synaptic elements. In normal mature mouse cochleae, the majority of NMDARs were distributed on the modiolar side of IHCs and close to the IHC nuclei region, while most of sy
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33

YE, EN-JIA, YI-JIAN SHI, and XUEAN ZHAO. "ELECTRON TRANSPORT IN MULTI-TERMINAL GRAPHENE NANODEVICE WITH INCLINED CROSS STRUCTURES." International Journal of Modern Physics B 28, no. 09 (2014): 1450035. http://dx.doi.org/10.1142/s0217979214500350.

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The DC and AC transport properties are investigated in multi-terminal graphene nanoribbon (GNR) devices. The devices are composed of three or four graphene ribbons connected with different angles. It is found that DC and AC conductances depend on the structural configurations and ribbon properties. In the vicinity of Dirac point, the intersection of graphene ribbons forms band mixing and results in resonant or anti-resonant states. The edge and width, as well as, the angles of the graphene ribbons influence the DC and AC transport properties drastically. These properties can be used to build f
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34

Golubeva, Elizaveta V., Anna A. Chlenova, Elena A. Stepanova, and Galina V. Kurlyandskaya. "Magnetic properties and giant magnetoimpedance of surface modified Co-based amorphous ribbons with carbon covering." EPJ Web of Conferences 185 (2018): 10001. http://dx.doi.org/10.1051/epjconf/201818510001.

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Fe3Co66Cr3Si16B12 and Fe6Co60Ni10Si14B10 amorphous ribbons were surface modified in toluene at room temperature. Such a treatment resulted in deposition of thin carbon-based layer. As a result of the carbon covering deposition the stress distribution in the near-surface layers was changed due to partial compensation of the initial quenching stresses. Comparative analysis of magnetic and magnetoimpedance properties of as-quenched and surface modified ribbons confirms changes in effective magnetic anisotropy as a result of surface treatment. An increase of the corrosion resistance of the ribbons
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35

Orlov, V. A., R. Yu Rudenko, A. V. Luk’yanenko, et al. "Features of the Magnetic State of an Ordered Array of Ferromagnetic Ribbons." Физика металлов и металловедение 124, no. 2 (2023): 117–25. http://dx.doi.org/10.31857/s0015323022601295.

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The features of the magnetic state of an array of parallel oriented permalloy ribbons are discussed. The arrays are made by explosive lithography. The ribbons have a thickness of 180 nm, a width of 2.8 μm, and a length of about 4 mm. The distance between ribbons in different samples varies in the range from 300 nm to 4 μm. It is found that the ribbons in the regions far from the end faces are in a single-domain state with small-angle ripples, the magnetization distribution of which correlates with inhomogeneities of the ribbon side surfaces. Moreover, there is a distinct relationship in the sp
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36

Schwarz, Karin, and Frank Schmitz. "RIBEYE(B)-domain binds to lipid components of synaptic vesicles in an NAD(H)-dependent, redox-sensitive manner." Biochemical Journal 474, no. 7 (2017): 1205–20. http://dx.doi.org/10.1042/bcj20160886.

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Synaptic ribbons are needed for fast and continuous exocytosis in ribbon synapses. RIBEYE is a main protein component of synaptic ribbons and is necessary to build the synaptic ribbon. RIBEYE consists of a unique A-domain and a carboxyterminal B-domain, which binds NAD(H). Within the presynaptic terminal, the synaptic ribbons are in physical contact with large numbers of synaptic vesicle (SV)s. How this physical contact between ribbons and synaptic vesicles is established at a molecular level is not well understood. In the present study, we demonstrate that the RIBEYE(B)-domain can directly in
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37

Suiwal, Shweta, Karin Schwarz, Stephan Maxeiner, and Frank Schmitz. "The Plus End-Directed Microtubule (Kinesin-3 Family) Motor Protein KIF13B Is Associated with the Photoreceptor Synaptic Ribbon Complex." International Journal of Molecular Sciences 26, no. 13 (2025): 6044. https://doi.org/10.3390/ijms26136044.

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Retinal ribbon synapses are continuously active chemical synapses. The eponymous synaptic ribbon is anchored to the active zone neurotransmitter release sites of ribbon synapses, recruits synaptic vesicles and guides ribbon-associated synaptic vesicles to the release sites. RIBEYE is the major protein component of synaptic ribbons. But likely, additional proteins contribute to ribbon synapse function. The synaptic ribbon of photoreceptor synapses is embedded into a highly polarized microtubule cytoskeleton. Interestingly, proteins of the photoreceptor primary cilium, such as NPHP4 and other ci
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38

Xing, Hongyang, Anak Khantachawana, Hee Young Kim, and Shuichi Miyazaki. "Effect of Ni-Content on Shape Memory Behavior of Ti-Rich Ti-Ni Melt-Spun Ribbons." Materials Science Forum 475-479 (January 2005): 1925–28. http://dx.doi.org/10.4028/www.scientific.net/msf.475-479.1925.

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The microstructure and shape memory behavior of Ti-rich Ti-Ni melt-spun ribbons with various Ni-contents were investigated. Ti-xNi(x=40~48at%) ribbons were fabricated by the melt-spinning method at the rotation speed of 5000rpm. They were heat-treated at 1073K for 3.6ks. It was found that the Ti-40at%Ni as-spun ribbon exhibited almost complete amorphous structure, while the specimen with more Ni-content, such as 48at%Ni ribbon exhibited the coexistence of amorphous and crystalline structures. It was also found that the maximum shape recovery strain increased with increasing Ni-content. The Ti-
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39

Frederick, Courtney E., and David Zenisek. "Ribbon Synapses and Retinal Disease: Review." International Journal of Molecular Sciences 24, no. 6 (2023): 5090. http://dx.doi.org/10.3390/ijms24065090.

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Synaptic ribbons are presynaptic protein complexes that are believed to be important for the transmission of sensory information in the visual system. Ribbons are selectively associated with those synapses where graded changes in membrane potential drive continuous neurotransmitter release. Defective synaptic transmission can arise as a result of the mutagenesis of a single ribbon component. Visual diseases that stem from malfunctions in the presynaptic molecular machinery of ribbon synapses in the retina are rare. In this review, we provide an overview of synaptopathies that give rise to reti
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40

Warshawsky, H. "Enamel Crystal Shape: History of an Idea." Advances in Dental Research 1, no. 2 (1987): 322–29. http://dx.doi.org/10.1177/08959374870010022401.

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The purpose of this paper is to review evidence which casts doubt on the interpretation universally applied to hexagonal images seen in sectioned enamel. The evidence is based on two possible models to explain the hexagonal profiles seen in mammalian enamel with transmission electron microscopy. The "hexagonal ribbon" model proposes that hexagonal profiles are true cross-sections of elongated hexagonal ribbons. The "rectangular ribbon" model proposes that hexagonal profiles are caused by three-dimensional segments that are parallelepipeds contained in the Epon section. Since shadow projections
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41

Norrander, Jan M., Aimee M. deCathelineau, Jennifer A. Brown, Mary E. Porter, and Richard W. Linck. "The Rib43a Protein Is Associated with Forming the Specialized Protofilament Ribbons of Flagellar Microtubules inChlamydomonas." Molecular Biology of the Cell 11, no. 1 (2000): 201–15. http://dx.doi.org/10.1091/mbc.11.1.201.

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Ciliary and flagellar microtubules contain a specialized set of three protofilaments, termed ribbons, that are composed of tubulin and several associated proteins. Previous studies of sea urchin sperm flagella identified three of the ribbon proteins astektins, which form coiled-coil filaments in doublet microtubules and which are associated with basal bodies and centrioles. To study the function of tektins and other ribbon proteins in the assembly of flagella and basal bodies, we have begun an analysis of ribbons from the unicellular biflagellate, Chlamydomonas reinhardtii, and report here the
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42

FENG, LIN, WENXING ZHANG, ENKE LIU, WENHONG WANG, and GUANGHENG WU. "MARTENSITIC TRANSFORMATION AND MAGNETIC PROPERTIES OF NiMnAl:Fe, Co FERROMAGNETIC SHAPE MEMORY ALLOYS." Functional Materials Letters 06, no. 06 (2013): 1350050. http://dx.doi.org/10.1142/s1793604713500501.

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A series of Ni 50-x Fe x Mn 34 Al 16(0 ≦ x ≦ 18) and Ni 38 Fe 12-z Co z Mn 34 Al 16(3 ≦ z ≦ 6) ribbons were prepared by the melt-spinning method. With Fe substitution for Ni in Ni 50 Mn 34 Al 16 ribbons, the magnetization of the austenitic phase increases greatly while that of the martensitic phase increases little. Thus, in the magnetic field of 5 T a large magnetization change (22 Am2/kg) during the martensitic transformation is observed in Ni 38 Fe 12 Mn 34 Al 16 ribbon. The effect of Fe substitution for Ni on the magnetic modulation was investigated, which is attributed to the change of th
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43

MORRIS, J. R. "NESTED DOMAIN DEFECTS." International Journal of Modern Physics A 13, no. 07 (1998): 1115–27. http://dx.doi.org/10.1142/s0217751x98000494.

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An example of a supersymmetric model involving two interacting chiral superfields is presented here which allows for solutions describing stringlike "domain ribbon" defects embedded within a domain wall. It is energetically favorable for the fermions within the wall to populate the domain ribbons, and an explicit solution is found for the fermion zero modes. The Fermi gas within ribbons can allow them to stabilize in the form of small loops.
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44

Legon, Edward. "Bound up with Meaning: The Politics and Memory of Ribbon Wearing in Restoration England and Scotland." Journal of British Studies 56, no. 1 (2017): 27–50. http://dx.doi.org/10.1017/jbr.2016.119.

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AbstractDuring the Exclusion Crisis (1678–83), political opinion polarized around the issue of who, or indeed what, should succeed Charles II. In addition to the labels “Whigs” and “Tories,” the rapid polarization of politics after 1681 resulted in the adoption of blue and red ribbons distinguishing the two movements. This article focuses on the Whigs’ blue ribbon, arguing that the device created the sense of an “imagined consensus” within the group's varied support base. The Whigs’ enemies used memories of Britain's troubled past in order to claim that ribbon wearing replicated the behavior o
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45

Dumin, Yu V., and B. V. Somov. "Topological model of the anemone microflares in the solar chromosphere." Astronomy & Astrophysics 623 (March 2019): L4. http://dx.doi.org/10.1051/0004-6361/201834645.

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Context. The chromospheric anemone microflares, which were discovered by Hinode satellite about a decade ago, are specific transient phenomena starting from a few luminous ribbons on the chromospheric surface and followed by an eruption upward. While the eruptive stage was studied in sufficient detail, a quantitative theory of formation of the initial multi-ribbon structure remains undeveloped until now. Aims. We construct a sufficiently simple but general model of the magnetic field sources that is able to reproduce all the observed types of luminous ribbons by varying only a single parameter
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46

Kim, H. J., K. K. Jee, H. W. Kang, J. K. Lee, G. S. Yang, and W. Y. Jang. "Effect of Grain Size on the Shape Recovery in a Melt-Spun Fe-24%Mn-4%Si-5%Cr-5%Co SMA Ribbon." Advanced Materials Research 488-489 (March 2012): 315–20. http://dx.doi.org/10.4028/www.scientific.net/amr.488-489.315.

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Effect of grain size on microstructure, transformation characteristics and shape recovery has been studied in Fe-24%Mn-4%Si-5%Cr-5%Co shape memory ribbons fabricated by melt spinning. Mean grain size of the ribbons could be controlled by wheel speed; in case of ribbon manufactured in the wheel speed of 10 m/sec, mean grain size was more or less 20 μm, while the mean grain size in 50 m/sec was about 1 μm. Thermal ε-martensite in the shape of plate could be observed in austenite matrix and the volume fraction of that decreased in smaller grains because of grain constraint. As a grain size decrea
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47

Chen, Shih Fan, Chih Yuan Chen, and Chien Fan Chiang. "The Influence of Annealing Temperature on Microstructure and Magnetic Properties of Fe74Co3Si8B10Al1Nb4 Amorphous Alloy Ribbons." Atlas Journal of Materials Science 2, no. 1 (2017): 44–47. http://dx.doi.org/10.5147/ajms.v2i1.122.

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Multi-component alloy ribbons with a composition of Fe74Co3Si8B10Al1Nb4 were prepared by a single roller melt-spinning method. The alloy had a fully amorphous structure, as determined by X-ray diffraction. The alloy ribbons were annealed for 10 min at temperatures of 350, 400, 450, 500, 550 and 600 oC, respectively. Differential scanning calorimetry curves indicated that the glass transition temperature (Tg) and the supercooled liquid range (ΔTx) of the amorphous alloy ribbon were about 494 oC and 43 oC, respectively. The ribbons showed soft magnetic properties, with a Curie temperature (Tc) a
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48

Huang, P. S., and G. Zhu. "Stress Analysis of Pressure Vessel With Wound-Flat Steel Ribbons." Journal of Pressure Vessel Technology 114, no. 1 (1992): 94–100. http://dx.doi.org/10.1115/1.2929019.

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Pressure vessels with wound-flat steel ribbons, also called ribbon-wound vessels, have excellent engineering and economic advantages and are widely used in the People’s Republic of China. A brief description of the structure and characteristics, and a comparison between the ribbon-wound technique with other methods are given. In this paper, a new mechanical model for the ribbons, in which the axial displacement and change of spiral angle are taken into account, is put forward. Then the universal formulas for the ribbon are obtained and a precise stress analysis of the vessel is presented. The
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49

Atalan, Cenk, and Taylan Eker. "PERFORMANCE EVALUATION OF GOLD (Au) WIRE AND RIBBON INTERCONNECTS IN HIGH FREQUENCY CIRCUITS." International Symposium on Microelectronics 2016, no. 1 (2016): 000450–55. http://dx.doi.org/10.4071/isom-2016-tha35.

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Abstract Gold (Au) wires and ribbons are widely being used in military and space applications of high frequency RF/microwave circuits. The purpose of this study is to examine the RF performance of different dimensions of Au wires & ribbons, which are typically bonded in cascade and parallel forms in the circuits operating microwave frequencies within 0–50 GHz. The second goal of this study is to establish a performance chart/handbook of Au wires, ribbons for high frequency circuit designers in order to show them which type of wire or ribbon as well as which type of interconnect form is sui
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50

Li, Dongyue, Chengshuang Wu, Yitian Su, Lu Xie, Yong Zhang, and Wenrui Wang. "Mechanical Response of Zr51.9Cu23.3Ni10.5Al14.3 Metallic Glass Ribbon under Varying Strain Rates." Metals 14, no. 2 (2024): 220. http://dx.doi.org/10.3390/met14020220.

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In this work, we investigated the mechanical behavior of a low-cost Zr51.9Cu23.3Ni10.5Al14.3 (at. %) metallic glass ribbon prepared with industrial-grade material through the melt-spinning method. The ribbons have good appearances and almost no defects. The mechanical behavior associated with the corresponding microstructure of the ribbon was tested at different strain rates. Striation and veining patterns were observed in the crack propagation zone and the fast fracture zone. The results show that the tensile strength of the ribbons exceeds 1 GPa. Therefore, they are considered to have good p
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