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Journal articles on the topic 'Orbital angular momentum'

Author: Grafiati
Published: 4 June 2021
Last updated: 29 July 2024

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1

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

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2

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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3

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

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4

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 (February 28, 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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5

Miao, Pei, Zhifeng Zhang, Jingbo Sun, Wiktor Walasik, Stefano Longhi, Natalia M. Litchinitser, and Liang Feng. "Orbital angular momentum microlaser." Science 353, no. 6298 (July 28, 2016): 464–67. http://dx.doi.org/10.1126/science.aaf8533.

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6

Burkardt, Matthias. "Quark Orbital Angular Momentum." Few-Body Systems 57, no. 6 (March 10, 2016): 385–89. http://dx.doi.org/10.1007/s00601-016-1064-6.

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7

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 (March 8, 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: see text].
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8

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 (October 2015): 2530–34. http://dx.doi.org/10.1016/j.physleta.2015.06.022.

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9

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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10

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

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11

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

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12

Bouchard, Frédéric, Harjaspreet Mand, Mohammad Mirhosseini, Ebrahim Karimi, and Robert W. Boyd. "Achromatic orbital angular momentum generator." New Journal of Physics 16, no. 12 (December 2, 2014): 123006. http://dx.doi.org/10.1088/1367-2630/16/12/123006.

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13

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 (September 2015): 504–6. http://dx.doi.org/10.1038/nature15265.

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14

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

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15

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 (August 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 femtoseconds using time-resolved photoemission electron microscopy, showing that the angular momentum grows by multiples of the chiral order of the cavity. The introduction of this degree of freedom to tame orbital angular momentum delivered by plasmonic vortices could miniaturize pump probe–like quantum initialization schemes, increase the torque exerted by plasmonic tweezers, and potentially achieve vortex lattice cavities with dynamically evolving topology.
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16

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 (July 19, 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 numerical aperture equal to one. We prove that the part of the spin angular momentum that transforms into the orbital angular momentum does not depend on the optical vortex topological charge. It is also shown that by virtue of spin–orbital conversion upon focusing, the total longitudinal energy flux decreases and partially transforms into the whole transversal (azimuthal) energy flow in the focus. Moreover, the longitudinal energy flux decreases by exactly the same amount that the total longitudinal spin angular momentum decreases.
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17

Boeyens, Jan C. A. "Angular Momentum in Chemistry." Zeitschrift für Naturforschung B 62, no. 3 (March 1, 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 atoms, minimization of orbital angular momentum leads to Hund’s rules. The orientation of angular momenta in lower-symmetry molecular environments follows from the well-known Jahn-Teller theorem.
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18

Alagashev, Grigory, Sergey Stafeev, Victor Kotlyar, and Andrey Pryamikov. "Angular Momentum of Leaky Modes in Hollow-Core Fibers." Fibers 10, no. 10 (October 21, 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 leaky air core modes also have an orbital part of AM in the case of circular polarization arising from the spin–orbit interaction of the air core modes. The reason for the appearance of AM is the leakage of the air core mode energy.
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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 (June 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. With a special choice of the ellipticity degree (1: 3), such a beam retains its structure upon propagation and the degenerate intensity null on the optical axis does not “split” into n optical vortices. Such a beam has fractional orbital angular momentum not equal to n. The third type is the astigmatic Hermite-Gaussian beam (HG) of order (n, 0), which is generated when a HG beam passes through a cylindrical lens. The cylindrical lens brings the orbital angular momentum into the original HG beam. The orbital angular momentum of such a beam is the sum of the vortex and astigmatic components, and can reach large values (tens and hundreds of thousands per photon). Under certain conditions, the zero intensity lines of the HG beam "merge" into an n-fold degenerate intensity null on the optical axis, and the orbital angular momentum of such a beam is equal to n. Using intensity distributions of the astigmatic HG beam in foci of two cylindrical lenses, we calculate the normalized orbital angular momentum which differs only by 7 % from its theoretical orbital angular momentum value (experimental orbital angular momentum is –13,62, theoretical OAM is –14.76).
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20

Zahidy, Mujtaba, Yaoxin Liu, Daniele Cozzolino, Yunhong Ding, Toshio Morioka, Leif K. Oxenløwe, and Davide Bacco. "Photonic integrated chip enabling orbital angular momentum multiplexing for quantum communication." Nanophotonics 11, no. 4 (November 30, 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 scalable photonic devices able to generate and manipulate it. Here, we present a photonic integrated chip able to excite orbital angular momentum modes in an 800 m long ring-core fiber, allowing us to perform parallel quantum key distribution using two and three different modes simultaneously. The experiment sets the first steps towards quantum orbital angular momentum division multiplexing enabled by a compact and light-weight silicon chip, and further pushes the development of integrated scalable devices supporting orbital angular momentum modes.
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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 (June 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

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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23

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 (September 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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24

Li, Jie, Guocui Wang, Chenglong Zheng, Jitao Li, Yue Yang, Zhang Zhang, Maosheng Yang, 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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25

KIM, Teun-Teun. "Spin-Orbital Angular Momentum of Light and Its Application." Physics and High Technology 29, no. 10 (October 31, 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 optical vortex tweezer and quantum entanglement of the spin-orbital angular momentum.
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26

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 (June 27, 2019): 2600. http://dx.doi.org/10.3390/app9132600.

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27

Allen, L. "Orbital angular momentum: a personal memoir." Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 375, no. 2087 (February 28, 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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28

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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29

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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30

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 matching conditions for the proton spin content in perturbative QCD.
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31

Volostnikov, V. G. "Orbital angular momentum of the spiral beams." Computer Optics 43, no. 3 (June 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 propagation of spiral beam and its OAM.
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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 (February 28, 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 therefore allow us to probe and access the quantum properties of light’s OAM, aiding our fundamental understanding of light–matter interactions, and moreover, allowing us to construct OAM-based applications, including quantum memories, frequency converters for shaped light and OAM-based sensors. This article is part of the themed issue ‘Optical orbital angular momentum’.
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33

Kovalev, A. A., and V. V. Kotlyar. "Pearcey beams carrying orbital angular momentum." Computer Optics 39, no. 4 (October 15, 2015): 453–58. http://dx.doi.org/10.18287/0134-2452-2015-39-4-453-458.

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34

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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35

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

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36

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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37

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

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38

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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39

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

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40

Ritsch-Marte, Monika. "Orbital angular momentum light in microscopy." Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 375, no. 2087 (February 28, 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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41

Bialynicki-Birula, Iwo, and Zofia Bialynicka-Birula. "Gravitational waves carrying orbital angular momentum." New Journal of Physics 18, no. 2 (February 4, 2016): 023022. http://dx.doi.org/10.1088/1367-2630/18/2/023022.

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42

de Lange, O. L., and R. E. Raab. "Ladder operators for orbital angular momentum." American Journal of Physics 54, no. 4 (April 1986): 372–75. http://dx.doi.org/10.1119/1.14625.

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43

Picón, A., J. Mompart, J. R. Vázquez de Aldana, L. Plaja, G. F. Calvo, and L. Roso. "Photoionization with orbital angular momentum beams." Optics Express 18, no. 4 (February 5, 2010): 3660. http://dx.doi.org/10.1364/oe.18.003660.

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44

Noyan, Mehmet A., and James M. Kikkawa. "Time-resolved orbital angular momentum spectroscopy." Applied Physics Letters 107, no. 3 (July 20, 2015): 032406. http://dx.doi.org/10.1063/1.4927321.

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45

Harwit, Martin. "Photon Orbital Angular Momentum in Astrophysics." Astrophysical Journal 597, no. 2 (November 10, 2003): 1266–70. http://dx.doi.org/10.1086/378623.

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46

Lorcé, Cédric. "Wilson lines and orbital angular momentum." Physics Letters B 719, no. 1-3 (February 2013): 185–90. http://dx.doi.org/10.1016/j.physletb.2013.01.007.

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47

de Lange, O. L., and R. E. Raab. "Ladder operators for orbital angular momentum." American Journal of Physics 55, no. 10 (October 1987): 950–51. http://dx.doi.org/10.1119/1.14914.

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48

McMorran, B., A. Agrawal, I. Anderson, A. Herzing, H. Lezec, J. McClelland, and J. Unguris. "Electron Beams with Orbital Angular Momentum." Microscopy and Microanalysis 17, S2 (July 2011): 1236–37. http://dx.doi.org/10.1017/s1431927611007057.

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49

Zhou, Hailong, Jianji Dong, Jian Wang, Shimao Li, Xinlun Cai, Siyuan Yu, and Xinliang Zhang. "Orbital Angular Momentum Divider of Light." IEEE Photonics Journal 9, no. 1 (February 2017): 1–8. http://dx.doi.org/10.1109/jphot.2016.2645896.

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50

Zhao, Sheng-Mei, Jian Ding, Xiao-Liang Dong, and Bao-Yu Zheng. "Ghost Imaging Using Orbital Angular Momentum." Chinese Physics Letters 28, no. 12 (December 2011): 124207. http://dx.doi.org/10.1088/0256-307x/28/12/124207.

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