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Journal articles on the topic 'Y-junctions'

Author: Grafiati

Published: 4 June 2021

Last updated: 1 February 2022

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1

Ting, Lucas H., Jessica R. Jahn, Joon I. Jung, Benjamin R. Shuman, Shirin Feghhi, Sangyoon J. Han, Marita L. Rodriguez, and Nathan J. Sniadecki. "Flow mechanotransduction regulates traction forces, intercellular forces, and adherens junctions." American Journal of Physiology-Heart and Circulatory Physiology 302, no. 11 (June 1, 2012): H2220—H2229. http://dx.doi.org/10.1152/ajpheart.00975.2011.

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Endothelial cells respond to fluid shear stress through mechanotransduction responses that affect their cytoskeleton and cell-cell contacts. Here, endothelial cells were grown as monolayers on arrays of microposts and exposed to laminar or disturbed flow to examine the relationship among traction forces, intercellular forces, and cell-cell junctions. Cells under laminar flow had traction forces that were higher than those under static conditions, whereas cells under disturbed flow had lower traction forces. The response in adhesion junction assembly matched closely with changes in traction forces since adherens junctions were larger in size for laminar flow and smaller for disturbed flow. Treating the cells with calyculin-A to increase myosin phosphorylation and traction forces caused an increase in adherens junction size, whereas Y-27362 cause a decrease in their size. Since tugging forces across cell-cell junctions can promote junctional assembly, we developed a novel approach to measure intercellular forces and found that these forces were higher for laminar flow than for static or disturbed flow. The size of adherens junctions and tight junctions matched closely with intercellular forces for these flow conditions. These results indicate that laminar flow can increase cytoskeletal tension while disturbed flow decreases cytoskeletal tension. Consequently, we found that changes in cytoskeletal tension in response to shear flow conditions can affect intercellular tension, which in turn regulates the assembly of cell-cell junctions.

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2

Treboux, Gabin, Paul Lapstun, and Kia Silverbrook. "Conductance in nanotube Y-junctions." Chemical Physics Letters 306, no. 5-6 (June 1999): 402–6. http://dx.doi.org/10.1016/s0009-2614(99)00445-5.

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3

Li, W. Z., J. G. Wen, and Z. F. Ren. "Straight carbon nanotube Y junctions." Applied Physics Letters 79, no. 12 (September 17, 2001): 1879–81. http://dx.doi.org/10.1063/1.1404400.

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4

Wilson, Rab, Tim J. Karle, I. Moerman, and Thomas F. Krauss. "Efficient photonic crystal Y-junctions." Journal of Optics A: Pure and Applied Optics 5, no. 4 (June 25, 2003): S76—S80. http://dx.doi.org/10.1088/1464-4258/5/4/358.

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5

Lu, Longhui, Deming Liu, Max Yan, and Minming Zhang. "Subwavelength adiabatic multimode Y-junctions." Optics Letters 44, no. 19 (September 20, 2019): 4729. http://dx.doi.org/10.1364/ol.44.004729.

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6

Liu, Zhao-Miao, Li-Kun Liu, and Feng Shen. "Effects of geometric configuration on droplet generation in Y-junctions and anti-Y-junctions microchannels." Acta Mechanica Sinica 31, no. 5 (August 25, 2015): 741–49. http://dx.doi.org/10.1007/s10409-015-0420-y.

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7

Love, John D., and Nicolas Riesen. "Single-, Few-, and Multimode Y-Junctions." Journal of Lightwave Technology 30, no. 3 (February 2012): 304–9. http://dx.doi.org/10.1109/jlt.2011.2179976.

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8

Ding, Dongyan, Jiannong Wang, and Sheng Chen. "Junctions formed in Y Ba2Cu3O7 nanowires." Superconductor Science and Technology 17, no. 3 (January 20, 2004): 438–42. http://dx.doi.org/10.1088/0953-2048/17/3/023.

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9

Yun, Sang H., Judy Z. Wu, Alan Dibos, Xiaodong Zou, and Ulf O. Karlsson. "Self-Assembled Boron Nanowire Y-Junctions." Nano Letters 6, no. 3 (March 2006): 385–89. http://dx.doi.org/10.1021/nl052138r.

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10

Zhu, Guang, XiaoPing Zou, Jin Cheng, MaoFa Wang, and Yi Su. "Straight SiO x nanorod Y junctions." Science in China Series E: Technological Sciences 52, no. 1 (January 2009): 32–36. http://dx.doi.org/10.1007/s11431-009-0006-7.

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11

Steegmans, Maartje L. J., Karin G. P. H. Schroën, and Remko M. Boom. "Microfluidic Y-junctions: A robust emulsification system with regard to junction design." AIChE Journal 56, no. 7 (January 4, 2010): 1946–49. http://dx.doi.org/10.1002/aic.12094.

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12

Liu, Zhao Miao, and Li Kun Liu. "Numerical Analysis of Junction Point Pressure during Droplet Formation in Y-Junction Microchannel." Applied Mechanics and Materials 481 (December 2013): 241–46. http://dx.doi.org/10.4028/www.scientific.net/amm.481.241.

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Junction point pressure changes during droplet formation in Y-junction microchannels with differed Y-angles, wetting property and capillary number of the liquid by using a three dimensional numerical simulation. The pressure of the junction point fluctuates throughout the droplet formation process, and it can be used to depict exactly and directly different stages of droplet in microchannels. And the pressure of junctions with different Y-angles of microchannel, different contact angles of dispersed phase with the surface, and different capillary numbers of continuous phase could thus be investigated via the droplet formation mechanism.

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13

Tavares, J. M., and P. I. C. Teixeira. "Phase diagrams of particles with dissimilar patches: X-junctions and Y-junctions." Journal of Physics: Condensed Matter 24, no. 28 (June 27, 2012): 284108. http://dx.doi.org/10.1088/0953-8984/24/28/284108.

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14

Latgé, A., R. B. Muniz, and D. Grimm. "Carbon nanotube structures: Y-junctions and nanorings." Brazilian Journal of Physics 34, no. 2b (June 2004): 585–89. http://dx.doi.org/10.1590/s0103-97332004000400012.

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15

Egger, R., B. Trauzettel, S. Chen, and F. Siano. "Transport theory of carbon nanotube Y junctions." New Journal of Physics 5 (September 30, 2003): 117. http://dx.doi.org/10.1088/1367-2630/5/1/117.

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16

Kevrekidis, P. G., D. J. Frantzeskakis, G. Theocharis, and I. G. Kevrekidis. "Guidance of matter waves through Y-junctions." Physics Letters A 317, no. 5-6 (October 2003): 513–22. http://dx.doi.org/10.1016/j.physleta.2003.08.069.

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17

Riesen, Nicolas, and John D. Love. "Design of mode-sorting asymmetric Y-junctions." Applied Optics 51, no. 15 (May 11, 2012): 2778. http://dx.doi.org/10.1364/ao.51.002778.

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18

Dekkiche, L., and R. Naoum. "Improved transmission for photonic crystal Y-junctions." Electrical Engineering 89, no. 1 (December 20, 2005): 71–77. http://dx.doi.org/10.1007/s00202-005-0318-y.

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19

Biró, L. P., Z. E. Horváth, G. I. Márk, Z. Osváth, A. A. Koós, A. M. Benito, W. Maser, and Ph Lambin. "Carbon nanotube Y junctions: growth and properties." Diamond and Related Materials 13, no. 2 (February 2004): 241–49. http://dx.doi.org/10.1016/j.diamond.2003.10.014.

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20

Henry, Wanda M., and John D. Love. "Variational approximations for couplers and Y junctions." Optical and Quantum Electronics 17, no. 5 (September 1985): 359–70. http://dx.doi.org/10.1007/bf00620400.

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21

Jiang, Y. S., X. Y. Cai, K. Usami, T. Kobayashi, and T. Goto. "Fabrication and properties of YBa2Cu3O7−y/PrGaO3/YBa2Cu3O7−y tunnel junctions." Physica C: Superconductivity and its Applications 282-287 (August 1997): 2463–64. http://dx.doi.org/10.1016/s0921-4534(97)01307-5.

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22

Kong, Qiao, Woochul Lee, Minliang Lai, Connor G. Bischak, Guoping Gao, Andrew B. Wong, Teng Lei, et al. "Phase-transition–induced p-n junction in single halide perovskite nanowire." Proceedings of the National Academy of Sciences 115, no. 36 (August 20, 2018): 8889–94. http://dx.doi.org/10.1073/pnas.1806515115.

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Semiconductor p-n junctions are fundamental building blocks for modern optical and electronic devices. The p- and n-type regions are typically created by chemical doping process. Here we show that in the new class of halide perovskite semiconductors, the p-n junctions can be readily induced through a localized thermal-driven phase transition. We demonstrate this p-n junction formation in a single-crystalline halide perovskite CsSnI3 nanowire (NW). This material undergoes a phase transition from a double-chain yellow (Y) phase to an orthorhombic black (B) phase. The formation energies of the cation and anion vacancies in these two phases are significantly different, which leads to n- and p- type electrical characteristics for Y and B phases, respectively. Interface formation between these two phases and directional interface propagation within a single NW are directly observed under cathodoluminescence (CL) microscopy. Current rectification is demonstrated for the p-n junction formed with this localized thermal-driven phase transition.

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23

Ifland, Benedikt, Patrick Peretzki, Birte Kressdorf, Philipp Saring, Andreas Kelling, Michael Seibt, and Christian Jooss. "Current–voltage characteristics of manganite–titanite perovskite junctions." Beilstein Journal of Nanotechnology 6 (July 7, 2015): 1467–84. http://dx.doi.org/10.3762/bjnano.6.152.

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After a general introduction into the Shockley theory of current voltage (J–V) characteristics of inorganic and organic semiconductor junctions of different bandwidth, we apply the Shockley theory-based, one diode model to a new type of perovskite junctions with polaronic charge carriers. In particular, we studied manganite–titanate p–n heterojunctions made of n-doped SrTi1− y Nb y O3, y = 0.002 and p-doped Pr1− x Ca x MnO3, x = 0.34 having a strongly correlated electron system. The diffusion length of the polaron carriers was analyzed by electron beam-induced current (EBIC) in a thin cross plane lamella of the junction. In the J–V characteristics, the polaronic nature of the charge carriers is exhibited mainly by the temperature dependence of the microscopic parameters, such as the hopping mobility of the series resistance and a colossal electro-resistance (CER) effect in the parallel resistance. We conclude that a modification of the Shockley equation incorporating voltage-dependent microscopic polaron parameters is required. Specifically, the voltage dependence of the reverse saturation current density is analyzed and interpreted as a voltage-dependent electron–polaron hole–polaron pair generation and separation at the interface.

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24

Dekkiche, Leila, and Rafah Naoum. "RETRACTED: IMPROVED TRANSMISSION FOR PHOTONIC CRYSTAL Y-JUNCTIONS." Progress In Electromagnetics Research 55 (2005): 79–93. http://dx.doi.org/10.2528/pier04112904.

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25

Alff, L., U. Schoop, R. Gross, R. Gerber, and A. Beck. "Ramp-edge Josephson junctions with Nd1.85Ce0.15CuO4−y barriers." Physica C: Superconductivity 271, no. 3-4 (November 1996): 339–48. http://dx.doi.org/10.1016/s0921-4534(96)00541-2.

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26

Li, Chenhui, Feng Pan, Chunyao Niu, Weiguang Chen, and Yu Jia. "Anomalous heat conduction in asymmetric graphene Y junctions." Physics Letters A 379, no. 47-48 (December 2015): 3136–40. http://dx.doi.org/10.1016/j.physleta.2015.10.021.

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27

Nakayama, A., A. Inoue, K. Takeuchi, H. Ito, and Y. Okabe. "Y-Ba-Cu-O/Nb Josephson tunnel junctions." IEEE Transactions on Magnetics 25, no. 2 (March 1989): 799–802. http://dx.doi.org/10.1109/20.92406.

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28

Li, W. Z., B. Pandey, and Y. Q. Liu. "Growth and Structure of Carbon Nanotube Y-Junctions." Journal of Physical Chemistry B 110, no. 47 (November 2006): 23694–700. http://dx.doi.org/10.1021/jp064233+.

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29

Cascio, L., T. Rozzi, and L. Zappelli. "Radiation loss of Y-junctions in rib waveguide." IEEE Transactions on Microwave Theory and Techniques 43, no. 8 (1995): 1788–97. http://dx.doi.org/10.1109/22.402261.

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30

Kleefisch, S., L. Alff, U. Schoop, A. Marx, R. Gross, M. Naito, and H. Sato. "Superconducting Nd1.85Ce0.15CuO4−y bicrystal grain boundary Josephson junctions." Applied Physics Letters 72, no. 22 (June 1998): 2888–90. http://dx.doi.org/10.1063/1.121449.

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31

van der Tol, J. J. G. M., and J. H. Laarhuis. "Measurement of mode splitting in asymmetric Y-junctions." IEEE Photonics Technology Letters 4, no. 5 (May 1992): 454–57. http://dx.doi.org/10.1109/68.136484.

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32

Kar, Ayan, Michael A. Stroscio, Mitra Dutta, and M. Meyyappan. "Electronic properties of Y-junctions in SnO2 nanowires." physica status solidi (b) 248, no. 12 (July 6, 2011): 2848–52. http://dx.doi.org/10.1002/pssb.201147233.

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33

Zhao, Cheng, Christophe Fumeaux, and Cheng-Chew Lim. "Substrate-integrated waveguide diplexers with improved Y-junctions." Microwave and Optical Technology Letters 58, no. 6 (March 28, 2016): 1384–88. http://dx.doi.org/10.1002/mop.29807.

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34

NIE, Y., Z. H. WANG, L. QIU, and J. GAO. "NONEQUILIBRIUM CHARACTERISTICS OF INTRINSIC Bi2.3Pb0.1Sr2CaCu2O8+y JOSEPHSON JUNCTIONS." International Journal of Modern Physics B 19, no. 01n03 (January 30, 2005): 235–37. http://dx.doi.org/10.1142/s021797920502830x.

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Using photolithography and Ar ion milling, we fabricate small mesas on top of the Bi 2.3 Pb 0.1 Sr 2 CaCu 2 O 8+y single crystals to study the inherent tunnelling property of intrinsic Josephson junctions. The I-V characteristics of the mesas show a typical multiple branches with large hysteresis. The return current I r depends on the N-th branch. The relation of I r and N follows I r= I 0* N m, where -1< m <0 might be related to the Coulomb blockade effect. The McCumber parameter βc of the samples is also investigated.

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35

Krijnen, G. J. M., H. J. W. M. Hoekstra, P. V. Lambeck, and T. J. M. A. Popma. "Simple analytical description of performance of Y-junctions." Electronics Letters 28, no. 22 (1992): 2072. http://dx.doi.org/10.1049/el:19921328.

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36

Steegmans, Maartje L. J., Karin G. P. H. Schroën, and Remko M. Boom. "Characterization of Emulsification at Flat Microchannel Y Junctions." Langmuir 25, no. 6 (March 17, 2009): 3396–401. http://dx.doi.org/10.1021/la8035852.

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37

Steegmans, Maartje L. J., Anja Warmerdam, Karin G. P. H. Schroën, and Remko M. Boom. "Dynamic Interfacial Tension Measurements with Microfluidic Y-Junctions." Langmuir 25, no. 17 (September 2009): 9751–58. http://dx.doi.org/10.1021/la901103r.

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38

Nunley, Hayden, Mikiko Nagashima, Kamirah Martin, Alcides Lorenzo Gonzalez, Sachihiro C. Suzuki, Declan A. Norton, Rachel O. L. Wong, Pamela A. Raymond, and David K. Lubensky. "Defect patterns on the curved surface of fish retinae suggest a mechanism of cone mosaic formation." PLOS Computational Biology 16, no. 12 (December 15, 2020): e1008437. http://dx.doi.org/10.1371/journal.pcbi.1008437.

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The outer epithelial layer of zebrafish retinae contains a crystalline array of cone photoreceptors, called the cone mosaic. As this mosaic grows by mitotic addition of new photoreceptors at the rim of the hemispheric retina, topological defects, called “Y-Junctions”, form to maintain approximately constant cell spacing. The generation of topological defects due to growth on a curved surface is a distinct feature of the cone mosaic not seen in other well-studied biological patterns like the R8 photoreceptor array in the Drosophila compound eye. Since defects can provide insight into cell-cell interactions responsible for pattern formation, here we characterize the arrangement of cones in individual Y-Junction cores as well as the spatial distribution of Y-junctions across entire retinae. We find that for individual Y-junctions, the distribution of cones near the core corresponds closely to structures observed in physical crystals. In addition, Y-Junctions are organized into lines, called grain boundaries, from the retinal center to the periphery. In physical crystals, regardless of the initial distribution of defects, defects can coalesce into grain boundaries via the mobility of individual particles. By imaging in live fish, we demonstrate that grain boundaries in the cone mosaic instead appear during initial mosaic formation, without requiring defect motion. Motivated by this observation, we show that a computational model of repulsive cell-cell interactions generates a mosaic with grain boundaries. In contrast to paradigmatic models of fate specification in mostly motionless cell packings, this finding emphasizes the role of cell motion, guided by cell-cell interactions during differentiation, in forming biological crystals. Such a route to the formation of regular patterns may be especially valuable in situations, like growth on a curved surface, where the resulting long-ranged, elastic, effective interactions between defects can help to group them into grain boundaries.

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39

Kim, Yongsam, Yunchang Seol, Ming-Chih Lai, and Charles S. Peskin. "The Immersed Boundary Method for Two-Dimensional Foam with Topological Changes." Communications in Computational Physics 12, no. 2 (August 2012): 479–93. http://dx.doi.org/10.4208/cicp.181210.080811s.

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AbstractWe extend the immersed boundary (IB) method to simulate the dynamics of a 2D dry foam by including the topological changes of the bubble network. In the article [Y. Kim, M.-C. Lai, and C. S. Peskin, J. Comput. Phys. 229:5194-5207,2010], we implemented an IB method for the foam problem in the two-dimensional case, and tested it by verifying the von Neumann relation which governs the coarsening of a two-dimensional dry foam. However, the method implemented in that article had an important limitation; we did not allow for the resolution of quadruple or higher order junctions into triple junctions. A total shrinkage of a bubble with more than four edges generates a quadruple or higher order junction. In reality, a higher order junction is unstable and resolves itself into triple junctions. We here extend the methodology previously introduced by allowing topological changes, and we illustrate the significance of such topological changes by comparing the behaviors of foams in which topological changes are allowed to those in which they are not.

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40

GAO, J., and J. L. SUN. "THE EFFECTIVE BARRIER THICKNESS IN RAMP-TYPE JUNCTIONS WITH A CONTINUALLY GRADED BARRIER OF Y1-xPrxBa2Cu3Oy." International Journal of Modern Physics B 19, no. 01n03 (January 30, 2005): 383–85. http://dx.doi.org/10.1142/s021797920502861x.

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Ramp junctions have been successfully synthesized utilizing an Y 1- x Pr x Ba 2 Cu 3 O y barrier with a continually graded concentration of Pr . The properties of these junctions are dominated by the barrier material rather than the boundary. Also, the damaged ramp surface is excluded from the weak link region so its influence is minimized. The Josephson coupling occurs at the naturally formed S/N interfaces within the Y 1- x Pr x Ba 2 Cu 3 O y layer. Thus it leads to a highly transparent S/N boundary and greatly enhances the performance of the junctions. The effective thickness of the barrier can be varied even post fabrication, depending on the measuring temperature and the concentration gradient. The temperature dependence of the barrier thickness and Josephson properties were investigated and compared with those junctions with a conventional single barrier. These unique features should motivate further studies on the nature of these junctions.

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41

Fülep, Dávid, Ibolya Zsoldos, and István László. "Self-organizing Behavior of Y-junctions of Graphene Nanoribbons." International Journal of Engineering Research and Applications 07, no. 05 (May 2017): 34–47. http://dx.doi.org/10.9790/9622-0705033447.

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42

Liu, Z., V. Srot, and J. Yang. "Crystalline Silcion Carbide Y Junctions Induced by Catalysts Coalescence." Microscopy and Microanalysis 17, S2 (July 2011): 1900–1901. http://dx.doi.org/10.1017/s1431927611010373.

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43

Wong, Wei Ru, Faisal Rafiq Mahamd Adikan, and Pierre Berini. "Long-range surface plasmon Y-junctions for referenced biosensing." Optics Express 23, no. 24 (November 20, 2015): 31098. http://dx.doi.org/10.1364/oe.23.031098.

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44

Witt, Thomas J. "Accurate Determination of2ehin Y-Ba-Cu-O Josephson Junctions." Physical Review Letters 61, no. 12 (September 19, 1988): 1423–26. http://dx.doi.org/10.1103/physrevlett.61.1423.

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45

Klotz, Matthew, Mike Crosser, Aqiang Guo, Michael Henry, Gregory J. Salamo, Mordechai Segev, and Gary L. Wood. "Fixing solitonic y junctions in photorefractive strontium–barium–niobate." Applied Physics Letters 79, no. 10 (September 3, 2001): 1423–25. http://dx.doi.org/10.1063/1.1389824.

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46

Inoue, Atsuki, Kiyoshi Takeuchi, Hiroyuki Ito, Akiyoshi Nakayama, Yoichi Okabe, Masashi Kawasaki, and Hideomi Koinuma. "Y-Ba-Cu-O/Nb Tunnel Type Josephson Junctions." Japanese Journal of Applied Physics 26, Part 2, No. 9 (September 20, 1987): L1443—L1444. http://dx.doi.org/10.1143/jjap.26.l1443.

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47

Rolland, C., D. M. Adams, D. Yevick, and B. Hermansson. "Optimization of strongly guiding semiconductor rib waveguide Y-junctions." IEEE Photonics Technology Letters 2, no. 6 (June 1990): 404–6. http://dx.doi.org/10.1109/68.56600.

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48

Nakayama, Akiyoshi, Atsuki Inoue, Kiyoshi Takeuchi, and Yoichi Okabe. "Y-Ba-Cu-O/AlOx/Nb Josephson Tunnel Junctions." Japanese Journal of Applied Physics 26, Part 2, No. 12 (December 20, 1987): L2055—L2058. http://dx.doi.org/10.1143/jjap.26.l2055.

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49

van der Tol, J. J. G. M., J. W. Pedersen, E. G. Metaal, Y. S. Oei, F. H. Green, and P. Demeester. "Sharp vertices in asymmetric Y-junctions by double masking." IEEE Photonics Technology Letters 6, no. 2 (February 1994): 249–51. http://dx.doi.org/10.1109/68.275440.

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50

Han-Bin Lin, Rei-Shin Cheng, and Way-Seen Wang. "Wide-angle low-loss single-mode symmetric Y-junctions." IEEE Photonics Technology Letters 6, no. 7 (July 1994): 825–27. http://dx.doi.org/10.1109/68.311467.

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