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Journal articles on the topic 'Gauge theories'

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Published: 4 June 2021
Last updated: 6 September 2023

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1

Wess, Julius. "Gauge Theories beyond Gauge Theories." Fortschritte der Physik 49, no. 4-6 (May 2001): 377–85. http://dx.doi.org/10.1002/1521-3978(200105)49:4/6<377::aid-prop377>3.0.co;2-2.

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2

Wess, Julius. "Gauge Theories beyond Gauge Theories." Fortschritte der Physik 49, no. 4-6 (May 2001): 377. http://dx.doi.org/10.1002/1521-3978(200105)49:4/6<377::aid-prop377>3.3.co;2-u.

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3

Reshetnyak, Alexander. "On gauge independence for gauge models with soft breaking of BRST symmetry." International Journal of Modern Physics A 29, no. 30 (December 8, 2014): 1450184. http://dx.doi.org/10.1142/s0217751x1450184x.

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A consistent quantum treatment of general gauge theories with an arbitrary gauge-fixing in the presence of soft breaking of the BRST symmetry in the field–antifield formalism is developed. It is based on a gauged (involving a field-dependent parameter) version of finite BRST transformations. The prescription allows one to restore the gauge-independence of the effective action at its extremals and therefore also that of the conventional S-matrix for a theory with BRST-breaking terms being additively introduced into a BRST-invariant action in order to achieve a consistency of the functional integral. We demonstrate the applicability of this prescription within the approach of functional renormalization group to the Yang–Mills and gravity theories. The Gribov–Zwanziger action and the refined Gribov–Zwanziger action for a many-parameter family of gauges, including the Coulomb, axial and covariant gauges, are derived perturbatively on the basis of finite gauged BRST transformations starting from Landau gauge. It is proved that gauge theories with soft breaking of BRST symmetry can be made consistent if the transformed BRST-breaking terms satisfy the same soft BRST symmetry breaking condition in the resulting gauge as the untransformed ones in the initial gauge, and also without this requirement.
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4

CLARK, T. E., C. H. LEE, and S. T. LOVE. "SUPERSYMMETRIC TENSOR GAUGE THEORIES." Modern Physics Letters A 04, no. 14 (July 20, 1989): 1343–53. http://dx.doi.org/10.1142/s0217732389001532.

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The supersymmetric extensions of anti-symmetric tensor gauge theories and their associated tensor gauge symmetry transformations are constructed. The classical equivalence between such supersymmetric tensor gauge theories and supersymmetric non-linear sigma models is established. The global symmetry of the supersymmetric tensor gauge theory is gauged and the locally invariant action is obtained. The supercurrent on the Kähler manifold is found in terms of the supersymmetric tensor gauge field.
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5

Yi, Piljin. "Index Theorems for Gauge Theories." Journal of the Korean Physical Society 73, no. 4 (August 2018): 436–48. http://dx.doi.org/10.3938/jkps.73.436.

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6

Kenyon, I. R. "Gauge theories." European Journal of Physics 7, no. 2 (April 1, 1986): 115–23. http://dx.doi.org/10.1088/0143-0807/7/2/008.

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7

Hooft, Gerard. "Gauge theories." Scholarpedia 3, no. 12 (2008): 7443. http://dx.doi.org/10.4249/scholarpedia.7443.

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8

Taubes, Clifford Henry. "Unique continuation theorems in gauge theories." Communications in Analysis and Geometry 2, no. 1 (1994): 35–52. http://dx.doi.org/10.4310/cag.1994.v2.n1.a2.

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9

Kogan, Ian I., Alex Lewis, and Oleg A. Soloviev. "Gauge Dressing of 2D Field Theories." International Journal of Modern Physics A 12, no. 13 (May 20, 1997): 2425–36. http://dx.doi.org/10.1142/s0217751x97001419.

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By using the gauge Ward identities, we study correlation functions of gauged WZNW models. We show that the gauge dressing of the correlation functions can be taken into account as a solution of the Knizhnik–Zamolodchikov equation. Our method is analogous to the analysis of the gravitational dressing of 2D field theories.
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10

Wohlgenannt, M. "Noncommutative Gauge Theories." Ukrainian Journal of Physics 57, no. 4 (April 30, 2012): 389. http://dx.doi.org/10.15407/ujpe57.4.389.

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We review two different noncommutative gauge models generalizing the approaches which lead to renormalizable scalar quantum field theories. One of them implements the crucial IR damping of the gauge field propagator in the so-called "soft breaking" part. We discuss one-loop renormalizability.
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11

Wess, Julius. "Deformed Gauge Theories." Journal of Physics: Conference Series 53 (November 1, 2006): 752–63. http://dx.doi.org/10.1088/1742-6596/53/1/049.

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12

Hasenfratz, A., and P. Hasenfratz. "Lattice Gauge Theories." Annual Review of Nuclear and Particle Science 35, no. 1 (December 1985): 559–604. http://dx.doi.org/10.1146/annurev.ns.35.120185.003015.

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13

Pokorski, Stefan, Paul H. Frampton, and Howard Georgi. "Gauge Field Theories." Physics Today 42, no. 1 (January 1989): 80–82. http://dx.doi.org/10.1063/1.2810886.

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14

Shuo-hong, Guo. "Lattice Gauge-Theories." Communications in Theoretical Physics 4, no. 5 (September 1985): 613–30. http://dx.doi.org/10.1088/0253-6102/4/5/613.

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15

Batalin, Igor, and Robert Marnelius. "Antisymplectic gauge theories." Nuclear Physics B 511, no. 1-2 (February 1998): 495–509. http://dx.doi.org/10.1016/s0550-3213(97)00663-9.

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16

Baulieu, Laurent. "Perturbative gauge theories." Physics Reports 129, no. 1 (December 1985): 1–74. http://dx.doi.org/10.1016/0370-1573(85)90091-2.

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17

Krasnikov, N. V. "Nonlocal gauge theories." Theoretical and Mathematical Physics 73, no. 2 (November 1987): 1184–90. http://dx.doi.org/10.1007/bf01017588.

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18

Teper, M. "Pure gauge theories." Nuclear Physics B - Proceedings Supplements 20 (May 1991): 159–72. http://dx.doi.org/10.1016/0920-5632(91)90901-p.

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19

LAGRAA, M. "QUANTUM GAUGE THEORIES." International Journal of Modern Physics A 11, no. 04 (February 10, 1996): 699–713. http://dx.doi.org/10.1142/s0217751x96000316.

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We consider a gauge theory by taking real quantum groups of nondegenerate bilinear form as a symmetry. The construction of this quantum gauge theory is developed in order to fit with the Hopf algebra structure. In this framework, we show that an appropriate definition of the infinitesimal gauge variations and the axioms of the Hopf algebra structure of the symmetry group lead to the closure of the infinitesimal gauge transformations without any assumption on the commutation rules of the gauge parameters, the connection and the curvature. An adequate definition of the quantum trace is given leading to the quantum Killing form. This is used to construct an invariant quantum Yang–Mills Lagrangian.
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20

ALFORD, MARK G., and JOHN MARCH-RUSSELL. "DISCRETE GAUGE THEORIES." International Journal of Modern Physics B 05, no. 16n17 (October 1991): 2641–73. http://dx.doi.org/10.1142/s021797929100105x.

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In this review we discuss the formulation and distinguishing characteristics of discrete gauge theories, and describe several important applications of the concept. For the abelian (ℤN) discrete gauge theories, we consider the construction of the discrete charge operator F(Σ*) and the associated gauge-invariant order parameter that distinguishes different Higgs phases of a spontaneously broken U(1) gauge theory. We sketch some of the important thermodynamic consequences of the resultant discrete quantum hair on black holes. We further show that, as a consequence of unbroken discrete gauge symmetries, Grand Unified cosmic strings generically exhibit a Callan-Rubakov effect. For non-abelian discrete gauge theories we discuss in some detail the charge measurement process, and in the context of a lattice formulation we construct the non-abelian generalization of F(Σ*). This enables us to build the order parameter that distinguishes the different Higgs phases of a non-abelian discrete lattice gauge theory with matter. We also describe some of the fascinating phenomena associated with non-abelian gauge vortices. For example, we argue that a loop of Alice string, or any non-abelian string, is super-conducting by virtue of charged zero modes whose charge cannot be localized anywhere on or around the string (“Cheshire charge”). Finally, we discuss the relationship between discrete gauge theories and the existence of excitations possessing exotic spin and statistics (and more generally excitations whose interactions are purely “topological”).
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21

Aldrovandi, R. "Extended gauge theories." Journal of Mathematical Physics 32, no. 9 (September 1991): 2503–12. http://dx.doi.org/10.1063/1.529144.

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22

Majumdar, Peter. "Lattice gauge theories." Scholarpedia 7, no. 4 (2012): 8615. http://dx.doi.org/10.4249/scholarpedia.8615.

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23

Aschieri, Paolo, Marija Dimitrijević, Frank Meyer, Stefan Schraml, and Julius Wess. "Twisted Gauge Theories." Letters in Mathematical Physics 78, no. 1 (September 1, 2006): 61–71. http://dx.doi.org/10.1007/s11005-006-0108-0.

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24

Becchi, Carlo M., Stefano Giusto, and Camillo Imbimbo. "Gauge dependence in topological gauge theories." Physics Letters B 393, no. 3-4 (February 1997): 342–48. http://dx.doi.org/10.1016/s0370-2693(96)01649-8.

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25

Kraus, E., and K. Sibold. "Gauge parameter dependence in gauge theories." Nuclear Physics B - Proceedings Supplements 37, no. 2 (November 1994): 120–25. http://dx.doi.org/10.1016/0920-5632(94)90667-x.

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26

Kobes, R., G. Kunstatter, and K. Mak. "Damping of fermions in hot gauge theories." Canadian Journal of Physics 71, no. 5-6 (May 1, 1993): 252–55. http://dx.doi.org/10.1139/p93-040.

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The calculation of the massless fermion damping rate to order g2T in the long-wavelength limit of hot gauge theories using the recently developed resummation methods in terms of hard thermal loops is reviewed. Ward identities between the effective propagators and vertices are used to formally prove the gauge independence of the damping rate to this order in a wide class of gauges. We also discuss some aspects of the cutoff dependence of the gauge-dependent terms proportional to the mass-shell condition.
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27

Nakkagawa, Hisao, Akira Niégawa, and Bernard Pire. "Gauge (in)dependence of the fermion damping rate in hot gauge theories." Canadian Journal of Physics 71, no. 5-6 (May 1, 1993): 269–75. http://dx.doi.org/10.1139/p93-043.

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The gauge-(in)dependence problem of the fermion damping rate in hot gauge theories is carefully examined to the effective one-loop order using a recently proposed resummation method in terms of the so-called "hard thermal loops." Explicit analysis is given in the case of a heavy fermion [Formula: see text], which enables us to investigate the essential point of the controversy in detail. Calculation in general covariant gauges shows in which calculation procedure we can get a gauge-parameter independent result. We also show, with explicit calculations, that the difference in the damping rate in the Landau and the Coulomb gauges is nonleading. Thus the leading-order damping rate is gauge independent within the Coulomb and general covariant gauges if an appropriate calculation procedure is employed.
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28

Bélusca-Maïto, Hermès, Amon Ilakovac, Paul Kühler, Marija Mađor-Božinović, Dominik Stöckinger, and Matthias Weißwange. "Introduction to Renormalization Theory and Chiral Gauge Theories in Dimensional Regularization with Non-Anticommuting γ5." Symmetry 15, no. 3 (March 1, 2023): 622. http://dx.doi.org/10.3390/sym15030622.

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This review provides a detailed introduction to chiral gauge theories, renormalization theory, and the application of dimensional regularization with the non-anticommuting BMHV scheme for γ5. One goal was to show how chiral gauge theories can be renormalized despite the spurious breaking of gauge invariance and how to obtain the required symmetry-restoring counterterms. A second goal was to familiarize the reader with the theoretical basis of the renormalization of chiral gauge theories, the theorems that guarantee the existence of renormalized chiral gauge theories at all orders as consistent quantum theories. Relevant topics include BPHZ renormalization, Slavnov–Taylor identities, the BRST formalism, and algebraic renormalization, as well as the theorems guaranteeing that dimensional regularization is a consistent regularization/renormalization scheme. All of these, including their proofs and interconnections, are explained and discussed in detail. Further, these theoretical concepts are illustrated in practical applications with the example of an Abelian and a non-Abelian chiral gauge theory. Not only the renormalization procedure for such chiral gauge theories is explained step by step, but also the results of all counterterms, including the symmetry-restoring ones, necessary for the consistent renormalization, are explicitly provided.
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29

Niemi, A. J., and G. W. Semenoff. "Gauge Algebras in Anomalous Gauge-Field Theories." Physical Review Letters 56, no. 10 (March 10, 1986): 1019–22. http://dx.doi.org/10.1103/physrevlett.56.1019.

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30

Barnich, Glenn, Marc Henneaux, Tobias Hurth, and Kostas Skenderis. "Cohomological analysis of gauge-fixed gauge theories." Physics Letters B 492, no. 3-4 (January 2000): 376–84. http://dx.doi.org/10.1016/s0370-2693(00)01087-x.

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31

SEILER, E. "Gauge Theories: Progress in Gauge Field Theory." Science 230, no. 4721 (October 4, 1985): 61–62. http://dx.doi.org/10.1126/science.230.4721.61-a.

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32

Haller, Kurt. "Gauge theories in the light-cone gauge." Physical Review D 42, no. 6 (September 15, 1990): 2095–102. http://dx.doi.org/10.1103/physrevd.42.2095.

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33

Fachin, Stefano, and Claudio Parrinello. "Global gauge fixing in lattice gauge theories." Physical Review D 44, no. 8 (October 15, 1991): 2558–64. http://dx.doi.org/10.1103/physrevd.44.2558.

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34

Modanese, G., and M. Toller. "Radial gauge in Poincaré gauge field theories." Journal of Mathematical Physics 31, no. 2 (February 1990): 452–58. http://dx.doi.org/10.1063/1.528879.

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35

KIEU, T. D. "GAUGE-INVARIANT QUANTISATION OF CHIRAL GAUGE THEORIES." Modern Physics Letters A 05, no. 03 (January 30, 1990): 175–82. http://dx.doi.org/10.1142/s0217732390000214.

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The path-integral functional of chiral gauge theories with background gauge potentials are derived in the holomorphic representation. Justification is provided, from first quantum mechanical principles, for the appearance of a functional phase factor of the gauge fields in order to maintain the gauge invariance. This term is shown to originate either from the Berry phase of the first-quantized hamiltonians or from the normal ordering of the second-quantized hamiltonian with respect to the Dirac in-vacuum. The quantization of the chiral Schwinger model is taken as an example.
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36

Wu, Yong-Shi, and A. Zee. "Abelian gauge structure inside nonabelian gauge theories." Nuclear Physics B 258 (January 1985): 157–78. http://dx.doi.org/10.1016/0550-3213(85)90607-8.

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37

Pisarski, Robert D. "Renormalized gauge propagator in hot gauge theories." Physica A: Statistical Mechanics and its Applications 158, no. 1 (May 1989): 146–57. http://dx.doi.org/10.1016/0378-4371(89)90515-3.

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38

Lima, Gabriel Di Lemos Santiago, Rafael Chaves, and Sebastião Alves Dias. "Gauge anomaly cancellation in chiral gauge theories." Annals of Physics 327, no. 6 (June 2012): 1435–49. http://dx.doi.org/10.1016/j.aop.2012.03.005.

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39

CASTELLANI, LEONARDO. "Uq(N) GAUGE THEORIES." Modern Physics Letters A 09, no. 30 (September 28, 1994): 2835–47. http://dx.doi.org/10.1142/s0217732394002689.

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Improving on an earlier proposal, we construct the gauge theories of the quantum groups U q(N). We find that these theories are also consistent with an ordinary (commuting) space-time. The bicovariance conditions of the quantum differential calculus are essential in our construction. The gauge potentials and the field strengths are q-commuting "fields," and satisfy q-commutation relations with the gauge parameters. The transformation rules of the potentials generalize the ordinary infinitesimal gauge variations. For particular deformations of U (N) ("minimal deformations"), the algebra of quantum gauge variations is shown to close, provided the gauge parameters satisfy appropriate q-commutations. The q-Lagrangian invariant under the U q(N) variations has the Yang–Mills form [Formula: see text], the "quantum metric" gij being a generalization of the Killing metric.
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40

Morozov, A. Yu. "Anomalies in gauge theories." Uspekhi Fizicheskih Nauk 150, no. 11 (1986): 337. http://dx.doi.org/10.3367/ufnr.0150.198611a.0337.

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41

Zharinov, V. V. "Algebra of gauge theories." Theoretical and Mathematical Physics 203, no. 2 (May 2020): 584–95. http://dx.doi.org/10.1134/s0040577920050025.

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42

Matsui, Kosuke, and Hiroshi Suzuki. "Anomalous gauge theories revisited." Journal of High Energy Physics 2005, no. 01 (February 1, 2005): 051. http://dx.doi.org/10.1088/1126-6708/2005/01/051.

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43

Ogilvie, Michael C. "Phases of gauge theories." Journal of Physics A: Mathematical and Theoretical 45, no. 48 (November 12, 2012): 483001. http://dx.doi.org/10.1088/1751-8113/45/48/483001.

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44

Wilczek, Frank. "Gauge theories of swimming." Physics World 2, no. 2 (February 1989): 36–40. http://dx.doi.org/10.1088/2058-7058/2/2/26.

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45

Morozov, A. Yu. "Anomalies in gauge theories." Soviet Physics Uspekhi 29, no. 11 (November 30, 1986): 993–1039. http://dx.doi.org/10.1070/pu1986v029n11abeh003537.

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46

Amariti, Antonio, Luciano Girardello, and Alberto Mariotti. "Meta-stableAnquiver gauge theories." Journal of High Energy Physics 2007, no. 10 (October 3, 2007): 017. http://dx.doi.org/10.1088/1126-6708/2007/10/017.

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47

Yi-shi, Duan. "Gauge Theories of Gravitation." Communications in Theoretical Physics 4, no. 5 (September 1985): 661–74. http://dx.doi.org/10.1088/0253-6102/4/5/661.

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48

Ooguri, Hirosi. "Gauge theories on branes." Nuclear Physics B - Proceedings Supplements 67, no. 1-3 (July 1998): 172–79. http://dx.doi.org/10.1016/s0920-5632(98)00129-7.

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49

Bonora, L., M. Schnabl, M. M. Sheikh-Jabbari, and A. Tomasiello. "Noncommutative and gauge theories." Nuclear Physics B 589, no. 1-2 (November 2000): 461–74. http://dx.doi.org/10.1016/s0550-3213(00)00527-7.

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50

Healey, Richard. "Gauge theories and holisms." Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics 35, no. 4 (December 2004): 619–42. http://dx.doi.org/10.1016/j.shpsb.2004.07.003.

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