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arxiv: 2604.15420 · v1 · submitted 2026-04-16 · ✦ hep-th · cond-mat.stat-mech· math-ph· math.MP

Recognition: unknown

Local CFTs extremise F

Authors on Pith no claims yet

Pith reviewed 2026-05-10 10:25 UTC · model grok-4.3

classification ✦ hep-th cond-mat.stat-mechmath-phmath.MP
keywords conformal field theorylong-range CFTsphere free energyextremizationO(N) modelepsilon expansionF-theoremnonlocal theories
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The pith

Local CFTs lie at the extrema of the sphere free energy along lines of long-range theories.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper proves that local conformal field theories appear as extrema of the universal sphere free energy when embedded in continuous families of nonlocal CFTs. These families are obtained by varying the scaling dimension Delta of the fundamental field via a nonlocal kinetic term with exponent zeta. At the value of Delta where the theory becomes local, the derivative of tilde F with respect to Delta is exactly zero. For unitary CFTs the local point is a maximum. The argument follows because only the nonlocal part of the action contributes to the derivative, and that part disappears in the local limit.

Core claim

Local CFTs lie at the extrema of the (universal part of the) sphere free energy tilde F(Delta) of the long-range CFTs: d tilde F / d Delta at Delta equal to Delta_local equals zero, and for unitary CFTs they locally maximise it. The simple proof uses the fact that the derivative of tilde F with respect to Delta receives contributions only from the nonlocal terms in the action. The nonlocal terms must be absent in the limit Delta to Delta_local, and hence the derivative is zero. Demonstrating maximisation then requires a proof of the generalised F-theorem in conformal perturbation theory to subleading order.

What carries the argument

The universal sphere free energy tilde F(Delta) equal to sin(pi d / 2) times log of the sphere partition function Z_S^d, whose derivative with respect to the parameter Delta vanishes when the long-range theory reaches its local point.

If this is right

  • The scaling dimension of the fundamental field is encoded as the zero of d tilde F / d Delta.
  • The result explains the derivative structure appearing in the large-N expansion of Delta_phi in the O(N) model.
  • It supplies a non-supersymmetric analogue of the known c, F, a extremisation mechanisms.
  • The relation is confirmed by direct calculation for the O(N) phi^4 theory and cubic CFTs in both the epsilon expansion and the large-N limit.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The same variational property might locate local fixed points inside other families of nonlocal deformations without separate computation of scaling dimensions.
  • It could be tested numerically in long-range models studied by bootstrap or Monte Carlo methods.
  • Higher derivatives of tilde F or other thermodynamic quantities on the sphere might obey related stationarity conditions at the local point.

Load-bearing premise

The derivative of tilde F with respect to Delta receives contributions only from the nonlocal terms in the action, which disappear as Delta approaches the local value.

What would settle it

An explicit computation of d tilde F / d Delta at the local Delta in any unitary model, such as the 3d Ising CFT or the O(N) vector model in epsilon expansion, that yields a nonzero result would falsify the claim.

read the original abstract

Many CFTs can be extended to lines of nonlocal CFTs parametrised by the scaling dimension $\Delta$ of the fundamental field appearing in the action. $\Delta=\frac{d}{2}-\zeta$ is set by the exponent of the kinetic term $(-\partial^2)^{\zeta}$, which is nonlocal for noninteger $\zeta$. If $\Delta$ is tuned to $\Delta_\mathrm{local}$, the scaling dimension of the fundamental field in the local CFT, arXiv:1703.05325 showed that we recover the conformal data of that CFT (plus a decoupled sector). One natural question is: how is the local point special on this line of nonlocal CFTs? We prove that these local CFTs lie at the extrema of the (universal part of the) sphere free energy $\tilde{F}(\Delta)=\sin(\frac{\pi d}{2}) \log Z_{S^d}$ of the long-range CFTs: $d\tilde{F}/d\Delta|_{\Delta=\Delta_\mathrm{local}}=0$; and for unitary CFTs they locally maximise it. The simple proof uses the fact that the derivative of $\tilde{F}$ with respect to $\Delta$ receives contributions only from the nonlocal terms in the action. The nonlocal terms must be absent in the limit $\Delta \to \Delta_\mathrm{local}$, and hence the derivative is zero. Demonstrating maximisation then requires a proof of the generalised $F$-theorem in conformal perturbation theory to subleading order. We check our result with the O$(N)$ $\phi^4$ and cubic CFTs in the $\epsilon$ expansion and the large-$N$ limit. This result provides a minimal encoding of the scaling dimension of the fundamental field in many CFTs, and also explains the curious derivative structure of the large-$N$ expansion of $\Delta_\phi$ in the O$(N)$ model. Finally, this nonlocal $F$-extremisation can be viewed as a non-supersymmetric version of the known $c,F,a$-extremisation mechanisms.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The paper claims that local CFTs recovered at a specific value of the parameter Delta in families of nonlocal long-range CFTs (with kinetic term exponent zeta) extremize the universal sphere free energy tilde F(Delta) = sin(pi d / 2) log Z_{S^d}. Specifically, it proves d tilde F / d Delta vanishes at Delta = Delta_local (the local CFT value), with local maximisation for unitary theories. The argument is that the derivative receives contributions only from nonlocal terms in the action, which are absent at the local point; maximisation requires a subleading generalised F-theorem in conformal perturbation theory. The result is checked via epsilon-expansion and large-N limits for O(N) phi^4 and cubic models, and interpreted as a non-supersymmetric analog of c,F,a-extremisation.

Significance. If the central claim holds, the result offers a simple, minimal encoding of the fundamental scaling dimension Delta_phi in many CFTs through extremisation of tilde F, explains the derivative structure of large-N expansions in the O(N) model, and provides a new perspective on F-theorems without supersymmetry. The explicit checks in controlled perturbative regimes add concrete support, and the connection to the referenced nonlocal construction strengthens the conceptual link between local and long-range CFTs.

major comments (2)
  1. [Abstract and §2] Abstract and §2 (proof sketch): the claim that d tilde F / d Delta receives contributions only from nonlocal terms in the action, which vanish as Delta -> Delta_local, does not yet address the decoupled sector recovered in the construction of arXiv:1703.05325. If this sector's action or sphere free energy retains any Delta dependence (e.g., via its own kinetic term or coupling to zeta), then its contribution to the derivative need not vanish, undermining the proof that d tilde F / d Delta = 0 at the local point.
  2. [Abstract and §4] Abstract and §4 (maximisation): demonstrating that the stationary point is a local maximum requires a proof of the generalised F-theorem to subleading order in conformal perturbation theory. The manuscript must supply the explicit steps of this argument (including any assumptions on unitarity or the form of the perturbation), as the abstract only states that it is needed; without these details the maximisation claim is not fully established.
minor comments (2)
  1. [Introduction] Clarify the precise definition of the universal part tilde F versus the full log Z_{S^d} and its relation to the standard F-theorem, especially in the presence of the decoupled sector.
  2. [§5] In the epsilon-expansion and large-N checks, provide explicit numerical values or a table showing that the derivative vanishes to the computed order, rather than only stating that the result is confirmed.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their careful reading of our manuscript and for the constructive comments. We address each major point below and have revised the text accordingly to strengthen the presentation.

read point-by-point responses
  1. Referee: [Abstract and §2] Abstract and §2 (proof sketch): the claim that d tilde F / d Delta receives contributions only from nonlocal terms in the action, which vanish as Delta -> Delta_local, does not yet address the decoupled sector recovered in the construction of arXiv:1703.05325. If this sector's action or sphere free energy retains any Delta dependence (e.g., via its own kinetic term or coupling to zeta), then its contribution to the derivative need not vanish, undermining the proof that d tilde F / d Delta = 0 at the local point.

    Authors: In the construction of arXiv:1703.05325, the limit Delta → Delta_local recovers the local CFT in the interacting sector together with a decoupled free scalar whose scaling dimension is fixed by the local theory. This decoupled sector has a strictly local kinetic term whose form is independent of the deformation parameter Delta (or zeta). Because the sector is completely decoupled, its contribution to the sphere partition function (and thus to tilde F) does not depend on Delta. The derivative d tilde F / d Delta therefore receives contributions exclusively from the nonlocal kinetic term of the interacting sector, which is absent at the local point. We will add a short clarifying paragraph in the revised §2 making this decoupling explicit. revision: yes

  2. Referee: [Abstract and §4] Abstract and §4 (maximisation): demonstrating that the stationary point is a local maximum requires a proof of the generalised F-theorem to subleading order in conformal perturbation theory. The manuscript must supply the explicit steps of this argument (including any assumptions on unitarity or the form of the perturbation), as the abstract only states that it is needed; without these details the maximisation claim is not fully established.

    Authors: We agree that the maximisation statement requires an explicit subleading argument. The present manuscript notes the necessity of a generalised F-theorem in conformal perturbation theory but does not derive the sign of the second derivative. In the revision we will expand §4 with the following steps: (i) the first-order variation of tilde F vanishes by the stationarity condition already established; (ii) the second-order term is proportional to the integral of the two-point function of the nonlocal perturbing operator; (iii) unitarity implies that this two-point function is positive definite, so the quadratic correction to tilde F is negative. The perturbation is taken to be the long-range deformation, which is relevant or marginal near the local fixed point. These assumptions will be stated clearly. The expanded derivation will be included in the revised manuscript. revision: yes

Circularity Check

0 steps flagged

No circularity: derivation is self-contained via external citation and independent F-theorem proof

full rationale

The central claim rests on two elements: (1) the cited result from arXiv:1703.05325 that nonlocal terms vanish at Delta_local (recovering the local CFT plus decoupled sector), and (2) a new proof of the generalized F-theorem in conformal perturbation theory to subleading order for the maximisation statement. Neither reduces to a self-definition, a fitted parameter renamed as prediction, nor a load-bearing self-citation chain; the derivative argument follows directly from the action's structure once the external vanishing is granted. The decoupled-sector concern raised in the skeptic note is a potential correctness issue, not a circularity reduction. The paper's checks in epsilon expansion and large-N are independent verifications, not inputs. Overall the derivation chain is non-circular.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central claim rests on the standard definition of nonlocal CFTs via fractional kinetic terms and the cited fact that Delta equals Delta_local recovers the local CFT. The generalized F-theorem is invoked for maximisation but its proof is not detailed in the abstract. No free parameters or invented entities are introduced.

axioms (1)
  • domain assumption The derivative of the sphere free energy tilde F with respect to Delta receives contributions only from the nonlocal terms in the action.
    This is the key fact used in the simple proof as stated in the abstract.

pith-pipeline@v0.9.0 · 5691 in / 1468 out tokens · 49765 ms · 2026-05-10T10:25:16.192338+00:00 · methodology

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Reference graph

Works this paper leans on

156 extracted references · 135 canonical work pages · 1 internal anchor

  1. [1]

    A scaling theory for the long-range to short-range crossover and an infrared duality

    Connor Behan, Leonardo Rastelli, Slava Rychkov and Bernardo Zan,A scaling theory for the long-range to short-range crossover and an infrared duality,Journal of Physics A: Mathematical and Theoretical50(Aug., 2017) 354002, [arXiv:1703.05325pdf], [Inspire]. (document), 1, 3, 2.3, 3, 11, 3.1, 3.2, 2, 3.3, 16, 3.3, 18, 5, 5.2.3, 7, G.2, G.2

  2. [2]

    6, 2, 2, 8, 4.2, 5.5, 5.7, 5.7.1, 6.1, 6.2, A, A

    Ludo Fraser-Taliente,The sphere free energy of the vector models to order 1/N, [arXiv:2507.16896pdf], [Inspire]. 6, 2, 2, 8, 4.2, 5.5, 5.7, 5.7.1, 6.1, 6.2, A, A

  3. [3]

    Ludo Fraser-Taliente and John Wheater,F-extremization determines certain large-N CFTs, JHEP04(Apr., 2025) 085, [arXiv:2412.10499 pdf], [Inspire]. 2, 7, B

  4. [4]

    Efrat Gerchkovitz, Jaume Gomis and Zohar Komargodski,Sphere Partition Functions and the Zamolodchikov Metric,JHEP11(Nov., 2014) 001, [arXiv:1405.7271 pdf], [Inspire]. 7, 5.1

  5. [5]

    The Exact Superconformal R-Symmetry Extremizes Z

    Daniel L. Jafferis,The Exact Superconformal R-Symmetry Extremizes Z,JHEP05(2012) 159, [arXiv:1012.3210pdf], [Inspire]. 7, 2.3

  6. [6]

    Towards the F-Theorem: N=2 Field Theories on the Three-Sphere

    Daniel L. Jafferis, Igor R. Klebanov, Silviu S. Pufu and Benjamin R. Safdi,Towards the F-Theorem:N= 2Field Theories on the Three-Sphere,JHEP06(2011) 102, [arXiv:1103.1181pdf], [Inspire]. – 73 –

  7. [7]

    Klebanov, Silviu S

    Igor R. Klebanov, Silviu S. Pufu and Benjamin R. Safdi,F-Theorem without Supersymmetry,JHEP10(2011) 038, [arXiv:1105.4598 pdf], [Inspire]. 7

  8. [8]

    A Background-Independent Closed String Action at Tree Level,

    Amr Ahmadain, Alexander Frenkel and Aron C. Wall,A Background-Independent Closed String Action at Tree Level, [arXiv:2410.11938pdf], [Inspire]. 2.3

  9. [9]

    Ludo Fraser-Taliente and Grigory Tarnopolsky,The large-Nstress tensor is not renormalized, 2026. 8, 2.3

  10. [10]

    Vasil’ev and Mikhail Yu

    Alexander N. Vasil’ev and Mikhail Yu. Nalimov,Analog of dimensional regularization for calculation of the renormalization-group functions in the 1/n expansion for arbitrary dimension of space,Theoretical and Mathematical Physics55(1983) 423–431, [Inspire]. 8

  11. [11]

    Derkachov, John A

    Massimiliano Ciuchini, Sergey E. Derkachov, John A. Gracey and Alexander N. Manashov, Computation of quark mass anomalous dimension at O(1/N2 f )in quantum chromodynamics, Nuclear Physics B579(2000) 56–100, [arXiv:hep-ph/9912221pdf], [Inspire]

  12. [12]

    Grigory Tarnopolsky,On Large N Expansion of the Sphere Free Energy,Phys. Rev. D96 (July, 2017) 025017, [arXiv:1609.09113pdf], [Inspire]. 8

  13. [13]

    Collins,Renormalization : An Introduction to Renormalization, the Renormalization Group and the Operator-Product Expansion, vol

    John C. Collins,Renormalization : An Introduction to Renormalization, the Renormalization Group and the Operator-Product Expansion, vol. 26 ofCambridge Monographs on Mathematical Physics. Cambridge University Press, Cambridge, 1984, doi:10.1017/9781009401807, [Inspire]. 2.3

  14. [14]

    Pufu,TheF-Theorem andF-Maximization,J

    Silviu S. Pufu,TheF-Theorem andF-Maximization,J. Phys. A50(Oct., 2017) 443008, [arXiv:1608.02960pdf], [Inspire]. 2.3, 2.3

  15. [15]

    Klebanov,Interpolating betweenaandF,JHEP03(Mar.,

    Simone Giombi and Igor R. Klebanov,Interpolating betweenaandF,JHEP03(Mar.,

  16. [16]

    Giombi and I

    117, [arXiv:1409.1937pdf], [Inspire]. 2.3, 2.3, 2.3

  17. [17]

    Ludo Fraser-Taliente,Quantum field theories with many fields, [arXiv:2603.04481pdf], [Inspire]. 2.3

  18. [18]

    2.3, 2.3

    Edwin Barnes, Ken Intriligator, Brian Wecht and Jason Wright,Evidence for the Strongest Version of the 4da-Theorem, viaa-Maximization Along RG Flows,Nuclear Physics B702 (2004) 131–162, [arXiv:hep-th/0408156pdf], [Inspire]. 2.3, 2.3

  19. [19]

    Sergei Gukov,Counting RG flows,Journal of High Energy Physics01(Jan., 2016) 020, [arXiv:1503.01474pdf], [Inspire]

  20. [20]

    Tatsuma Nishioka,Entanglement entropy: Holography and renormalization group,Reviews of Modern Physics90(Sept., 2018) 035007, [arXiv:1801.10352pdf], [Inspire]. 2.3

  21. [21]

    Zamolodchikov,Irreversibility of the Flux of the Renormalization Group in a 2D Field Theory,JETP Lett.43(1986) 730–732, [Inspire]

    Alexander B. Zamolodchikov,Irreversibility of the Flux of the Renormalization Group in a 2D Field Theory,JETP Lett.43(1986) 730–732, [Inspire]. 2.3

  22. [22]

    Casini, M

    Horacio Casini, Marina Huerta, Robert C. Myers and Alexandre Yale,Mutual information and the F-theorem, [arXiv:1506.06195pdf], [Inspire]. 2.3

  23. [23]

    Zohar Komargodski and Adam Schwimmer,On Renormalization Group Flows in Four Dimensions,JHEP12(2011) 099, [arXiv:1107.3987 pdf], [Inspire]. 2.3

  24. [24]

    Zohar Komargodski,The Constraints of Conformal Symmetry on RG Flows,JHEP07 (2012) 069, [arXiv:1112.4538pdf], [Inspire]

  25. [25]

    Luty, Joseph Polchinski and Riccardo Rattazzi,Thea-theorem and the Asymptotics of 4D Quantum Field Theory,JHEP01(2013) 152, [arXiv:1204.5221pdf], [Inspire]

    Markus A. Luty, Joseph Polchinski and Riccardo Rattazzi,Thea-theorem and the Asymptotics of 4D Quantum Field Theory,JHEP01(2013) 152, [arXiv:1204.5221pdf], [Inspire]. 2.3 – 74 –

  26. [26]

    Cardy,Is There a c Theorem in Four-Dimensions?,Phys

    John L. Cardy,Is There a c Theorem in Four-Dimensions?,Phys. Lett. B215(1988) 749–752, [Inspire]. 2.3

  27. [27]

    Heckman and Tom Rudelius,Evidence for C-theorems in 6D SCFTs, [arXiv:1506.06753pdf], [Inspire]

    Jonathan J. Heckman and Tom Rudelius,Evidence for C-theorems in 6D SCFTs, [arXiv:1506.06753pdf], [Inspire]. 2.3

  28. [28]

    Uhlemann,Evidence for a 5d F-theorem,Journal of High Energy Physics02(Feb., 2021) 192, [arXiv:2011.00006pdf], [Inspire]

    Martin Fluder and Christoph F. Uhlemann,Evidence for a 5d F-theorem,Journal of High Energy Physics02(Feb., 2021) 192, [arXiv:2011.00006pdf], [Inspire]

  29. [29]

    Sandipan Kundu,Renormalization Group Flows, the a-Theorem and Conformal Bootstrap, Journal of High Energy Physics2020(May, 2020) 14, [arXiv:1912.09479pdf], [Inspire]. 2.3

  30. [30]

    Klebanov and Grigory Tarnopolsky,Generalized F-Theorem and theϵExpansion,JHEP12(Dec., 2015) 155, [arXiv:1507.01960 pdf], [Inspire]

    Lin Fei, Simone Giombi, Igor R. Klebanov and Grigory Tarnopolsky,Generalized F-Theorem and theϵExpansion,JHEP12(Dec., 2015) 155, [arXiv:1507.01960 pdf], [Inspire]. 2.3, 5, 5.1, 27, 5.5, 6.2, 6.2.2, E, 2

  31. [31]

    Victor Gorbenko, Slava Rychkov and Bernardo Zan,Walking, Weak first-order transitions, and Complex CFTs,Journal of High Energy Physics10(Oct., 2018) 108, [arXiv:1807.11512pdf], [Inspire]. 2.3

  32. [32]

    Klebanov and Grigory Tarnopolsky,Conformal QEDd,F-Theorem and theϵExpansion,J

    Simone Giombi, Igor R. Klebanov and Grigory Tarnopolsky,Conformal QEDd,F-Theorem and theϵExpansion,J. Phys. A49(Feb., 2016) 135403, [arXiv:1508.06354 pdf], [Inspire]. 9

  33. [33]

    Klebanov,OnCJ andC T in Conformal QED,Journal of High Energy Physics08(Aug., 2016) 156, [arXiv:1602.01076pdf], [Inspire]

    Simone Giombi, Grigory Tarnopolsky and Igor R. Klebanov,OnCJ andC T in Conformal QED,Journal of High Energy Physics08(Aug., 2016) 156, [arXiv:1602.01076pdf], [Inspire]

  34. [34]

    Herzog and Abhay Shrestha,A Nonlocal Schwinger Model,JHEP06(June, 2025) 252, [arXiv:2412.02514 pdf], [Inspire]

    Ludo Fraser-Taliente, Christopher P. Herzog and Abhay Shrestha,A Nonlocal Schwinger Model,JHEP06(June, 2025) 252, [arXiv:2412.02514 pdf], [Inspire]. 7.1

  35. [35]

    Ludo Fraser-Taliente and Grigory Tarnopolsky,Conformal QED, in preparation, 2026. 9, 7.1

  36. [36]

    2.3, 2.3, 3.1, 3.1, 3.5

    Kit Fraser-Taliente and Ludo Fraser-Taliente,TheTµν of the conformal scalars, [arXiv:2601.05311pdf], [Inspire]. 2.3, 2.3, 3.1, 3.1, 3.5

  37. [37]

    2.3, 3.5, 6.2, 7.1

    Junchen Rong,Local/Short-range conformal field theories from long-range perturbation theory, [arXiv:2406.17958pdf], [Inspire]. 2.3, 3.5, 6.2, 7.1

  38. [38]

    PhD thesis, Stony Brook U., 2019

    Connor Classen Behan,Bootstrapping Some Continuous Families of Conformal Field Theories. PhD thesis, Stony Brook U., 2019. 2.3, 45

  39. [39]

    Albert Schwarz,Axiomatic conformal theory in dimensions>2 and AdS/CT correspondence,Letters in Mathematical Physics106(Sept., 2016) 1181–1197, [arXiv:1509.08064pdf], [Inspire]. 2.3

  40. [40]

    Paulos, Joao Penedones, Jonathan Toledo, Balt C

    Miguel F. Paulos, Joao Penedones, Jonathan Toledo, Balt C. van Rees and Pedro Vieira, The S-matrix bootstrap. Part I: QFT in AdS,Journal of High Energy Physics2017(Nov.,

  41. [41]

    133, [arXiv:1607.06109pdf], [Inspire]. 2.3

  42. [42]

    Idse Heemskerk, Joao Penedones, Joseph Polchinski and James Sully,Holography from Conformal Field Theory,Journal of High Energy Physics10(2009) 079, [arXiv:0907.0151pdf], [Inspire]. 2.3

  43. [43]

    2.3, 3, G, 45

    Connor Behan,Bootstrapping the long-range Ising model in three dimensions,Journal of – 75 – Physics A: Mathematical and Theoretical52(Jan., 2019) 075401, [arXiv:1810.07199pdf], [Inspire]. 2.3, 3, G, 45

  44. [44]

    Shota Komatsu, Yuya Kusuki, Marco Meineri and Hirosi Ooguri,Continuous Family of Conformal Field Theories and Exactly Marginal Operators, [arXiv:2512.11045pdf], [Inspire]. 2.3

  45. [45]

    Eric Perlmutter, Leonardo Rastelli, Cumrun Vafa and Irene Valenzuela,A CFT Distance Conjecture,Journal of High Energy Physics10(Oct., 2021) 070, [arXiv:2011.10040pdf], [Inspire]. 10

  46. [46]

    Matthias R. Gaberdiel, Anatoly Konechny and Cornelius Schmidt-Colinet,Conformal perturbation theory beyond the leading order,Journal of Physics A: Mathematical and Theoretical42(2009) 105402, [arXiv:0811.3149 pdf], [Inspire]. 10, 2, C.1

  47. [47]

    Vladimir Bashmakov, Matteo Bertolini and Himanshu Raj,On non-supersymmetric conformal manifolds: Field theory and holography,Journal of High Energy Physics2017 (Nov., 2017) 167, [arXiv:1709.01749pdf], [Inspire]

  48. [48]

    Connor Behan,Conformal manifolds: ODEs from OPEs,Journal of High Energy Physics 03(Mar., 2018) 127, [arXiv:1709.03967pdf], [Inspire]. 3.2

  49. [49]

    Kallol Sen and Yuji Tachikawa,First-order conformal perturbation theory by marginal operators, [arXiv:1711.05947pdf], [Inspire]

  50. [50]

    Stefan Hollands,Action principle for OPE,Nuclear Physics B926(Jan., 2018) 614–638, [arXiv:1710.05601pdf], [Inspire]. 10

  51. [51]

    Soumyadeep Chaudhuri, Changha Choi and Eliezer Rabinovici,Thermal order in large N conformal gauge theories,Journal of High Energy Physics04(Apr., 2021) 203, [arXiv:2011.13981pdf], [Inspire]. 10

  52. [52]

    Yu Nakayama,On the Trace Anomaly of the Chaudhuri–Choi–Rabinovici Model,Symmetry 13(Feb., 2021) 276, [arXiv:2101.02861pdf], [Inspire]. 10

  53. [53]

    Alfredo Giambrone, Adolfo Guarino, Emanuel Malek, Henning Samtleben, Colin Sterckx and Mario Trigiante,Holographic evidence for nonsupersymmetric conformal manifolds, Phys. Rev. D105(Mar., 2022) 066018, [arXiv:2112.11966pdf], [Inspire]. 10

  54. [54]

    Does hot QCD have a conformal manifold in the chiral limit?

    Shi Chen, Aleksey Cherman and Robert D. Pisarski,Does hot QCD have a conformal manifold in the chiral limit?, [arXiv:2603.09977pdf], [Inspire]. 10

  55. [55]

    Andreas Stergiou, Gian Paolo Vacca and Omar Zanusso,Weyl Covariance and the Energy Momentum Tensors of Higher-Derivative Free Conformal Field Theories,Journal of High Energy Physics06(June, 2022) 104, [arXiv:2202.04701pdf], [Inspire]. 2.3

  56. [56]

    Enrico Parisini, Kostas Skenderis and Benjamin Withers,The ambient space formalism, JHEP05(May, 2024) 296, [arXiv:2312.03820 pdf], [Inspire]

  57. [57]

    Anatoly Konechny,OPE in a generally covariant form, [arXiv:2603.06246pdf], [Inspire]. 2.3

  58. [58]

    Luty and Valentina Prilepina,Weyl versus Conformal Invariance in Quantum Field Theory,JHEP10(Oct., 2017) 170, [arXiv:1702.07079pdf], [Inspire]

    Kara Farnsworth, Markus A. Luty and Valentina Prilepina,Weyl versus Conformal Invariance in Quantum Field Theory,JHEP10(Oct., 2017) 170, [arXiv:1702.07079pdf], [Inspire]. 2.3

  59. [59]

    2.3, C.2

    Florent Baume, Boaz Keren-Zur, Riccardo Rattazzi and Lorenzo Vitale,The local – 76 – Callan-Symanzik equation: Structure and applications,Journal of High Energy Physics08 (2014) 152, [arXiv:1401.5983pdf], [Inspire]. 2.3, C.2

  60. [60]

    Ken Intriligator and Brian Wecht,The Exact Superconformal R-Symmetry Maximizes a, Nucl. Phys. B667(2003) 183–200, [arXiv:hep-th/0304128pdf], [Inspire]. 2.3

  61. [61]

    Francesco Benini and Nikolay Bobev,Exact two-dimensional superconformal R-symmetry and c-extremization,Physical Review Letters110(Feb., 2013) 061601, [arXiv:1211.4030pdf], [Inspire]

  62. [62]

    Francesco Benini and Nikolay Bobev,Two-dimensional SCFTs from wrapped branes and c-extremization,JHEP06(2013) 005, [arXiv:1302.4451 pdf], [Inspire]. 2.3

  63. [63]

    Fisher, Shang-keng Ma and Bernhard G

    Michael E. Fisher, Shang-keng Ma and Bernhard G. Nickel,Critical Exponents for Long-Range Interactions,Phys. Rev. Lett.29(1972) 917–920, [Inspire]. 3

  64. [64]

    Conformal Invariance in the Long-Range Ising Model

    Miguel F. Paulos, Slava Rychkov, Balt C. van Rees and Bernardo Zan,Conformal Invariance in the Long-Range Ising Model,Nuclear Physics B902(Jan., 2016) 246–291, [arXiv:1509.00008pdf], [Inspire]. 3, 3, 6.2.1, G

  65. [65]

    Connor Behan, Leonardo Rastelli, Slava Rychkov and Bernardo Zan,Long-range critical exponents near the short-range crossover,Physical Review Letters118(June, 2017) 241601, [arXiv:1703.03430pdf], [Inspire]. 3.3

  66. [66]

    Gubser, Christian Jepsen, Sarthak Parikh and Brian Trundy,O(N) and O(N) and O(N),JHEP11(Nov., 2017) 107, [arXiv:1703.04202 pdf], [Inspire]

    Steven S. Gubser, Christian Jepsen, Sarthak Parikh and Brian Trundy,O(N) and O(N) and O(N),JHEP11(Nov., 2017) 107, [arXiv:1703.04202 pdf], [Inspire]. 6.2.3

  67. [67]

    Simone Giombi and Himanshu Khanchandani,O(N)models with Boundary Interactions and their Long Range Generalizations,Journal of High Energy Physics08(Aug., 2020) 010, [arXiv:1912.08169pdf], [Inspire]. 36, 7.1

  68. [68]

    Phillips,Nonlocal Conformal Field Theory, [arXiv:2011.04662pdf], [Inspire]

    Bora Basa, Gabriele La Nave and Philip W. Phillips,Nonlocal Conformal Field Theory, [arXiv:2011.04662pdf], [Inspire]

  69. [69]

    Noam Chai, Mikhail Goykhman and Ritam Sinha,Long-Range Vector Models at Large N, JHEP09(Sept., 2021) 194, [arXiv:2107.08052 pdf], [Inspire]. 6.1

  70. [70]

    Connor Behan, Edoardo Lauria, Maria Nocchi and Philine van Vliet,Analytic and numerical bootstrap for the long-range Ising model,JHEP03(Mar., 2024) 136, [arXiv:2311.02742pdf], [Inspire]. 45

  71. [71]

    Dario Benedetti, Razvan Gurau, Sabine Harribey and Davide Lettera,Finite-size versus finite-temperature effects in the critical long-range O(N) model,JHEP02(2024) 078, [arXiv:2311.04607pdf], [Inspire]

  72. [72]

    Dario Benedetti, Edoardo Lauria, Dalimil Mazáč and Philine van Vliet,One-Dimensional Ising Model with1/r1.99 Interaction,Phys. Rev. Lett.134(May, 2025) 201602, [arXiv:2412.12243pdf], [Inspire]

  73. [73]

    Dario Benedetti, Edoardo Lauria, Dalimil Mazáč and Philine van Vliet,A strong-weak duality for the 1d long-range Ising model,SciPost Phys.20(2026) 029, [arXiv:2509.05250pdf], [Inspire]

  74. [74]

    Fanny Eustachon,The Lee-Yang model and its generalizations through the lens of long-range deformations, [arXiv:2603.27031pdf], [Inspire]. 16, 7.1

  75. [75]

    Valerio Pagni, Guido Giachetti, Andrea Trombettoni and Nicolò Defenu,One-dimensional – 77 – long-range Ising model: Two almost equivalent approximations,Phys. Rev. B113(Jan.,

  76. [76]

    014406, [arXiv:2510.02458pdf], [Inspire]

  77. [77]

    Super Sum rules for Long-Range Models,

    Kausik Ghosh, Miguel F. Paulos, Noé Suchel and Zechuan Zheng,Super Sum rules for Long-Range Models, [arXiv:2603.22395pdf], [Inspire]

  78. [78]

    Zhijin Li,Conformality loss and short-range crossover in long-range conformal field theories, [arXiv:2409.19392pdf], [Inspire]. 3

  79. [79]

    Ali Maalaoui,Conformal Fractional Dirac Operator and Spinorial Q-curvature, [arXiv:2505.05706pdf]. 3.1

  80. [80]

    Martin Lohmann, Gordon Slade and Benjamin C. Wallace,Critical two-point function for long-rangeO(n)models below the upper critical dimension,Journal of Statistical Physics 169(Nov., 2017) 1132–1161, [arXiv:1705.08540pdf], [Inspire]. 3.1

Showing first 80 references.