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Journal articles on the topic 'Orbital angular momentum'

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1

Pile, David. "Orbital angular momentum." Nature Photonics 6, no. 5 (2012): 268. http://dx.doi.org/10.1038/nphoton.2012.92.

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2

Hua, Yilin, Yaodong Chen, Weijia Meng, et al. "Visualized quantum 3D orbital-angular-momentum holography." Chinese Optics Letters 22, no. 11 (2024): 110501. http://dx.doi.org/10.3788/col202422.110501.

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3

Burkardt, Matthias. "Quark Orbital Angular Momentum." EPJ Web of Conferences 85 (2015): 02009. http://dx.doi.org/10.1051/epjconf/20158502009.

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4

Padgett, Miles, Johannes Courtial, and Les Allen. "Light’s Orbital Angular Momentum." Physics Today 57, no. 5 (2004): 35–40. http://dx.doi.org/10.1063/1.1768672.

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5

Barnett, Stephen M., Mohamed Babiker, and Miles J. Padgett. "Optical orbital angular momentum." Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 375, no. 2087 (2017): 20150444. http://dx.doi.org/10.1098/rsta.2015.0444.

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We present a brief introduction to the orbital angular momentum of light, the subject of our theme issue and, in particular, to the developments in the 13 years following the founding paper by Allen et al. (Allen et al. 1992 Phys. Rev. A 45 , 8185 ( doi:10.1103/PhysRevA.45.8185 )). The papers by our invited authors serve to bring the field up to date and suggest where developments may take us next. This article is part of the themed issue ‘Optical orbital angular momentum’.
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6

Miao, Pei, Zhifeng Zhang, Jingbo Sun, et al. "Orbital angular momentum microlaser." Science 353, no. 6298 (2016): 464–67. http://dx.doi.org/10.1126/science.aaf8533.

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7

Burkardt, Matthias. "Quark Orbital Angular Momentum." Few-Body Systems 57, no. 6 (2016): 385–89. http://dx.doi.org/10.1007/s00601-016-1064-6.

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8

Momeni-Feili, Maryam, Firooz Arash, Fatemeh Taghavi-Shahri, and Abolfazl Shahveh. "Contribution of orbital angular momentum to the nucleon spin." International Journal of Modern Physics A 32, no. 06n07 (2017): 1750036. http://dx.doi.org/10.1142/s0217751x17500361.

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We have calculated the orbital angular momentum of quarks and gluons in the nucleon. The calculations are carried out in the next to leading order utilizing the so-called valon model. It is found that the average quark orbital angular momentum is positive, but small, and the average gluon orbital angular momentum is negative and large. We also report on some regularities about the total angular momentum of the quarks and the gluon, as well as on the orbital angular momentum of the separate partons. We have also provided partonic angular momentum, [Formula: see text] as a function of [Formula:
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9

Chen, Dong-Xu, Pei Zhang, Rui-Feng Liu, Hong-Rong Li, Hong Gao, and Fu-Li Li. "Orbital angular momentum filter of photon based on spin-orbital angular momentum coupling." Physics Letters A 379, no. 39 (2015): 2530–34. http://dx.doi.org/10.1016/j.physleta.2015.06.022.

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10

Spektor, Grisha, Eva Prinz, Michael Hartelt, Anna-Katharina Mahro, Martin Aeschlimann, and Meir Orenstein. "Orbital angular momentum multiplication in plasmonic vortex cavities." Science Advances 7, no. 33 (2021): eabg5571. http://dx.doi.org/10.1126/sciadv.abg5571.

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Orbital angular momentum of light is a core feature in photonics. Its confinement to surfaces using plasmonics has unlocked many phenomena and potential applications. Here, we introduce the reflection from structural boundaries as a new degree of freedom to generate and control plasmonic orbital angular momentum. We experimentally demonstrate plasmonic vortex cavities, generating a succession of vortex pulses with increasing topological charge as a function of time. We track the spatiotemporal dynamics of these angularly decelerating plasmon pulse train within the cavities for over 300 femtose
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11

Yang, Ye, Chengyuan Wang, Yun Chen, et al. "Quantum erasure based on orbital angular momentum of photons." Chinese Optics Letters 23, no. 3 (2025): 032701. https://doi.org/10.3788/col202523.032701.

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12

Kotlyar, Victor V., Sergey S. Stafeev, Vladislav D. Zaitsev, Alexey M. Telegin, and Elena S. Kozlova. "Spin–Orbital Transformation in a Tight Focus of an Optical Vortex with Circular Polarization." Applied Sciences 13, no. 14 (2023): 8361. http://dx.doi.org/10.3390/app13148361.

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In the framework of the Richards–Wolf formalism, the spin–orbit conversion upon tight focusing of an optical vortex with circular polarization is studied. We obtain exact formulas which show what part of the total (averaged over the beam cross-section) longitudinal spin angular momentum is transferred to the total longitudinal orbital angular momentum in the focus. It is shown that the maximum part of the total longitudinal angular momentum that can be transformed into the total longitudinal orbital angular momentum is equal to half the beam power, and this maximum is reached at the maximum nu
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13

Kim, Junyeon, and Yoshichika Otani. "Orbital angular momentum for spintronics." Journal of Magnetism and Magnetic Materials 563 (December 2022): 169974. http://dx.doi.org/10.1016/j.jmmm.2022.169974.

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14

Mendonca, J. T., S. Ali, and B. Thidé. "Plasmons with orbital angular momentum." Physics of Plasmas 16, no. 11 (2009): 112103. http://dx.doi.org/10.1063/1.3261802.

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15

Ayub, M. K., S. Ali, and J. T. Mendonca. "Phonons with orbital angular momentum." Physics of Plasmas 18, no. 10 (2011): 102117. http://dx.doi.org/10.1063/1.3655429.

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16

Bouchard, Frédéric, Harjaspreet Mand, Mohammad Mirhosseini, Ebrahim Karimi, and Robert W. Boyd. "Achromatic orbital angular momentum generator." New Journal of Physics 16, no. 12 (2014): 123006. http://dx.doi.org/10.1088/1367-2630/16/12/123006.

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17

Clark, Charles W., Roman Barankov, Michael G. Huber, Muhammad Arif, David G. Cory, and Dmitry A. Pushin. "Controlling neutron orbital angular momentum." Nature 525, no. 7570 (2015): 504–6. http://dx.doi.org/10.1038/nature15265.

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18

Liboff, R. L. "Spin and orbital angular momentum." Europhysics Letters (EPL) 68, no. 4 (2004): 577–81. http://dx.doi.org/10.1209/epl/i2004-10231-5.

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19

Kotlyar, V. V., A. A. Kovalev, and A. P. Porfirev. "Measurement of the orbital angular momentum of an astigmatic Hermite–Gaussian beam." Computer Optics 43, no. 3 (2019): 356–67. http://dx.doi.org/10.18287/2412-6179-2019-43-3-356-367.

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Here we study three different types of astigmatic Gaussian beams, whose complex amplitude in the Fresnel diffraction zone is described by the complex argument Hermite polynomial of the order (n, 0). The first type is a circularly symmetric Gaussian optical vortex with and a topological charge n after passing through a cylindrical lens. On propagation, the optical vortex "splits" into n first-order optical vortices. Its orbital angular momentum per photon is equal to n. The second type is an elliptical Gaussian optical vortex with a topological charge n after passing through a cylindrical lens.
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20

Zahidy, Mujtaba, Yaoxin Liu, Daniele Cozzolino, et al. "Photonic integrated chip enabling orbital angular momentum multiplexing for quantum communication." Nanophotonics 11, no. 4 (2021): 821–27. http://dx.doi.org/10.1515/nanoph-2021-0500.

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Abstract Light carrying orbital angular momentum constitutes an important resource for both classical and quantum information technologies. Its inherently unbounded nature can be exploited to generate high-dimensional quantum states or for channel multiplexing in classical and quantum communication in order to significantly boost the data capacity and the secret key rate, respectively. While the big potentials of light owning orbital angular momentum have been widely ascertained, its technological deployment is still limited by the difficulties deriving from the fabrication of integrated and s
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21

Qin, Huawang, and Raylin Tso. "High-capacity quantum secret sharing based on orbital angular momentum." Quantum Information and Computation 18, no. 7&8 (2018): 579–91. http://dx.doi.org/10.26421/qic18.7-8-3.

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A high-capacity quantum secret sharing scheme based on orbital angular momentum is proposed. The dealer uses single particles in the orbital angular momentum (OAM) basis to bring the secret and encodes the secret through performing the transformation between the orbital angular momentum (OAM) basis and the angular position (ANG) basis. In the recovery, the participants perform the single-particle measurements to reconstruct the secret. The proposed scheme can use the multi-dimension of OAM to reach higher information capacity and enhanced security.
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22

Alagashev, Grigory, Sergey Stafeev, Victor Kotlyar, and Andrey Pryamikov. "Angular Momentum of Leaky Modes in Hollow-Core Fibers." Fibers 10, no. 10 (2022): 92. http://dx.doi.org/10.3390/fib10100092.

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It is known that angular momentum (AM) is an important characteristic of light, which can be separated into the spin (SAM) and orbital parts (OAM). The dynamical properties of the spin and orbital angular momentums are determined by the polarization and spatial degrees of freedom of light. In addition to optical vortex beams possessing spatial polarization and phase singularities, optical fibers can be used to generate and propagate optical modes with the orbital and spin parts of the angular momentum. In this paper, using the example of hollow-core fibers, we demonstrate the fact that their l
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23

Boeyens, Jan C. A. "Angular Momentum in Chemistry." Zeitschrift für Naturforschung B 62, no. 3 (2007): 373–85. http://dx.doi.org/10.1515/znb-2007-0311.

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Noting that current chemical theory is based almost exclusively on electronic energy and spin variables the equal importance of orbital angular momentum is explored in this paper. From its classical definition the angular momentum of electrons in an atom is shown to obey Laplace’s equation, which automatically leads to discrete values in terms of spherical harmonics. This analysis assumes a continuous distribution of electronic charge, which resembles a fluid at equilibrium. It serves to elucidate the success and failure of Bohr’s conjecture and the origin of wave-particle duality. Applied to
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24

Schimmoller, Alex, Spencer Walker, and Alexandra S. Landsman. "Photonic Angular Momentum in Intense Light–Matter Interactions." Photonics 11, no. 9 (2024): 871. http://dx.doi.org/10.3390/photonics11090871.

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Light contains both spin and orbital angular momentum. Despite contributing equally to the total photonic angular momentum, these components derive from quite different parts of the electromagnetic field profile, namely its polarization and spatial variation, respectively, and therefore do not always share equal influence in light–matter interactions. With the growing interest in utilizing light’s orbital angular momentum to practice added control in the study of atomic systems, it becomes increasingly important for students and researchers to understand the subtlety involved in these interact
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25

Hu, Anguang, and Brett I. Dunlap. "Three-center molecular integrals and derivatives using solid harmonic Gaussian orbital and Kohn–Sham potential basis sets." Canadian Journal of Chemistry 91, no. 9 (2013): 907–15. http://dx.doi.org/10.1139/cjc-2012-0485.

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Three-center integrals over Gaussian orbital and Kohn–Sham (KS) basis sets are reviewed. An orbital basis function carries angular momentum about its atomic center. That angular momentum is created by solid harmonic differentiation with respect to the center of an s-type basis function. That differentiation can be brought outside any purely s-type integral, even nonlocal pseudopotential integrals. Thus the angular factors associated with angular momentum and differentiation with respect to atom position can be pulled outside loops over orbital and KS Gaussian exponents.
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26

Li, Jie, Guocui Wang, Chenglong Zheng, et al. "All-silicon metasurfaces for polarization multiplexed generation of terahertz photonic orbital angular momentum superposition states." Journal of Materials Chemistry C 9, no. 16 (2021): 5478–85. http://dx.doi.org/10.1039/d1tc00594d.

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The superposition state of photonic orbital angular momentum (OAM) has more degrees of freedom than pure photonic orbital angular momentum, with rich physical implications and engineering application possibilities.
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27

Yue, Yang, Hao Huang, Yongxiong Ren, Zhongqi Pan, and Alan E. Willner. "Special Issue on Novel Insights into Orbital Angular Momentum Beams: From Fundamentals, Devices to Applications." Applied Sciences 9, no. 13 (2019): 2600. http://dx.doi.org/10.3390/app9132600.

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28

KIM, Teun-Teun. "Spin-Orbital Angular Momentum of Light and Its Application." Physics and High Technology 29, no. 10 (2020): 28–31. http://dx.doi.org/10.3938/phit.29.037.

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Like the eletron, the photon carries spin and orbital angular momentum caused by the polarization and the spatial phase distribution of light, respectively. Since the first observation of an optical vortex beam with orbital angular momentum (OAM), the use of an optical vortex beam has led to further studies on the light-matter interaction, the quantum nature of light, and a number of applications. In this article, using a metasurface with geometrical phase, we introduce the fundamental origins and some important applications of light with spin-orbit angular momentum as examples, including opti
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29

BURKARDT, MATTHIAS. "QUARK ORBITAL ANGULAR MOMENTUM AND FINAL STATE INTERACTIONS." International Journal of Modern Physics: Conference Series 25 (January 2014): 1460029. http://dx.doi.org/10.1142/s2010194514600295.

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Definitions of orbital angular momentum based on Wigner distributions are used to discuss the connection between the Ji definition of the quark orbital angular momentum and that of Jaffe and Manohar. The difference between these two definitions can be interpreted as the change in the quark orbital angular momentum as it leaves the target in a DIS experiment. The mechanism responsible for that change is similar to the mechanism that causes transverse single-spin asymmetries in semi-inclusive deep-inelastic scattering.
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30

Burkardt, Matthias. "Quark Orbital Angular Momentum and Final State Interactions." International Journal of Modern Physics: Conference Series 37 (January 2015): 1560035. http://dx.doi.org/10.1142/s2010194515600356.

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Definitions of orbital angular momentum based on Wigner distributions are used to discuss the connection between the Ji definition of the quark orbital angular momentum and that of Jaffe and Manohar. The difference between these two definitions can be interpreted as the change in the quark orbital angular momentum as it leaves the target in a DIS experiment. The mechanism responsible for that change is similar to the mechanism that causes transverse single-spin asymmetries in semi-inclusive deep-inelastic scattering.
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31

Ji, Xiangdong, and Yong Zhao. "The Spin Structure of the Nucleon." International Journal of Modern Physics: Conference Series 40 (January 2016): 1660001. http://dx.doi.org/10.1142/s2010194516600016.

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We justify the physical meaning of the spin and orbital angular momentum of free partons in the infinite momentum frame, and discuss the relationship between the Jaffe-Manohar and Ji’s sum rules for proton spin. The parton orbital angular momentum in the Jaffe-Manohar sum rule can be measured through twist-three GPD’s in hard scattering processes such as deeply virtual Compton scattering. Furthermore, we propose that the paton orbital angular momentum as well as the gluon helicity can be calculated in lattice QCD through a large momentum effective theory approach, and provide all the one-loop
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32

Franke-Arnold, Sonja. "Optical angular momentum and atoms." Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 375, no. 2087 (2017): 20150435. http://dx.doi.org/10.1098/rsta.2015.0435.

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Any coherent interaction of light and atoms needs to conserve energy, linear momentum and angular momentum. What happens to an atom’s angular momentum if it encounters light that carries orbital angular momentum (OAM)? This is a particularly intriguing question as the angular momentum of atoms is quantized, incorporating the intrinsic spin angular momentum of the individual electrons as well as the OAM associated with their spatial distribution. In addition, a mechanical angular momentum can arise from the rotation of the entire atom, which for very cold atoms is also quantized. Atoms therefor
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33

Bai, Yihua, Haoran Lv, Xin Fu, and Yuanjie Yang. "Vortex beam: generation and detection of orbital angular momentum [Invited]." Chinese Optics Letters 20, no. 1 (2022): 012601. http://dx.doi.org/10.3788/col202220.012601.

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34

Volostnikov, V. G. "Orbital angular momentum of the spiral beams." Computer Optics 43, no. 3 (2019): 504–6. http://dx.doi.org/10.18287/2412-6179-2019-43-3-504-506.

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At first sight, any rotation generates some angular momentum (it is true for a solid body). But these characteristics (rotation and orbital angular momentum) are rather different for optics and mechanics. In optics there are the situation when the rotation is important. On the other hand, there are the cases where the nonzero orbital angular momentum is necessary. The main goal of this article is to investigate a relationship between a rotation under propagation of spiral beam and its angular momentum. It can be done the following conclusion: there is no any relation between rotation under pro
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35

Allen, L. "Orbital angular momentum: a personal memoir." Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 375, no. 2087 (2017): 20160280. http://dx.doi.org/10.1098/rsta.2016.0280.

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A definitive statement of the model used to describe orbital angular momentum is essentially now available. Its early history, and the interaction of those who played key roles in its development over 20 years ago in its development, is outlined in this Memoir. This article is part of the themed issue ‘Optical orbital angular momentum’.
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36

Magaña-Loaiza, Omar S., Mohammad Mirhosseini, Robert M. Cross, Seyed Mohammad Hashemi Rafsanjani, and Robert W. Boyd. "Hanbury Brown and Twiss interferometry with twisted light." Science Advances 2, no. 4 (2016): e1501143. http://dx.doi.org/10.1126/sciadv.1501143.

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The rich physics exhibited by random optical wave fields permitted Hanbury Brown and Twiss to unveil fundamental aspects of light. Furthermore, it has been recognized that optical vortices are ubiquitous in random light and that the phase distribution around these optical singularities imprints a spectrum of orbital angular momentum onto a light field. We demonstrate that random fluctuations of intensity give rise to the formation of correlations in the orbital angular momentum components and angular positions of pseudothermal light. The presence of these correlations is manifested through dis
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37

Liuti, Simonetta, Aurore Courtoy, Gary R. Goldstein, J. Osvaldo Gonzalez Hernandez, and Abha Rajan. "Observables for Quarks and Gluons Orbital Angular Momentum Distributions." International Journal of Modern Physics: Conference Series 37 (January 2015): 1560039. http://dx.doi.org/10.1142/s2010194515600393.

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We discuss the observables that have been recently put forth to describe quarks and gluons orbital angular momentum distributions. Starting from a standard parameterization of the energy momentum tensor in QCD one can single out two forms of angular momentum, a so-called kinetic term – Ji decomposition – or a canonical term – Jaffe-Manohar decomposition. Orbital angular momentum has been connected in each decomposition to a different observable, a Generalized Transverse Momentum Distribution (GTMD), for the canonical term, and a twist three Generalized Parton Distribution (GPD) for the kinetic
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38

SONG, XIAOTONG. "QUARK ORBITAL ANGULAR MOMENTUM IN THE BARYON." International Journal of Modern Physics A 16, no. 22 (2001): 3673–97. http://dx.doi.org/10.1142/s0217751x01005018.

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Analytical and numerical results, for the orbital and spin content carried by different quark flavors in the baryons, are given in the chiral quark model with symmetry breaking. The reduction of the quark spin, due to the spin dilution in the chiral splitting processes, is transferred into the orbital motion of quarks and antiquarks. The orbital angular momentum for each quark flavor in the proton as a function of the partition factor κ and the chiral splitting probability a is shown. The cancellation between the spin and orbital contributions in the spin sum rule and in the baryon magnetic mo
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39

Kovalev, A. A., and V. V. Kotlyar. "Pearcey beams carrying orbital angular momentum." Computer Optics 39, no. 4 (2015): 453–58. http://dx.doi.org/10.18287/0134-2452-2015-39-4-453-458.

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40

SAITOH, Koh, and Masaya UCHIDA. "Electron Beam Carrying Orbital Angular Momentum." Nihon Kessho Gakkaishi 58, no. 2 (2016): 79–84. http://dx.doi.org/10.5940/jcrsj.58.79.

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41

Cappelletti, Ronald L., and John Vinson. "Photons, Orbital Angular Momentum, and Neutrons." physica status solidi (b) 258, no. 9 (2021): 2170045. http://dx.doi.org/10.1002/pssb.202170045.

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42

ZHANG, Chao, and Lu MA. "Trellis Coded Orbital Angular Momentum Modulation." IEICE Transactions on Fundamentals of Electronics, Communications and Computer Sciences E99.A, no. 8 (2016): 1618–21. http://dx.doi.org/10.1587/transfun.e99.a.1618.

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43

Cheng, Wenchi, Wei Zhang, Haiyue Jing, Shanghua Gao, and Hailin Zhang. "Orbital Angular Momentum for Wireless Communications." IEEE Wireless Communications 26, no. 1 (2019): 100–107. http://dx.doi.org/10.1109/mwc.2017.1700370.

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44

Oesch, Denis W., and Darryl J. Sanchez. "Photonic orbital angular momentum in starlight." Astronomy & Astrophysics 567 (July 2014): A114. http://dx.doi.org/10.1051/0004-6361/201323140.

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45

Basar, Ertugrul. "Orbital Angular Momentum With Index Modulation." IEEE Transactions on Wireless Communications 17, no. 3 (2018): 2029–37. http://dx.doi.org/10.1109/twc.2017.2787992.

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46

Ritsch-Marte, Monika. "Orbital angular momentum light in microscopy." Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 375, no. 2087 (2017): 20150437. http://dx.doi.org/10.1098/rsta.2015.0437.

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Light with a helical phase has had an impact on optical imaging, pushing the limits of resolution or sensitivity. Here, special emphasis will be given to classical light microscopy of phase samples and to Fourier filtering techniques with a helical phase profile, such as the spiral phase contrast technique in its many variants and areas of application. This article is part of the themed issue ‘Optical orbital angular momentum’.
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47

Bialynicki-Birula, Iwo, and Zofia Bialynicka-Birula. "Gravitational waves carrying orbital angular momentum." New Journal of Physics 18, no. 2 (2016): 023022. http://dx.doi.org/10.1088/1367-2630/18/2/023022.

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48

Zhang, Xiaofan, and Xiaomeng Ma. "Photoelectron momentum distributions with twisted attosecond X waves carrying orbital angular momentum." Frontiers in Physics 10 (January 9, 2023). http://dx.doi.org/10.3389/fphy.2022.1103142.

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We theoretically investigate the photoelectron momentum distributions of 1s and 2px,y states of hydrogen by twisted attosecond X waves carrying orbital angular momentum based on first-order perturbation theory. The photoionization spectra as a function of photoelectron energy and emission angle are analyzed respectively. The results indicate that there are interference fringes in the energy spectra and more nodes in the angular distributions. These angular nodes are attributed to both orbital structure and the temporal-spatial structure of X waves. We derive an equation that can quantitatively
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49

Jia Yi-Cheng, Zhang Fu-Rong, Zhang Jing-Feng, Kong Ling-Jun, and Zhang Xiang-Dong. "Three-dimensional spatial orbital angular momentum holography." Acta Physica Sinica, 2024, 0. http://dx.doi.org/10.7498/aps.73.20231822.

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The degree of freedom of orbital angular momentum of light has been used as a new information carrier in optical holographic information processing technology. However, current research on orbital angular momentum holography mainly focuses on two-dimensional orbital angular momentum holography, where the reconstructed two-dimensional holographic image is located in a certain plane in three-dimensional space. How to further implement three-dimensional spatial orbital angular momentum holographic technology and use it to increase the information capacity of holographic communication is still a b
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50

Zhang Zhuo, Zhang Jing-Feng, and Kong Ling-Jun. "Orbital angular momentum splitter of light based on beam displacer." Acta Physica Sinica, 2024, 0. http://dx.doi.org/10.7498/aps.73.20231874.

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In recent years, the high dimensional properties of the orbital angular momentum degree of freedom of light have attracted extensive attention. This degree of freedom has been studied and applied in many scientific fields, especially in optical communication and quantum information. In order to give full play to the high dimensional characteristics of orbital angular momentum, it is a basic requirement to separate different orbital angular momentum states without destruction. However, the existing orbital angular momentum beam-splitting systems either lack in stability and cascade expansibilit
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