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1

LEIGH, ROBERT G. "MARGINAL DEFORMATIONS OF N=4 SYM AND NON-COMMUTATIVE MODULI SPACES OF VACUA." International Journal of Modern Physics A 16, supp01c (2001): 955–57. http://dx.doi.org/10.1142/s0217751x0100859x.

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We review recent work on the application of the non-commutative geometric framework to an interpretation of the moduli space of vacua of marginal deformations of N = 4 super Yang-Mills theories. At rational values of couplings, different regions of moduli space may be associated with D5-branes of various topologies, and orbifold dual descriptions exist which may be accessed by T-duality. Singularities in the moduli space are associated with topology change.
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2

Mateos, Toni. "Marginal deformations of Script N=4 SYM and Penrose limits with continuous spectrum." Journal of High Energy Physics 2005, no. 08 (2005): 026. http://dx.doi.org/10.1088/1126-6708/2005/08/026.

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3

Aharony, Ofer, and Shlomo S. Razamat. "Exactly Marginal Deformations of Script N = 4 SYM and of its Supersymmetric Orbifold Descendants." Journal of High Energy Physics 2002, no. 05 (2002): 029. http://dx.doi.org/10.1088/1126-6708/2002/05/029.

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4

Aharony, Ofer, Barak Kol, and Shimon Yankielowicz. "On exactly marginal deformations of Script N = 4 SYM and Type IIB Supergravity onAdS5×S5." Journal of High Energy Physics 2002, no. 06 (2002): 039. http://dx.doi.org/10.1088/1126-6708/2002/06/039.

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5

Kulaxizi, M., and K. Zoubos. "Marginal deformations of tree-level  = 4 SYM from twistor string theory." Fortschritte der Physik 54, no. 5-6 (2006): 423–29. http://dx.doi.org/10.1002/prop.200510299.

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6

Ünsal, Mithat. "Supersymmetric deformations of type IIB matrix model as matrix regularization of Script N = 4 SYM." Journal of High Energy Physics 2006, no. 04 (2006): 002. http://dx.doi.org/10.1088/1126-6708/2006/04/002.

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7

Vesman, A. V., and B. V. Ivanov. "Types of sea ice conditions north of Spitzbergen archipelago." Arctic and Antarctic Research 68, no. 2 (2022): 118–32. http://dx.doi.org/10.30758/0555-2648-2022-68-2-118-132.

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Sea ice is an important part of the Arctic climate system. In the recent decade, rapid changes in the sea ice conditions have been observed: sea ice extent and sea ice thickness are declining; conversely, ice drift speed and deformations are increasing [1–10]. The main aim of this paper was to describe the variability of sea ice conditions north of the Svalbard archipelago and analyze the changes occurring there. For most of the year, a stable polynya is observed north of the archipelago, which is commonly called “Whalers Bay”. The prevailing wind direction (8–9 months out of 12) is north-east
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8

Jin, Qingjun. "Emergent supersymmetry in the marginal deformations of N = 4 $$ \mathcal{N}=4 $$ SYM." Journal of High Energy Physics 2016, no. 10 (2016). http://dx.doi.org/10.1007/jhep10(2016)131.

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9

Amariti, Antonio, Massimo Bianchi, Marco Fazzi, Salvo Mancani, Fabio Riccioni, and Simone Rota. "Multi-planarizable quivers, orientifolds, and conformal dualities." Journal of High Energy Physics 2023, no. 9 (2023). http://dx.doi.org/10.1007/jhep09(2023)094.

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Abstract We study orientifold projections of families of four-dimensional $$ \mathcal{N} $$ N = 1 toric quiver gauge theories. We restrict to quivers that have the unusual property of being associated with multiple periodic planar diagrams which give rise, in general, to inequivalent models. A suitable orientifold projection relates a subfamily of the latter by conformal duality. That is, there exist exactly marginal deformations that connect the projected models. The deformations take the form of a sign flip in some of the superpotential interactions, similarly to the β-deformation of $$ \mat
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10

Arav, Igal, Jerome P. Gauntlett, Matthew M. Roberts, and Christopher Rosen. "Marginal deformations and RG flows for type IIB S-folds." Journal of High Energy Physics 2021, no. 7 (2021). http://dx.doi.org/10.1007/jhep07(2021)151.

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Abstract We construct a continuous one parameter family of AdS4× S1× S5 S-fold solutions of type IIB string theory which have nontrivial SL(2, ℤ) monodromy in the S1 direction. The solutions span a subset of a conformal manifold that contains the known $$ \mathcal{N} $$ N = 4 S-fold SCFT in d = 3, and generically preserve $$ \mathcal{N} $$ N = 2 supersymmetry. We also construct RG flows across dimensions, from AdS5× S5, dual to $$ \mathcal{N} $$ N = 4, d = 4 SYM compactified with a twisted spatial circle, to various AdS4×S1×S5 S-fold solutions, dual to d = 3 SCFTs. We construct additional flow
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11

Arav, Igal, Jerome P. Gauntlett, Yusheng Jiao, Matthew M. Roberts, and Christopher Rosen. "Superconformal monodromy defects in $$ \mathcal{N} $$=4 SYM and LS theory." Journal of High Energy Physics 2024, no. 8 (2024). http://dx.doi.org/10.1007/jhep08(2024)177.

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Abstract We study type IIB supergravity solutions that are dual to two-dimensional superconformal defects in d = 4 SCFTs which preserve $$ \mathcal{N} $$ N = (0, 2) supersymmetry. We consider solutions dual to defects in $$ \mathcal{N} $$ N = 4 SYM theory that have non-trivial monodromy for U(1)3 ⊂ SO(6) global symmetry and we also allow for the possibility of conical singularities. In addition, we consider the addition of fermionic and bosonic mass terms that have non trivial dependence on the spatial directions transverse to the defect, while preserving the superconformal symmetry of the def
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12

Arav, Igal, K. C. Matthew Cheung, Jerome P. Gauntlett, Matthew M. Roberts, and Christopher Rosen. "Spatially modulated and supersymmetric mass deformations of $$ \mathcal{N} $$ = 4 SYM." Journal of High Energy Physics 2020, no. 11 (2020). http://dx.doi.org/10.1007/jhep11(2020)156.

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Abstract We study mass deformations of $$ \mathcal{N} $$ N = 4, d = 4 SYM theory that are spatially modulated in one spatial dimension and preserve some residual supersymmetry. We focus on generalisations of $$ \mathcal{N} $$ N = 1∗ theories and show that it is also possible, for suitably chosen supersymmetric masses, to preserve d = 3 conformal symmetry associated with a co-dimension one interface. Holographic solutions can be constructed using D = 5 theories of gravity that arise from consistent truncations of SO(6) gauged supergravity and hence type IIB supergravity. For the mass deformatio
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13

Harmark, Troels, and Matthias Wilhelm. "Solving the Hagedorn temperature of AdS5/CFT4 via the Quantum Spectral Curve: chemical potentials and deformations." Journal of High Energy Physics 2022, no. 7 (2022). http://dx.doi.org/10.1007/jhep07(2022)136.

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Abstract We describe how to calculate the Hagedorn temperature of $$ \mathcal{N} $$ N = 4 SYM theory and type IIB superstring theory on AdS5 × S5 via the Quantum Spectral Curve (QSC) — providing further details on our previous letters [1] and [2]. We solve the QSC equations perturbatively at weak ‘t Hooft coupling λ up to seven-loop order and numerically at finite coupling, finding that the perturbative results can be expressed in terms of single-valued harmonic polylogarithms. Moreover, we generalize the QSC to describe the Hagedorn temperature in the presence of chemical potentials. Finally,
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14

Arav, Igal, K. C. Matthew Cheung, Jerome P. Gauntlett, Matthew M. Roberts, and Christopher Rosen. "Superconformal RG interfaces in holography." Journal of High Energy Physics 2020, no. 11 (2020). http://dx.doi.org/10.1007/jhep11(2020)168.

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Abstract We construct gravitational solutions that holographically describe two different d = 4 SCFTs joined together at a co-dimension one, planar RG interface and preserving d = 3 superconformal symmetry. The RG interface joins $$ \mathcal{N} $$ N = 4 SYM theory on one side with the $$ \mathcal{N} $$ N = 1 Leigh-Strassler SCFT on the other. We construct a family of such solutions, which in general are associated with spatially dependent mass deformations on the $$ \mathcal{N} $$ N = 4 SYM side, but there is a particular solution for which these deformations vanish. We also construct a Janus
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15

Berenstein, David, та Eric Dzienkowski. "Giant gravitons and the emergence of geometric limits in β-deformations of N = 4 $$ \mathcal{N}=4 $$ SYM". Journal of High Energy Physics 2015, № 1 (2015). http://dx.doi.org/10.1007/jhep01(2015)126.

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16

Bachas, Constantin, Ioannis Lavdas, and Bruno Le Floch. "Marginal deformations of 3d $$ \mathcal{N} $$ = 4 linear quiver theories." Journal of High Energy Physics 2019, no. 10 (2019). http://dx.doi.org/10.1007/jhep10(2019)253.

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17

Bena, Iosif, Mariana Graña, Stanislav Kuperstein, Praxitelis Ntokos, and Michela Petrini. "Fermionic and bosonic mass deformations of N $$ \mathcal{N} $$ = 4 SYM and their bulk supergravity dual." Journal of High Energy Physics 2016, no. 5 (2016). http://dx.doi.org/10.1007/jhep05(2016)149.

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18

Gromov, Nikolay, Árpád Hegedűs, Julius Julius, and Nika Sokolova. "Fast QSC solver: tool for systematic study of $$ \mathcal{N} $$ = 4 Super-Yang-Mills spectrum." Journal of High Energy Physics 2024, no. 5 (2024). http://dx.doi.org/10.1007/jhep05(2024)185.

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Abstract Integrability methods give us access to a number of observables in the planar $$ \mathcal{N} $$ N = 4 SYM. Among them, the Quantum Spectral Curve (QSC) governs the spectrum of anomalous dimensions. Low lying states were successfully studied in the past using the QSC. However, with the increased demand for a systematic study of a large number of states for various applications, there is a clear need for a fast QSC solver which can easily access a large number of excited states. Here, we fill this gap by developing a new algorithm and applied it to study all 219 states with the bare dim
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19

Buican, Matthew, and Takahiro Nishinaka. "$$ \mathcal{N} $$ = 4 SYM, Argyres-Douglas theories, and an exact graded vector space isomorphism." Journal of High Energy Physics 2022, no. 4 (2022). http://dx.doi.org/10.1007/jhep04(2022)028.

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Abstract In this first of two papers, we explain in detail the simplest example of a broader set of relations between apparently very different theories. Our example relates $$ \mathfrak{su}(2) $$ su 2 $$ \mathcal{N} $$ N = 4 super Yang-Mills (SYM) to a theory we call “(3, 2)”. This latter theory is an exactly marginal diagonal SU(2) gauging of three D3(SU(2)) Argyres-Douglas (AD) theories. We begin by observing that the Schur indices of these two theories are related by an algebraic transformation that is surprisingly reminiscent of index transformations describing spontaneous symmetry breaki
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20

de Leeuw, Marius, and Ana Lucia Retore. "Lifting integrable models and long-range interactions." SciPost Physics 15, no. 6 (2023). http://dx.doi.org/10.21468/scipostphys.15.6.241.

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In this paper we discuss a constructive approach to check whether a constant Hamiltonian is Yang-Baxter integrable. We then apply our method to long-range interactions and find the Lax operator and R-matrix of the three-loop SU(2) sector in N=4 SYM. We show that all known integrable long-range deformations of the 6-vertex models of this type can be obtained from a Lax operator and an R-matrix. Finally we discuss what happens at higher loops and highlight some general structures that these models exhibit.
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21

Chicherin, Dmitry, and Gregory P. Korchemsky. "The SAGEX review on scattering amplitudes, chapter 9: integrability of amplitudes in fishnet theories." Journal of Physics A: Mathematical and Theoretical, August 24, 2022. http://dx.doi.org/10.1088/1751-8121/ac8c72.

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Abstract We discuss the properties of scattering amplitudes in a conformal bi-scalar fishnet theory that previously appeared in the study of integrable deformations of N=4 SYM. In distinction with the latter theory, the scattering amplitudes in the conformal fishnet theory do not suffer from infrared divergences and possess enhanced symmetries. We demonstrate that for the simplest four-particle scattering the single- and double-trace partial amplitudes can be computed for arbitrary coupling in the leading color approximation. We also review the invariance of single-trace components of multi-pa
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22

Naseer, Usman, and Charles Thull. "Flavor deformations and supersymmetry enhancement in $4d$ $\mathcal{N}=2$ theories." SciPost Physics 13, no. 3 (2022). http://dx.doi.org/10.21468/scipostphys.13.3.058.

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We study \mathcal{N}=2𝒩=2 theories on four-dimensional manifolds that admit a Killing vector vv with isolated fixed points. It is possible to deform these theories by coupling position-dependent background fields to the flavor current multiplet. The partition function of the deformed theory only depends on the value of the background scalar fields at the fixed points of vv. For a single adjoint hypermultiplet, the partition function becomes independent of the supergravity as well as the flavor background if the scalars attain special values at the fixed points. For these special values, supers
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23

Zacarías, Salomon. "Marginal deformations of a class of AdS3 $$ \mathcal{N} $$ = (0, 4) holographic backgrounds." Journal of High Energy Physics 2021, no. 6 (2021). http://dx.doi.org/10.1007/jhep06(2021)017.

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Abstract We discuss marginal deformations of warped AdS3×S2 solutions preserving small $$ \mathcal{N} $$ N = (0, 4) supersymmetry in massive IIA and eleven-dimensional supergravity and obtain a whole family of new solutions. We characterise these new backgrounds by studying some observables like the quantised charges, associated Hannany-Witten brane set-ups and the holographic central charge, the latter is shown to be invariant under the deformation. The study of the preservation of supersymmetry shows that the new backgrounds support a dynamical SU(2) structure on the internal five-dimensiona
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24

Arav, Igal, K. C. Matthew Cheung, Jerome P. Gauntlett, Matthew M. Roberts, and Christopher Rosen. "A new family of AdS4 S-folds in type IIB string theory." Journal of High Energy Physics 2021, no. 5 (2021). http://dx.doi.org/10.1007/jhep05(2021)222.

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Abstract We construct infinite new classes of AdS4× S1× S5 solutions of type IIB string theory which have non-trivial SL(2, ℤ) monodromy along the S1 direction. The solutions are supersymmetric and holographically dual, generically, to $$ \mathcal{N} $$ N = 1 SCFTs in d = 3. The solutions are first constructed as AdS4× ℝ solutions in D = 5 SO(6) gauged supergravity and then uplifted to D = 10. Unlike the known AdS4× ℝ S-fold solutions, there is no continuous symmetry associated with the ℝ direction. The solutions all arise as limiting cases of Janus solutions of d = 4, $$ \mathcal{N} $$ N = 4
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25

Guarino, Adolfo, and Colin Sterckx. "Flat deformations of type IIB S-folds." Journal of High Energy Physics 2021, no. 11 (2021). http://dx.doi.org/10.1007/jhep11(2021)171.

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Abstract Type IIB S-folds of the form AdS4× S1× S5 have been shown to contain axion-like deformations parameterising flat directions in the 4D scalar potential and corresponding to marginal deformations of the dual S-fold CFT’s. In this note we present a group-theoretical characterisation of such flat deformations and provide a 5D interpretation thereof in terms of $$ \mathfrak{s}(6) $$ s 6 -valued duality twists inducing a class of Cremmer-Scherk-Schwarz flat gaugings in a reduction from 5D to 4D. In this manner we establish the existence of two flat deformations for the $$ \mathcal{N} $$ N =
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26

Bertle, Hanno, Elli Pomoni, Xinyu Zhang, and Konstantinos Zoubos. "Hidden symmetries of 4D $$ \mathcal{N} $$ = 2 gauge theories." Journal of High Energy Physics 2025, no. 2 (2025). https://doi.org/10.1007/jhep02(2025)205.

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Abstract We study the global symmetries of the ℤ 2-orbifold of $$ \mathcal{N} $$ N = 4 Super-Yang-Mills theory and its marginal deformations. The process of orbifolding to obtain an $$ \mathcal{N} $$ N = 2 theory would appear to break the SU(4) R-symmetry down to SU(2) × SU(2) × U(1). We show that the broken generators can be recovered by moving beyond the Lie algebraic setting to that of a Lie algebroid. This remains true when marginally deforming away from the orbifold point by allowing the couplings of the SU(N) × SU(N) gauge groups to vary independently. The information about the marginal
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27

Caetano, João, Shota Komatsu, and Yifan Wang. "Large charge ’t Hooft limit of $$ \mathcal{N} $$ = 4 super-Yang-Mills." Journal of High Energy Physics 2024, no. 2 (2024). http://dx.doi.org/10.1007/jhep02(2024)047.

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Abstract The planar integrability of $$ \mathcal{N} $$ N = 4 super-Yang-Mills (SYM) is the cornerstone for numerous exact observables. We show that the large charge sector of the SU(2) $$ \mathcal{N} $$ N = 4 SYM provides another interesting solvable corner which exhibits striking similarities despite being far from the planar limit. We study non-BPS operators obtained by small deformations of half-BPS operators with R-charge J in the limit J → ∞ with $$ {\lambda}_J\equiv {g}_{\textrm{YM}}^2J/2 $$ λ J ≡ g YM 2 J / 2 fixed. The dynamics in this large charge ’t Hooft limit is constrained by a ce
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28

Damia, Jeremias Aguilera, Riccardo Argurio, Francesco Benini, Sergio Benvenuti, Christian Copetti, and Luigi Tizzano. "Non-invertible symmetries along 4d RG flows." Journal of High Energy Physics 2024, no. 2 (2024). http://dx.doi.org/10.1007/jhep02(2024)084.

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Abstract We explore novel examples of RG flows preserving a non-invertible self-duality symmetry. Our main focus is on $$ \mathcal{N} $$ N = 1 quadratic superpotential deformations of 4d $$ \mathcal{N} $$ N = 4 super-Yang-Mills theory with gauge algebra $$ \mathfrak{su}(N) $$ su N . A theory that can be obtained in this way is the so-called $$ \mathcal{N} $$ N = 1* SYM where all adjoint chiral multiplets have a mass. Such IR theory exhibits a rich structure of vacua which we thoroughly examine. Our analysis elucidates the physics of spontaneous breaking of self-duality symmetry occurring in th
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29

Beratto, Emanuele, Noppadol Mekareeya, and Matteo Sacchi. "Marginal operators and supersymmetry enhancement in 3d S-fold SCFTs." Journal of High Energy Physics 2020, no. 12 (2020). http://dx.doi.org/10.1007/jhep12(2020)017.

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Abstract The study of exactly marginal deformations of superconformal field theories is a topic that has received considerable attention due to their rich properties. We investigate the $$ \mathcal{N} $$ N = 2 preserving exactly marginal operators of 3d S-fold SCFTs. Two families of such theories are considered: one is constructed by gauging the diagonal flavour symmetry of the T(U(2)) and T(U(3)) theories, and the other by gauging the diagonal flavour symmetry of the $$ {T}_{\left[2,{1}^2\right]}^{\left[2,{1}^2\right]}\left( SU(4)\right) $$ T 2 1 2 2 1 2 SU 4 theory. In both families, it is p
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30

Eden, Burkhard, Dennis le Plat, and Anne Spiering. "Higher-rank sectors in the hexagon formalism and marginal deformations." Journal of Physics A: Mathematical and Theoretical, October 8, 2024. http://dx.doi.org/10.1088/1751-8121/ad8492.

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Abstract The hexagon approach provides an integrability framework for the computation of structure constants in N = 4 super Yang-Mills theory in four dimensions. Three-point functions are cut into two hexagonal patches, on which the excitations of the long-range Bethe ansatz of the spectrum problem scatter. To this end, the Bethe states representing the operators also need to be cut into two parts. In rank-one sectors such entangled states are fairly straightforward to construct so that most applications of the method have so far been restricted to this simplest case. In this article we constr
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31

Chai, Noam, Eliezer Rabinovici, Ritam Sinha, and Michael Smolkin. "The bi-conical vector model at 1/N." Journal of High Energy Physics 2021, no. 5 (2021). http://dx.doi.org/10.1007/jhep05(2021)192.

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Abstract We study finite N aspects of the O(m) × O(N − m) vector model with quartic interactions in general 2 ≤ d ≤ 6 spacetime dimensions. This model has recently been shown [1, 2] to display the phenomenon of persistent symmetry breaking at a perturbative Wilson-Fisher-like fixed point in d = 4 − ϵ dimensions. The large rank limit of the biconical model displays a conformal manifold and a moduli space of vacua. We find a set of three double trace scalar operators that are respectively irrelevant, relevant and marginal deformations of the conformal manifold in general d. We calculate the anom
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32

Anabalón, Andrés, Horatiu Nastase, and Marcelo Oyarzo. "Supersymmetric AdS solitons and the interconnection of different vacua of $$ \mathcal{N} $$ = 4 Super Yang-Mills." Journal of High Energy Physics 2024, no. 5 (2024). http://dx.doi.org/10.1007/jhep05(2024)217.

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Abstract We find AdS soliton solutions in 5-dimensional gauged supergravity, obtained from the S5 compactification of type IIB, with a dilaton saturating the Breitenlohner-Freedman bound. The solutions depend on the value of the periodicity of an S1 cycle and the boundary values for two U(1) gauge fields, and give a scalar VEV in the dual field theory. At certain values of the gauge sources we have supersymmetric solutions, corresponding to supersymmetric flows, which are a deformation of the Coulomb Branch flow in $$ \mathcal{N} $$ N = 4 SYM. The solutions parameterize quantum phase transitio
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33

Lavdas, Ioannis, and Bruno Le Floch. "Mixed moduli in 3d $$ \mathcal{N} $$ = 4 higher-genus quivers." Journal of High Energy Physics 2023, no. 5 (2023). http://dx.doi.org/10.1007/jhep05(2023)124.

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Abstract We analyze exactly marginal deformations of 3d $$ \mathcal{N} $$ N = 4 Lagrangian gauge theories, especially mixed-branch operators with both electric and magnetic charges. These mixed-branch moduli can either belong to products of electric and magnetic current supermultiplets, or be single-trace (non-factorizable). Apart from some exceptional quivers that have additional moduli, 3d $$ \mathcal{N} $$ N = 4 theories described by genus g quivers with nonabelian unitary gauge groups have exactly g single-trace mixed moduli, which preserve the global flavour symmetries. This partly explai
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34

Macpherson, Niall T., Paul Merrikin, and Carlos Nunez. "Marginally deformed AdS5/CFT4 and spindle-like orbifolds." Journal of High Energy Physics 2024, no. 7 (2024). http://dx.doi.org/10.1007/jhep07(2024)042.

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Abstract We study marginal deformations of $$ \mathcal{N} $$ N = 2, d = 4 long linear quiver CFTs using the holographic description. We find a two-parameter family of AdS5 solutions that generically break all of supersymmetry, but preserve $$ \mathcal{N} $$ N = 1 for a particular tuning of the parameters. We study the G-structure of the $$ \mathcal{N} $$ N = 2 “parent” and the $$ \mathcal{N} $$ N = 1 backgrounds and carefully discuss the quantisation of charges in all cases. For the $$ \mathcal{N} $$ N = 1 and $$ \mathcal{N} $$ N = 0 cases, a picture emerges with “branes” back-reacted on eithe
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35

Castellani, Federico, and Carlos Nunez. "Holography for confined and deformed theories: TsT-generated solutions in type IIB supergravity." Journal of High Energy Physics 2024, no. 12 (2024). https://doi.org/10.1007/jhep12(2024)155.

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Abstract In this paper, we present a series of solutions of type IIB Supergravity, obtained through the TsT deformation of a seed background that is holographically dual to $$ \mathcal{N} $$ N = 4 Super Yang-Mills theory compactified on a circle (with a twist). We explore various holographic observables, focusing on disentangling the contributions of confinement, marginal deformations, and their interplay. Additionally, we provide a detailed analysis of how certain observables are influenced by the dynamics of the Kaluza-Klein (KK) modes arising from the circle compactification. Our results of
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36

Niarchos, Vasilis, and Kyriakos Papadodimas. "On the Kähler-Hodge structure of superconformal manifolds." Journal of High Energy Physics 2022, no. 9 (2022). http://dx.doi.org/10.1007/jhep09(2022)104.

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Abstract We show that conformal manifolds in d ≥ 3 conformal field theories with at least 4 supercharges are Kähler-Hodge, thus extending to 3d $$ \mathcal{N} $$ N = 2 and 4d $$ \mathcal{N} $$ N = 1 similar results previously derived for 4d $$ \mathcal{N} $$ N = 2 and $$ \mathcal{N} $$ N = 4 and various types of 2d SCFTs. Conformal manifolds in SCFTs are equipped with a holomorphic line bundle ℒ, which encodes the operator mixing of supercharges under marginal deformations. Using conformal perturbation theory and superconformal Ward identities, we compute the curvature of ℒ at a generic point
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37

Prakash, Shiroman, and Shubham Kumar Sinha. "Emergent supersymmetry at large N." Journal of High Energy Physics 2024, no. 1 (2024). http://dx.doi.org/10.1007/jhep01(2024)025.

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Abstract We search for infrared fixed points of Gross-Neveu Yukawa models with matrix degrees of freedom in d = 4 − ε. We consider three models — a model with SU(N) symmetry in which the scalar and fermionic fields both transform in the adjoint representation, a model with SO(N) symmetry in which the scalar and fermion fields both transform as real symmetric-traceless matrices, and a model with SO(N) symmetry in which the scalar field transforms as a real symmetric-traceless matrix, while the fermion transforms in the adjoint representation. These models differ at finite N, but their large-N l
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38

Eberhardt, Lorenz. "Summing over geometries in string theory." Journal of High Energy Physics 2021, no. 5 (2021). http://dx.doi.org/10.1007/jhep05(2021)233.

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Abstract We examine the question how string theory achieves a sum over bulk geometries with fixed asymptotic boundary conditions. We discuss this problem with the help of the tensionless string on $$ {\mathrm{\mathcal{M}}}_3\times {\mathrm{S}}^3\times {\mathbbm{T}}^4 $$ ℳ 3 × S 3 × T 4 (with one unit of NS-NS flux) that was recently understood to be dual to the symmetric orbifold SymN ($$ {\mathbbm{T}}^4 $$ T 4 ). We strengthen the analysis of [1] and show that the perturbative string partition function around a fixed bulk background already includes a sum over semi-classical geometries and la
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Lima, A. A., G. M. Sotkov, and M. Stanishkov. "On the dynamics of protected ramond ground states in the D1-D5 CFT." Journal of High Energy Physics 2021, no. 7 (2021). http://dx.doi.org/10.1007/jhep07(2021)120.

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Abstract We examine the behavior of the Ramond ground states in the D1-D5 CFT after a deformation of the free-orbifold sigma model on target space ($$ {\mathbbm{T}}^4 $$ T 4 )N/SN by a marginal interaction operator. These states are compositions of Ramond ground states of the twisted and untwisted sectors. They are characterized by a conjugacy class of SN and by the set of their “spins”, including both R-charge and “internal” SU(2) charge. We compute the four-point functions of an arbitrary Ramond ground state with its conjugate and two interaction operators, for genus-zero covering surfaces r
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40

Awata, Hidetoshi, Hiroaki Kanno, Andrei Mironov, and Alexei Morozov. "Shiraishi functor and non-Kerov deformation of Macdonald polynomials." European Physical Journal C 80, no. 10 (2020). http://dx.doi.org/10.1140/epjc/s10052-020-08540-4.

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AbstractWe suggest a further generalization of the hypergeometric-like series due to M. Noumi and J. Shiraishi by substituting the Pochhammer symbol with a nearly arbitrary function. Moreover, this generalization is valid for the entire Shiraishi series, not only for its Noumi–Shiraishi part. The theta function needed in the recently suggested description of the double-elliptic systems [Awata et al. JHEP 2020:150, arXiv:2005.10563, (2020)], 6d N = 2* SYM instanton calculus and the doubly-compactified network models, is a very particular member of this huge family. The series depends on two kin
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41

Minahan, Joseph, Usman Naseer, and Charles Thull. "Conformal field theories on deformed spheres, anomalies, and supersymmetry." SciPost Physics 10, no. 3 (2021). http://dx.doi.org/10.21468/scipostphys.10.3.063.

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We study the free energy of four-dimensional CFTs on deformed spheres. For generic nonsupersymmetric CFTs only the coefficient of the logarithmic divergence in the free energy is physical, which is an extremum for the round sphere. We then specialize to N=2N=2 SCFTs where one can preserve some supersymmetry on a compact manifold by turning on appropriate background fields. For deformations of the round sphere the cc anomaly receives corrections proportional to the supersymmetric completion of the (Weyl)^22 term, which we determine up to one constant by analyzing the scale dependence of various
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