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Journal articles on the topic 'Band crossing'

Author: Grafiati

Published: 2 June 2025

Last updated: 31 July 2025

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1

Li, Yang, Jihong Xia, Rabah Khenata, and Minquan Kuang. "Perfect Topological Metal CrB2: A One-Dimensional (1D) Nodal Line, a Zero-Dimensional (0D) Triply Degenerate Point, and a Large Linear Energy Range." Materials 13, no. 19 (2020): 4321. http://dx.doi.org/10.3390/ma13194321.

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Topological materials with band-crossing points exhibit interesting electronic characteristics and have special applications in electronic devices. However, to further facilitate the experimental detection of the signatures of these band crossings, topological materials with a large linear energy range around the band-crossing points need to be found, which is challenging. Here, via first-principle approaches, we report that the previously prepared P6/mmm-type CrB2 material is a topological metal with one pair of 1D band-crossing points, that is, nodal lines, in the kz= 0 plane, and one pair o

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2

Li, Hua, Ming Yue Feng, and Xiao Wang. "A Zebra-Crossing Detection Algorithm for Intelligent Vehicles." Applied Mechanics and Materials 236-237 (November 2012): 390–95. http://dx.doi.org/10.4028/www.scientific.net/amm.236-237.390.

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This paper describes a robust algorithm for detecting zebra crossings to provide information for intelligent vehicles’ autonomous navigation in urban environment. First, transform images framed by the camera to the top view by an Inverse Perspective Mapping (IPM); extract the region of interest (ROI) from IPM image by local threshold segmentation. Then, extract datum band from RIO by analysis of every region’s length, direction, as well as mutual relations between the bands; finally, extract all bands belonging to the zebra crossing. The zebra crossing’s distance and direction are easily calcu

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3

Huibin, Sun, Wan Xiongwen, Liu Yunzuo, et al. "Band-crossing frequencies of strongly populated bands in174Ta." Journal of Physics G: Nuclear and Particle Physics 20, no. 6 (1994): 991–95. http://dx.doi.org/10.1088/0954-3899/20/6/013.

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4

Lieder, Rainer M. "Band crossing in the superdeformed band of 146Gd." Nuclear Physics A 520 (December 1990): c59—c66. http://dx.doi.org/10.1016/0375-9474(90)91133-c.

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5

Li, Yang, Jihong Xia, Rabah Khenata, and Minquan Kuang. "Insight into the Topological Nodal Line Metal YB2 with Large Linear Energy Range: A First-Principles Study." Materials 13, no. 17 (2020): 3841. http://dx.doi.org/10.3390/ma13173841.

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The presence of one-dimensional (1D) nodal lines, which are formed by band crossing points along a line in the momentum space of materials, is accompanied by several interesting features. However, in order to facilitate experimental detection of the band crossing point signatures, the materials must possess a large linear energy range around the band crossing points. In this work, we focused on a topological metal, YB2, with phase stability and a P6/mmm space group, and studied the phonon dispersion, electronic structure, and topological nodal line signatures via first principles. The computed

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6

Cristancho, F., C. J. Gross, K. P. Lieb, et al. "Band crossing in 83Y revisited." Nuclear Physics A 540, no. 1-2 (1992): 307–27. http://dx.doi.org/10.1016/0375-9474(92)90206-y.

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7

KANENOBU, TAIZO. "BAND SURGERY ON KNOTS AND LINKS, II." Journal of Knot Theory and Its Ramifications 21, no. 09 (2012): 1250086. http://dx.doi.org/10.1142/s0218216512500861.

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An oriented 2-component link is called band-trivializable, if it can be unknotted by a single band surgery. We consider whether a given 2-component link is band-trivializable or not. Then we can completely determine the band-trivializability for the prime links with up to 9 crossings. We use the signature, the Jones and Q polynomials, and the Arf invariant. Since a band-trivializable link has 4-ball genus zero, we also give a table for the 4-ball genus of the prime links with up to 9 crossings. Furthermore, we give an additional answer to the problem of whether a (2n + 1)-crossing 2-bridge kno

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8

Hebbinghaus, G., K. Strähle, T. Rzaca-Urban, et al. "Superdeformed band in 146Gd. First observation of band crossing." Physics Letters B 240, no. 3-4 (1990): 311–16. http://dx.doi.org/10.1016/0370-2693(90)91104-j.

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9

Matta, A., O. M. Knio, R. G. Ghanem, et al. "Computational Study of Band-Crossing Reactions." Journal of Microelectromechanical Systems 13, no. 2 (2004): 310–22. http://dx.doi.org/10.1109/jmems.2004.825315.

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10

Astuti, Septiana Widi, Puspita Dewi, Windi Nopriyanto, Ahmad Ependi, and Ilham Satrio Utomo. "Pemodelan Data Kecelakaan pada Perlintasan Sebidang Kereta Api DAOP VII Madiun." Jurnal Manajemen Transportasi & Logistik (JMTRANSLOG) 1, no. 1 (2024): 1. http://dx.doi.org/10.54324/j.mtl.v1i1.1351.

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The study aims to find the most suitable regression model of railroad level crossings accident data to obtain factors significantly affect the number of fatalities in DAOP VII Madiun. The variables used were road width, right slope, left slope, train frequency, type of crossing, large kilometer angle of view, small kilometer angle of view, Early Warning System, road status, type of crossing gates, left and right caution sign, and rumble band markings. The study used comparing method between the results of the Poisson regression model and the Negative Binomial regression model. It is found that

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11

Nikolaev, Sergey, Dmitry Pshenay-Severin, Yuri Ivanov, and Alexander Burkov. "Effect of Deformation on Topological Properties of Cobalt Monosilicide." Crystals 11, no. 2 (2021): 143. http://dx.doi.org/10.3390/cryst11020143.

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Recently, it was shown that materials with certain crystal structures can exhibit multifold band crossings with large topological charges. CoSi is one such material that belongs to non-centrosymmetric space group P213 (#198) and posseses multifold band crossing points with a topological charge of 4. The change of crystal symmetry, e.g., by means of external stress, can lift the degeneracy and change its topological properties. In the present work, the influence of uniaxial deformation on the band structure and topological properties of CoSi is investigated on the base of ab initio calculations

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12

Luo, Y. X., J. O. Rasmussen, J. H. Hamilton, et al. "First observation of collective rotational bands in neutron-rich 142La and the study of octupole/triaxial deformations in 142,143La." International Journal of Modern Physics E 30, no. 05 (2021): 2150037. http://dx.doi.org/10.1142/s0218301321500373.

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Collective rotational bands were observed for the first time in neutron-rich odd–odd [Formula: see text]La by means of [Formula: see text]-[Formula: see text]-[Formula: see text] and [Formula: see text]-[Formula: see text]-[Formula: see text]-[Formula: see text] coincidence measurements of prompt fission [Formula: see text] rays from [Formula: see text]Cf using multi-detector array Gammasphere. Similarity between the yrast band of [Formula: see text]La and those of neighboring [Formula: see text]La, [Formula: see text]Ce was found and interpreted as quasiparticle excitations. PES calculations

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13

Bark, R. A., E. O. Lieder, R. M. Lieder, et al. "Studies of chirality in the mass 80, 100 and 190 regions." International Journal of Modern Physics E 23, no. 07 (2014): 1461001. http://dx.doi.org/10.1142/s0218301314610011.

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A brief survey of results of studies of nuclear chirality in the mass 80 and 190 region at iThemba LABS is given, before looking at the case of 106 Ag in detail. Here, the crossing of a pair of candidate chiral bands is re-interpreted as the crossing of a prolate band by an aligned four-quasiparticle band.

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14

Tazaki, S., and M. Hasegawa. "Band crossing in the odd-particle system." Physical Review C 48, no. 4 (1993): 1643–47. http://dx.doi.org/10.1103/physrevc.48.1643.

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15

Walker, P. M., K. C. Yeung, G. D. Dracoulis, et al. "Backbending in 180W: a t-band crossing." Physics Letters B 309, no. 1-2 (1993): 17–22. http://dx.doi.org/10.1016/0370-2693(93)91496-a.

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16

Buck, Dorothy, and Kai Ishihara. "Coherent band pathways between knots and links." Journal of Knot Theory and Its Ramifications 24, no. 02 (2015): 1550006. http://dx.doi.org/10.1142/s0218216515500066.

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We categorize coherent band (aka nullification) pathways between knots and 2-component links. Additionally, we characterize the minimal coherent band pathways (with intermediates) between any two knots or 2-component links with small crossing number. We demonstrate these band surgeries for knots and links with small crossing number. We apply these results to place lower bounds on the minimum number of recombinant events separating DNA configurations, restrict the recombination pathways and determine chirality and/or orientation of the resulting recombinant DNA molecules.

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17

Gao, Heng, Jörn W. F. Venderbos, Youngkuk Kim, and Andrew M. Rappe. "Topological Semimetals from First Principles." Annual Review of Materials Research 49, no. 1 (2019): 153–83. http://dx.doi.org/10.1146/annurev-matsci-070218-010049.

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We review recent theoretical progress in the understanding and prediction of novel topological semimetals. Topological semimetals define a class of gapless electronic phases exhibiting topologically stable crossings of energy bands. Different types of topological semimetals can be distinguished on the basis of the degeneracy of the band crossings, their codimension (e.g., point or line nodes), and the crystal space group symmetries on which the protection of stable band crossings relies. The dispersion near the band crossing is a further discriminating characteristic. These properties give ris

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18

Milosevic, Marko D. G., Björn A. Pålsson, Arne Nissen, Jens C. O. Nielsen, and Håkan Johansson. "Condition Monitoring of Railway Crossing Geometry via Measured and Simulated Track Responses." Sensors 22, no. 3 (2022): 1012. http://dx.doi.org/10.3390/s22031012.

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This paper presents methods for continuous condition monitoring of railway switches and crossings (S&C, turnout) via sleeper-mounted accelerometers at the crossing transition. The methods are developed from concurrently measured sleeper accelerations and scanned crossing geometries from six in situ crossing panels. These measurements combined with a multi-body simulation (MBS) model with a structural track model and implemented scanned crossing geometries are used to derive the link between the crossing geometry condition and the resulting track excitation. From this analysis, a crossing c

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19

Winter, G., J. Doring, L. Funke, et al. "Transition probabilities in the band crossing region of79Kr." Journal of Physics G: Nuclear Physics 14, no. 1 (1988): L13—L18. http://dx.doi.org/10.1088/0305-4616/14/1/003.

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20

Buck, Dorothy, Kai Ishihara, Matt Rathbun, and Koya Shimokawa. "Band surgeries and crossing changes between fibered links." Journal of the London Mathematical Society 94, no. 2 (2016): 557–82. http://dx.doi.org/10.1112/jlms/jdw049.

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21

Hader, J., S. C. Badescu, L. C. Bannow, J. V. Moloney, S. R. Johnson, and S. W. Koch. "Extended band anti-crossing model for dilute bismides." Applied Physics Letters 112, no. 6 (2018): 062103. http://dx.doi.org/10.1063/1.5009668.

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22

Sun, H., J. Döring, G. D. Johns, et al. "New band structures and an unpaired crossing in78Kr." Physical Review C 59, no. 2 (1999): 655–64. http://dx.doi.org/10.1103/physrevc.59.655.

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23

Horibata, Takatoshi, Makito Oi, and Naoki Onishi. "Band crossing studied by GCM with 3D-CHFB." Journal of Physics G: Nuclear and Particle Physics 25, no. 4 (1999): 885–88. http://dx.doi.org/10.1088/0954-3899/25/4/061.

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24

Lee, Ming-Yi, Ming-Che Chang, and Tzay-Ming Hong. "Change of Hall conductance induced by band crossing." Physical Review B 57, no. 19 (1998): 11895–98. http://dx.doi.org/10.1103/physrevb.57.11895.

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25

Rza̧ca-Urban, T., R. M. Lieder, S. Utzelmann, et al. "Double band crossing in the superdeformed nucleus 145Gd." Physics Letters B 356, no. 4 (1995): 456–61. http://dx.doi.org/10.1016/0370-2693(95)00851-b.

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26

Lin, T. H., K. K. F. Wong, N. J. Teng, and S. R. Lin. "Micromechanic analysis of fatigue band crossing grain boundary." Materials Science and Engineering: A 246, no. 1-2 (1998): 169–79. http://dx.doi.org/10.1016/s0921-5093(97)00692-8.

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27

Wang, Lu, Hongquan Zhou, Hao Shi, et al. "Ultra-Low Loss and Ultra-Compact Polarization-Insensitive SOI Multimode Waveguide Crossing Based on an Inverse Design Method." Photonics 11, no. 12 (2024): 1137. https://doi.org/10.3390/photonics11121137.

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Polarization-insensitive waveguide crossings are indispensable components of photonic integrated circuits (PICs), enabling the concurrent computing of optical signals from diverse waveguides inside the limits of a restricted spatial footprint. Leveraging mirror symmetry direct binary search, we successfully demonstrate an ultra-compact and ultra-low loss polarization-insensitive waveguide crossing that achieves insertion losses below −0.11 dB and crosstalk levels beneath −22.6 dB for transverse electric (TE) mode, as well as insertion losses below 0.05 dB and crosstalk levels beneath −24.5 dB

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28

Muhila Suba Janani, A., N. Boomadevi, and T. R. Rajasekaran. "Rotational behavior of thermally excited 56Fe, 58Fe and 60Fe isotopes." International Journal of Modern Physics E 28, no. 10 (2019): 1950088. http://dx.doi.org/10.1142/s0218301319500885.

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Thermal and rotational behaviors of neutron rich fp-shell isotopes such as [Formula: see text], [Formula: see text] and [Formula: see text] were analyzed microscopically within the framework of statistical theory of hot rotating nuclei (STHRN) for the angular momentum range (0–15)[Formula: see text] at excitation energy above 4[Formula: see text]MeV. Pair-breaking phenomenon and band-crossing phenomenon of Fe isotopes were discussed with and without the inclusion of BCS pairing. The STHRN method with BCS effect was extended to the Fe isotopes to determine the critical temperature [Formula: see

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29

Belousov, Yu, M. Karev, A. Malyutin, A. Miller, and E. Fominykh. "Lernaean knots and band surgery." St. Petersburg Mathematical Journal 33, no. 1 (2021): 23–46. http://dx.doi.org/10.1090/spmj/1687.

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The paper is devoted to a line of the knot theory related to the conjecture on the additivity of the crossing number for knots under connected sum. A series of weak versions of this conjecture are proved. Many of these versions are formulated in terms of the band surgery graph also called the H ( 2 ) H(2) -Gordian graph.

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30

Onoda, A., T. Une, and J. Terasaki. "A Step toward Large-Amplitude Description of the Ground Band around Band Crossing." Progress of Theoretical Physics 97, no. 3 (1997): 553–57. http://dx.doi.org/10.1143/ptp.97.553.

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31

Alisultanov, Z. Z., and N. A. Demirov. "Tilt and Anisotropy of the Dirac Spectrum Caused by the Overlapping of Bloch Functions." JETP Letters 117, no. 10 (2023): 776–80. http://dx.doi.org/10.1134/s002136402360115x.

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It has been shown that the overlapping of bands belonging to equivalent representation of the symmetry group is possible in systems with Dirac points appearing at the crossing of these bands. This overlapping results in the tilt and additional anisotropy of the Dirac spectrum, as well as in the renormalization of the velocity. At the same time, overlapping does not violate the general conditions of existence of the stable band crossing point. The effective Dirac Hamiltonian in the presence of band overlapping is pseudo-Hermitian and corresponds to the effective action of a massless spinor fiel

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32

Cheng, Zhengwang, Zhilong Hu, Shaojian Li, et al. "Searching for a promising topological Dirac nodal-line semimetal by angle resolved photoemission spectroscopy." New Journal of Physics 23, no. 12 (2021): 123026. http://dx.doi.org/10.1088/1367-2630/ac3d51.

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Abstract Topological semimetals, in which conduction and valence bands cross each other at either discrete points or along a closed loop with symmetry protected in the momentum space, exhibited great potential in applications of optical devices as well as heterogeneous catalysts or antiferromagnetic spintronics, especially when the crossing points/lines matches Fermi level (E F). It is intriguing to find the ‘ideal’ topological semimetal material, in which has a band structure with Dirac band-crossing located at E F without intersected by other extraneous bands. Here, by using angle resolved p

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33

Puebla, Jorge, Yunyoung Hwang, Kouta Kondou, and Yoshichika Otani. "Progress in Spinconversion and its Connection with Band Crossing." Annalen der Physik 534, no. 4 (2022): 2100398. http://dx.doi.org/10.1002/andp.202100398.

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34

Efimov, A. D., and V. M. Mikhajlov. "Boson Description of Band Crossing in Even Barium Isotopes." Bulletin of the Russian Academy of Sciences: Physics 83, no. 9 (2019): 1136–43. http://dx.doi.org/10.3103/s1062873819090053.

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35

Bark, R. A., G. D. Dracoulis, A. E. Stuchbery, et al. "Low-frequency band crossing in171Re: a deformed intruder interpretation." Journal of Physics G: Nuclear and Particle Physics 15, no. 8 (1989): L169—L175. http://dx.doi.org/10.1088/0954-3899/15/8/005.

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36

Harder, A., F. Dönau, K. P. Lieb, et al. "A new type of band crossing at large deformation." Physics Letters B 374, no. 4 (1996): 277–82. http://dx.doi.org/10.1016/0370-2693(96)00184-0.

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37

Fallon, P., C. W. Beausang, S. Clarke, et al. "Pair Excitations and a Proton Band Crossing in SuperdeformedGd150." Physical Review Letters 73, no. 6 (1994): 782–85. http://dx.doi.org/10.1103/physrevlett.73.782.

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38

Mandal, Ipsita. "Tunneling in Fermi systems with quadratic band crossing points." Annals of Physics 419 (August 2020): 168235. http://dx.doi.org/10.1016/j.aop.2020.168235.

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39

Li, Zhi, Dan-Dan Xu, Shu-Yu Ning, et al. "Predicted Weyl fermions in magnetic GdBi and GdSb." International Journal of Modern Physics B 31, no. 29 (2017): 1750217. http://dx.doi.org/10.1142/s0217979217502174.

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Motivated by the chiral anomaly steering negative longitudinal magnetoresistance in GdBiPt under external magnetic field, we studied the electronic structures of GdBi with paramagnetism, antiferromagnetism and ferromagnetism by first-principles calculations with modified Becke and Johnson local density approximation plus Hubbard [Formula: see text]. Our calculated results reveal that paramagnetic GdBi is semiconducting, while the antiferromagnetic GdBi is a topological nontrivial compensation metal. We also predict the presence of a pair of Weyl fermions in ferromagnetic GdBi and GdSb. The ban

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40

Yuan, Mingrui, Yanfeng Li, Yongchang Lu, et al. "High-performance and compact broadband terahertz plasmonic waveguide intersection." Nanophotonics 8, no. 10 (2019): 1811–19. http://dx.doi.org/10.1515/nanoph-2019-0191.

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AbstractFor terahertz (THz) integrated systems, an intersection between waveguides is inevitable and is often accompanied by considerable crosstalk and loss. Here, we propose and experimentally demonstrate a novel type of crossing with a footprint less than 0.2 × 0.2 mm2 for THz surface plasmon polariton waveguiding. With an optimized crossover structure, the measured loss of the intersection is as low as 0.89 dB/crossing, and the crosstalk is less than −19.06 dB/crossing at 0.55 THz. The proposed crossing structure is compact and has low loss and crosstalk within a broad band, which will pave

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41

Lin, Yih Bin, Rei Shin Chen, Ting Chung Yu, and Ju Feng Liu. "Simulation of Broadband Transmission Photonic Crystal Waveguide Crossing with Linear Taper." Applied Mechanics and Materials 479-480 (December 2013): 133–36. http://dx.doi.org/10.4028/www.scientific.net/amm.479-480.133.

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A novel design of photonic crystal waveguide crossing with taper structure is proposed. Simulations are performed by finite-difference time-domain method. The results show the proposed design has both high transmission and low cross talk characteristics. The transmission band and low cross talk band can be tuned to match each other by adjusting the taper structure..

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42

Ishida, H. "Spin-dependent band-gap formation for the L-gap surface state on the (22×3) reconstructed Au(111) surface." Journal of Physics: Condensed Matter 34, no. 19 (2022): 195002. http://dx.doi.org/10.1088/1361-648x/ac553a.

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Abstract We elucidate how the free-electron-like energy dispersion of the L-gap surface state on a Au(111)-(1 × 1) surface is modified by the experimentally observed uniaxial reconstruction of the topmost atomic layer. For this purpose, we perform a first-principles embedded Green’s function calculation for the ( 22 × 3 ) reconstructed semi-infinite Au(111) surface. The obtained band structure unfolded into the surface Brillouin zone of the (1 × 1) surface can be understood in terms of two spin-split parabolic bands centered at the Γ ¯ point, their umklapp-induced replicas centered at reciproc

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43

Ashley, T. "G-band position effects on meiotic synapsis and crossing over." Genetics 118, no. 2 (1988): 307–17. http://dx.doi.org/10.1093/genetics/118.2.307.

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Abstract An examination of synaptic data from a series of X-autosome translocations and crossover data from an extensive series of autosome-autosome translocations and autosomal inversions in mice has lead to the development of a hypothesis which predicts synaptic and recombinational behavior of chromosomal aberrations during meiosis. This hypothesis predicts that in heterozygotes for chromosomal rearrangements that meiotically align G-light chromatin with G-light chromatin lack of homology will be recognized. If homologous synapsis cannot proceed, synaptonemal complex formation will cease and

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44

Aly, O. M., and S. M. Abdel-Rahman. "Molecular-phenotypic analysis and efficiency of crossing on meat production in local chicken strains." Biotehnologija u stocarstvu 26, no. 3-4 (2010): 215–23. http://dx.doi.org/10.2298/bah1004215a.

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DNA was extracted from blood of developed local stains of chicken; Bandara, Gimmizah, and their crossing (Bandara x Gimmizah and Gimmizah x Bandara). RAPD-PCR technique was applied to detect genetic similarity as a band sharing (BS) among chicken hybrids and their parents using nine short oligonucleiotides primers. The genetic similarity as BS-values was calculated and ranged from 68 to 91%. Bandara male with Gimmizah female appeared positive heterosis at 8 wks of age. However, evidence from this study indicated that crossing of the developed local hens is capable of rapidly improving the body

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45

Batool, Z., K. Hild, T. J. C. Hosea, X. Lu, T. Tiedje, and S. J. Sweeney. "The electronic band structure of GaBiAs/GaAs layers: Influence of strain and band anti-crossing." Journal of Applied Physics 111, no. 11 (2012): 113108. http://dx.doi.org/10.1063/1.4728028.

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46

Ferreira, S. O., E. Abramof, P. Motisuke, et al. "Band crossing evidence in PbSnTe observed by optical transmission measurements." Brazilian Journal of Physics 29, no. 4 (1999): 771–74. http://dx.doi.org/10.1590/s0103-97331999000400033.

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47

Ishihara, Kai, and Koya Shimokawa. "Band Surgeries between Knots and Links with Small Crossing Numbers." Progress of Theoretical Physics Supplement 191 (2011): 245–55. http://dx.doi.org/10.1143/ptps.191.245.

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48

Perry, Jason K., and Jamil Tahir-Kheli. "Electronic structure ofLa1.85Sr0.15CuO4:Characterization of a Fermi-level band crossing." Physical Review B 58, no. 18 (1998): 12323–32. http://dx.doi.org/10.1103/physrevb.58.12323.

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49

Velázquez, Victor, Jorge G. Hirsch, and Yang Sun. "Band crossing and signature splitting in odd mass shell nuclei." Nuclear Physics A 686, no. 1-4 (2001): 129–40. http://dx.doi.org/10.1016/s0375-9474(00)00507-8.

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50

LIU, C., S. Y. WANG, B. QI, et al. "CONFIGURATION ASSIGNMENT OF THE POSITIVE-PARITY STRUCTURES IN 108Ag." International Journal of Modern Physics E 20, no. 11 (2011): 2351–59. http://dx.doi.org/10.1142/s0218301311020368.

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The high-spin states of 108 Ag have been studied by the in-beam γ spectroscopy with the reaction 104 Ru (7 Li ,3n)108 Ag at a beam energy of 33 MeV. The previously known positive-parity band structures have been extended up to higher spins. Their configurations are discussed based on alignments, band-crossing frequencies, and B(M1)/B(E2) ratios.

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