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Journal articles on the topic 'The higher order mode'

Author: Grafiati

Published: 30 May 2022

Last updated: 31 May 2022

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1

Le Clainche, Soledad, and José M. Vega. "Higher Order Dynamic Mode Decomposition." SIAM Journal on Applied Dynamical Systems 16, no. 2 (January 2017): 882–925. http://dx.doi.org/10.1137/15m1054924.

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2

Deguchi, Hiroyuki, Mikio Tsuji, and Hiroshi Shigesawa. "Dual-mode horn antennas suppressing higher-order modes." Electronics and Communications in Japan (Part I: Communications) 86, no. 9 (September 2003): 17–24. http://dx.doi.org/10.1002/ecja.10089.

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3

Swanson, D. G. "Higher-order terms in mode conversion." Physics of Plasmas 5, no. 7 (July 1998): 2810–12. http://dx.doi.org/10.1063/1.872969.

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4

Jacobs, Ingo, Lisa Lenz, Anna Wollny, and Antje Horsch. "The Higher-Order Structure of Schema Modes." Journal of Personality Disorders 34, no. 3 (June 2020): 348–76. http://dx.doi.org/10.1521/pedi_2018_32_401.

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In schema therapy, modes are proposed as a key concept and main target for treatment of personality disorders. The present study aimed to assess a comprehensive set of 20 modes, to explore their higher-order structure, and to link the mode factors to the generic schema factor and basic personality traits. The sample consisted of N = 533 inpatients. Earlier versions of the Schema Mode Inventory (SMI, SMI-2) were merged into the German Extended SMI (GE-SMI). Item-level confirmatory factor analyses indicated that the structure of 16 out of 20 GE-SMI scales might be unidimensional. Scale-level exploratory factor analysis revealed three hierarchically structured mode factors: internalization, externalization, and compulsivity. Regressing mode factor scores on the Big Five factors and the generic schema factor supported the validity of the mode factors. The hierarchical structure of modes will be linked to the Hierarchical Taxonomy of Psychopathology, and implications for case conceptualization and treatment will be discussed.

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5

Taleb, M., F. Plestan, and B. Bououlid. "Higher order sliding mode control based on adaptive first order sliding mode controller." IFAC Proceedings Volumes 47, no. 3 (2014): 1380–85. http://dx.doi.org/10.3182/20140824-6-za-1003.02487.

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6

Pearlmutter, Barak A., and Jeffrey Mark Siskind. "Lazy multivariate higher-order forward-mode AD." ACM SIGPLAN Notices 42, no. 1 (January 17, 2007): 155–60. http://dx.doi.org/10.1145/1190215.1190242.

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7

Sharma, Nalin Kumar, Spandan Roy, S. Janardhanan, and I. N. Kar. "Adaptive Discrete-Time Higher Order Sliding Mode." IEEE Transactions on Circuits and Systems II: Express Briefs 66, no. 4 (April 2019): 612–16. http://dx.doi.org/10.1109/tcsii.2018.2849975.

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8

Castro-Linares, R., A. Glumineau, S. Laghrouche, and F. Plestan. "Higher Order Sliding Mode Observer-Based Control." IFAC Proceedings Volumes 37, no. 21 (December 2004): 481–86. http://dx.doi.org/10.1016/s1474-6670(17)30515-3.

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9

Fuscaldo, Walter, Guido Valerio, Alessandro Galli, Ronan Sauleau, Anthony Grbic, and Mauro Ettorre. "Higher-Order Leaky-Mode Bessel-Beam Launcher." IEEE Transactions on Antennas and Propagation 64, no. 3 (March 2016): 904–13. http://dx.doi.org/10.1109/tap.2015.2513076.

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10

Edwards, Christopher, and Yuri Shtessel. "Adaptive Continuous Higher Order Sliding Mode Control." IFAC Proceedings Volumes 47, no. 3 (2014): 10826–31. http://dx.doi.org/10.3182/20140824-6-za-1003.01833.

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11

Yerolatsitis, Stephanos, and Timothy A. Birks. "Higher Order Mode Convertors for “Ribbon” Fibre." Journal of Lightwave Technology 33, no. 6 (March 15, 2015): 1182–85. http://dx.doi.org/10.1109/jlt.2014.2374991.

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12

Nguyen, K. T., J. P. Calame, B. G. Danly, B. Levush, M. Garven, and T. Antonsen. "Higher order mode excitations in gyro-amplifiers." Physics of Plasmas 8, no. 5 (May 2001): 2488–94. http://dx.doi.org/10.1063/1.1348330.

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13

Horikis, Theodoros P., and Mark J. Ablowitz. "Passive mode-locking under higher order effects." Journal of the Optical Society of America B 31, no. 11 (October 17, 2014): 2748. http://dx.doi.org/10.1364/josab.31.002748.

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14

Hirose, A., L. Zhang, and M. Elia. "Higher Order Collisionless Ballooning Mode in Tokamaks." Physical Review Letters 72, no. 25 (June 20, 1994): 3993–96. http://dx.doi.org/10.1103/physrevlett.72.3993.

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15

Minnotte, Michael C. "Mode testing via higher-order density estimation." Computational Statistics 25, no. 3 (February 11, 2010): 391–407. http://dx.doi.org/10.1007/s00180-010-0183-7.

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16

Edwards, Christopher, and Yuri B. Shtessel. "Adaptive continuous higher order sliding mode control." Automatica 65 (March 2016): 183–90. http://dx.doi.org/10.1016/j.automatica.2015.11.038.

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17

Tiwari, Pyare Mohan, S. Janardhanan, and Mashuq un Nabi. "Attitude control using higher order sliding mode." Aerospace Science and Technology 54 (July 2016): 108–13. http://dx.doi.org/10.1016/j.ast.2016.04.012.

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18

Laghrouche, Salah, Franck Plestan, and Alain Glumineau. "Higher order sliding mode control based on integral sliding mode." Automatica 43, no. 3 (March 2007): 531–37. http://dx.doi.org/10.1016/j.automatica.2006.09.017.

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19

Wazwaz, Abdul-Majid. "Two wave mode higher-order modified KdV equations." International Journal of Numerical Methods for Heat & Fluid Flow 27, no. 10 (October 2, 2017): 2223–30. http://dx.doi.org/10.1108/hff-10-2016-0413.

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Purpose The purpose of this paper is concerned with developing two-mode higher-order modified Korteweg-de Vries (KdV) equations. The study shows that multiple soliton solutions exist for essential conditions related to the nonlinearity and dispersion parameters. Design/methodology/approach The proposed technique for constructing a two-wave model, as presented in this work, has been shown to be very efficient. The employed approach formally derives the essential conditions for soliton solutions to exist. Findings The examined two-wave model features interesting results in propagation of waves and fluid flow. Research limitations/implications The paper presents a new and efficient algorithm for constructing and studying two-wave-mode higher-order modified KdV equations. Practical implications A two-wave model was constructed for higher-order modified KdV equations. The essential conditions for multiple soliton solutions to exist were derived. Social implications The work shows the distinct features of the standard equation and the newly developed equation. Originality/value The work is original and this is the first time for two-wave-mode higher-order modified KdV equations to be constructed and studied.

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20

Xi, Heng-Dong, Yi-Bao Zhang, Jian-Tao Hao, and Ke-Qing Xia. "Higher-order flow modes in turbulent Rayleigh–Bénard convection." Journal of Fluid Mechanics 805 (September 16, 2016): 31–51. http://dx.doi.org/10.1017/jfm.2016.572.

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We present experimental studies of higher-order modes of the flow in turbulent thermal convection in cells of aspect ratio ($\unicode[STIX]{x1D6E4}$) 1 and 0.5. The working fluid is water with the Prandtl number ($Pr$) kept at around 5.0. The Rayleigh number ($Ra$) ranges from $9\times 10^{8}$ to $6\times 10^{9}$ for $\unicode[STIX]{x1D6E4}=1$ and from $1.6\times 10^{10}$ to $7.2\times 10^{10}$ for $\unicode[STIX]{x1D6E4}=0.5$. We found that in $\unicode[STIX]{x1D6E4}=1$ cells, the first mode, which corresponds to the large-scale circulation (LSC), dominates the flow. The second mode (quadrupole mode), the third mode (sextupole mode) and the fourth mode (octupole mode) are very weak, on average these higher-order modes each contains less than 4 % of the total flow energy. In $\unicode[STIX]{x1D6E4}=0.5$ cells, the first mode is still the strongest but less dominant, the second mode becomes stronger which contains 13.7 % of the total flow energy and the third and the fourth modes are also stronger (containing 6.5 % and 1.1 % of the total flow energy respectively). It is found that during a reversal/cessation, the amplitude of the second mode and the remaining modes experiences a rapid increase followed by a decrease, which is opposite to the behaviour of the amplitude of the first mode – it decreases to almost zero then rebounds. In addition, it is found that during the cessation (reversal) of the LSC, the second mode dominates, containing 51.3 % (50.1 %) of the total flow energy, which reveals that the commonly called cessation event is not the cessation of the entire flow but only the cessation of the first mode (LSC). The experiment reveals that the second mode and the remaining higher-order modes play important roles in the dynamical process of the reversal/cessation of the LSC. We also show direct evidence that the first mode is more efficient for heat transfer. Furthermore, our study reveals that, during the cessation/reversal of the LSC, $Nu$ drops to its local minimum and the minimum of $Nu$ is ahead of the minimum of the amplitude of the LSC; and reversals can be distinguished from cessations in terms of global heat transport. A direct velocity measurement reveals the flow structure of the first- and higher-order modes.

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21

Pyeon, Cheol Ho, Yoshihiro Yamane, Tsuyoshi Misawa, and Seiji Shiroya. "Higher order perturbation calculation with higher mode eigenfunctions in homogeneous system." Annals of Nuclear Energy 27, no. 13 (September 2000): 1227–35. http://dx.doi.org/10.1016/s0306-4549(00)00019-0.

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22

McCleary, J., Ming-yi Li, and Kai Chang. "Slot-fed higher order mode Fabry-Perot filters." IEEE Transactions on Microwave Theory and Techniques 41, no. 10 (1993): 1703–9. http://dx.doi.org/10.1109/22.247914.

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23

Peng, Wang, Youping Chen, and Wu Ai. "Higher-order mode photonic crystal based nanofluidic sensor." Optics Communications 382 (January 2017): 105–12. http://dx.doi.org/10.1016/j.optcom.2016.07.019.

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24

Defoort, Michael, Thierry Floquet, Annemarie Kokosy, and Wilfrid Perruquetti. "A novel higher order sliding mode control scheme." Systems & Control Letters 58, no. 2 (February 2009): 102–8. http://dx.doi.org/10.1016/j.sysconle.2008.09.004.

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25

Frawley, Mary C., Alex Petcu-Colan, Viet Giang Truong, and Síle Nic Chormaic. "Higher order mode propagation in an optical nanofiber." Optics Communications 285, no. 23 (October 2012): 4648–54. http://dx.doi.org/10.1016/j.optcom.2012.05.016.

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26

Tsankov, M. A., S. I. Ganchev, and L. G. Milenova. "Higher-order mode waveguide circulators for millimeter wavelengths." IEEE Transactions on Magnetics 28, no. 5 (September 1992): 3228–30. http://dx.doi.org/10.1109/20.179767.

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27

Sugiura, Hiroyuki, Nobuyosi Kikuma, and Naoki Inagaki. "Higher order mode 3-D Corner Reflector Antenna." IEEJ Transactions on Electronics, Information and Systems 116, no. 1 (1996): 16–21. http://dx.doi.org/10.1541/ieejeiss1987.116.1_16.

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28

Hernández, Debbie, Fernando Castaños, and Leonid Fridman. "Pole-Placement in Higher-Order Sliding-Mode Control." IFAC Proceedings Volumes 47, no. 3 (2014): 1386–91. http://dx.doi.org/10.3182/20140824-6-za-1003.00949.

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29

Yan, Xing-Gang, Leonid Fridman, Sarah K. Spurgeon, and Qingling Zhang. "Decentralised Observation Using Higher Order Sliding Mode Techniques." IFAC Proceedings Volumes 47, no. 3 (2014): 4613–18. http://dx.doi.org/10.3182/20140824-6-za-1003.01809.

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30

Abdulmajid, Abdulmajid A., and Salam Khamas. "HIGHER ORDER MODE LAYERED CYLINDRICAL DIELECTRIC RESONATOR ANTENNA." Progress In Electromagnetics Research C 90 (2019): 65–77. http://dx.doi.org/10.2528/pierc18112808.

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31

Tsitsos, S., and A. A. P. Gibson. "Higher order mode suppression in strip line geometries." Microwave and Optical Technology Letters 18, no. 1 (May 1998): 1–3. http://dx.doi.org/10.1002/(sici)1098-2760(199805)18:1<1::aid-mop1>3.0.co;2-k.

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32

Dinuzzo, F., and A. Ferrara. "Higher Order Sliding Mode Controllers With Optimal Reaching." IEEE Transactions on Automatic Control 54, no. 9 (September 2009): 2126–36. http://dx.doi.org/10.1109/tac.2009.2026940.

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33

Sharma, Nalin Kumar, and Sivaramakrishnan Janardhanan. "Discrete higher order sliding mode: concept to validation." IET Control Theory & Applications 11, no. 8 (May 12, 2017): 1098–103. http://dx.doi.org/10.1049/iet-cta.2016.0993.

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34

Nicholson, J. W., J. M. Fini, A. M. DeSantolo, E. Monberg, F. DiMarcello, J. Fleming, C. Headley, D. J. DiGiovanni, S. Ghalmi, and S. Ramachandran. "A higher-order-mode Erbium-doped-fiber amplifier." Optics Express 18, no. 17 (August 2, 2010): 17651. http://dx.doi.org/10.1364/oe.18.017651.

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35

He, Yongli, Zhenxing Liu, Yachao Liu, Junxiao Zhou, Yougang Ke, Hailu Luo, and Shuangchun Wen. "Higher-order laser mode converters with dielectric metasurfaces." Optics Letters 40, no. 23 (November 19, 2015): 5506. http://dx.doi.org/10.1364/ol.40.005506.

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36

Ramachandran, S., S. Ghalmi, S. Chandrasekhar, I. Ryazansky, M. F. Yan, F. V. Dimarcello, W. A. Reed, and P. Wisk. "Tunable dispersion compensators utilizing higher order mode fibers." IEEE Photonics Technology Letters 15, no. 5 (May 2003): 727–29. http://dx.doi.org/10.1109/lpt.2003.810255.

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37

Trivedi, P. K., B. Bandyopadhyay, S. Mahata, and S. Chaudhuri. "Roll stabilization: a higher-order sliding-mode approach." IEEE Transactions on Aerospace and Electronic Systems 51, no. 3 (July 2015): 2489–96. http://dx.doi.org/10.1109/taes.2015.140057.

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38

Sakawa, Y., N. Koshikawa, and T. Shoji. "A higher-order radial mode of helicon waves." Plasma Sources Science and Technology 6, no. 1 (February 1, 1997): 96–100. http://dx.doi.org/10.1088/0963-0252/6/1/014.

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39

Yamamoto, Toshihiro. "Higher order mode analyses in Feynman-α method." Annals of Nuclear Energy 38, no. 6 (June 2011): 1231–37. http://dx.doi.org/10.1016/j.anucene.2011.02.017.

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40

Barth, Alexander, Johann Reger, and Jaime A. Moreno. "Indirect Adaptive Control for Higher Order Sliding Mode." IFAC-PapersOnLine 51, no. 13 (2018): 591–96. http://dx.doi.org/10.1016/j.ifacol.2018.07.344.

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41

Kumar, Jayendra. "Higher-order mode substrate integrated rectangular patch antenna." AEU - International Journal of Electronics and Communications 139 (September 2021): 153934. http://dx.doi.org/10.1016/j.aeue.2021.153934.

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42

Lindlein, Norbert, Gerd Leuchs, and Siddharth Ramachandran. "Achieving Gaussian outputs from large-mode-area higher-order-mode fibers." Applied Optics 46, no. 22 (July 9, 2007): 5147. http://dx.doi.org/10.1364/ao.46.005147.

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43

Lee, In Joon, and Sangin Kim. "On-Chip Guiding of Higher-Order Orbital Angular Momentum Modes." Photonics 6, no. 2 (June 23, 2019): 72. http://dx.doi.org/10.3390/photonics6020072.

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Higher-order orbital angular momentum (OAM) mode guiding in a waveguide which is suitable for on-chip integration has been investigated. Based on the relation between the Laguerre-Gaussian mode and the Hermite-Gaussian mode, it has been shown that two degenerate guided modes of π/2l-rotation symmetry can support the l-th order OAM mode. In order to mimic the rotational symmetry, we have proposed the waveguide structure of a cross-shaped core and designed a waveguide that can support OAM modes of ±1 and ±2 topological charges simultaneously at a wavelength of 1550 nm. Purity of the OAM modes guided in the designed waveguide has been assessed by numerically calculating their topological charges from the field distribution, which were close to the theoretical values. We also investigated the guiding of OAM modes of ±3 and ±4 topological charges in our proposed waveguide structure, which revealed the possibility of the separate guiding of those OAM modes with relatively lower purity.

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44

Schulze, Christian, Daniel Flamm, Sonja Unger, Siegmund Schröter, and Michael Duparré. "Measurement of higher-order mode propagation losses in effectively single mode fibers." Optics Letters 38, no. 23 (November 20, 2013): 4958. http://dx.doi.org/10.1364/ol.38.004958.

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45

Fini, John M., and Siddharth Ramachandran. "Natural bend-distortion immunity of higher-order-mode large-mode-area fibers." Optics Letters 32, no. 7 (March 5, 2007): 748. http://dx.doi.org/10.1364/ol.32.000748.

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46

Nicholson, J. W., S. Ramachandran, S. Ghalmi, M. F. Yan, P. Wisk, E. Monberg, and F. V. Dimarcello. "Propagation of femtosecond pulses in large-mode-area, higher-order-mode fiber." Optics Letters 31, no. 21 (October 11, 2006): 3191. http://dx.doi.org/10.1364/ol.31.003191.

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47

Ge, Aichen, Fanchao Meng, Yanfeng Li, Bowen Liu, and Minglie Hu. "Higher-Order Mode Suppression in Antiresonant Nodeless Hollow-Core Fibers." Micromachines 10, no. 2 (February 15, 2019): 128. http://dx.doi.org/10.3390/mi10020128.

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Negative curvature hollow-core fibers (NC-HCFs) are useful as gas sensors. We numerically analyze the single-mode performance of NC-HCFs. Both single-ring NC-HCFs and nested antiresonant fibers (NANFs) are investigated. When the size of the cladding tubes is properly designed, higher-order modes (HOMs) in the fiber core can be coupled with the cladding modes effectively and form high-loss supermodes. For the single-ring structure, we propose a novel NC-HCF with hybrid cladding tubes to enable suppression of the first two HOMs in the core simultaneously. For the nested structure, we find that cascaded coupling is necessary to maximize the loss of the HOMs in NANFs, and, as a result, NANFs with five nested tubes have an advantage in single-mode guidance performance. Moreover, a novel NANF with hybrid extended cladding tubes is proposed. In this kind of NANF, higher-order mode extinction ratios (HOMERs) of 105 and even 106 are obtained for the LP11 and LP21 modes, respectively, and a similar level of 105 for the LP02 modes. Good single-mode performance is maintained within a broad wavelength range. In addition, the loss of the LP01 modes in this kind of NANF is as low as 3.90 × 10−4 dB/m.

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48

Asthan, Rheyuniarto Sahlendar, and Achmad Munir. "Antena Ring Sirkular dengan Kemampuan Penekanan Higher Order Mode." Jurnal Nasional Teknik Elektro dan Teknologi Informasi (JNTETI) 8, no. 4 (November 20, 2019): 371. http://dx.doi.org/10.22146/jnteti.v8i4.538.

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49

Solyak, N., M. Awida, A. Hocker, T. Khabibobulline, and A. Lunin. "Higher Order Mode Coupler Heating in Continuous Wave Operation." Physics Procedia 79 (2015): 63–73. http://dx.doi.org/10.1016/j.phpro.2015.11.063.

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50

Feingold, M., C. Cetrulo, M. Peters, A. Chaudhury, S. Shmoys, and O. Geifman. "Mode of Delivery in Multiple Birth of Higher Order." Acta geneticae medicae et gemellologiae: twin research 37, no. 1 (January 1988): 105–9. http://dx.doi.org/10.1017/s0001566000004323.

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AbstractA retrospective review of triplets delivered at a Boston perinatal center from 1977 to 1986 was performed. Comparison was made between this group (study group) and previously published data on triplets in our institution (control group). Since 1977 there was a more liberal use of abdominal delivery. Cesarean sections (CS) of all triplets with malpresentation was our protocol. Of the 15 sets of triplet pregnancies in the study group, 11 were delivered by CS and 4 by vaginal delivery, vs only 1 CS in the control group wich consisted also of 15 triplets. The corrected mortality rate in the study group was lower than in the control group (2.6% vs 7.1%) but did not reach statistical significance. Apgar scores at 1 and 5 minutes were significantly higher in the study group (P < 0.002). Apgar scores for the third triplet were also higher in the study group (P < 0.05). In comparing the combined mortality and morbidity between the study group and the control group, no difference was found in the first triplet, but those of the second and third triplets were significantly lower in the study group. Of interest is the finding that the combined mortality and morbidity was not different statistically among the first, second, and third triplets in the study group, while in the control group an increase from the first to the third triplet was noted (21%, 31%, and 43%, respectively). A more liberal approach toward abdominal delivery of pregnancies of higher fetal number is advocated.

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