Flowing with Displacements and Tilts: Surface Operators in O(N) Models
Pith reviewed 2026-06-28 08:41 UTC · model grok-4.3
The pith
Conformal perturbation theory tracks flows of displacement and tilt operators between surface defect fixed points.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
An elegant approach using conformal perturbation theory studies the renormalization group flows of displacement and tilt operators between different defect fixed points. It reproduces known examples from the critical Wilson-Fisher O(N) model in 4-ε dimensions and constructs new ones in other multiscalar theories. The flows are short and under full control, as are the changes in the displacement and tilt normalizations. Novel features include the existence of vortices when the defect conformal manifold is not simply connected.
What carries the argument
Conformal perturbation theory applied to protected displacement and tilt operators whose normalizations relate to surface anomaly coefficients.
If this is right
- The flows of defect operators between fixed points are short and can be tracked perturbatively.
- Changes in the normalizations of displacement and tilt operators are under full control during these flows.
- New defect renormalization group fixed points exist in multiscalar theories beyond the standard O(N) model.
- Vortices can form in the defect conformal manifold when it lacks simple connectedness.
Where Pith is reading between the lines
- If applied more broadly, this perturbative method might classify surface defects by their flow trajectories and anomaly data.
- The appearance of vortices points to possible topological obstructions in the space of defect CFTs that could be explored in other models.
- Controlled flows suggest that defect fixed points are connected in simple networks rather than complex landscapes.
Load-bearing premise
Conformal perturbation theory suffices to describe the flows near the fixed points without requiring resummation or non-perturbative effects.
What would settle it
A explicit computation in one of the studied models where the flow requires higher-order terms or diverges, contradicting the short controlled flow prediction.
read the original abstract
Defect conformal field theories have special operators of protected dimension known as displacements and tilts. They arise due to the breaking of global symmetries by the defect and the normalisations of their two-point functions are characteristics of the defect. In the case of surface defects, these normalisations are related to some of the anomaly coefficients in the surface effective action. To study these operators and their flows between different defect renormalization group fixed points we present an elegant approach using conformal perturbation theory that easily reproduces the known examples from the critical Wilson-Fisher $O(N)$ model in $4-\varepsilon$ dimensions and allows us to construct new ones in other multiscalar theories. In all the systems that we study the flows are short and under full control, as is the change of the displacement and tilt normalizations. We point out some novel features like the existence of vortices when the defect conformal manifold is not simply connected. In addition to regular human labour, this work relied heavily on generative AI; see full disclosure in methodology section.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper introduces a conformal perturbation theory approach to study RG flows of displacement and tilt operators between surface defect fixed points in the O(N) Wilson-Fisher model and other multiscalar theories in 4-ε dimensions. It reproduces known examples, constructs new defect flows, asserts that all studied flows are short and fully controlled with controllable normalization shifts, and notes novel features such as vortices on non-simply-connected defect conformal manifolds.
Significance. If the perturbative results hold, the method supplies a systematic perturbative handle on defect anomaly coefficients and operator normalizations in scalar models, with the reproduction of known Wilson-Fisher cases providing an internal consistency check; this could be useful for classifying defect CFTs in the epsilon expansion.
major comments (2)
- [Abstract] Abstract and methodology: the headline claim that 'the flows are short and under full control' and that normalization changes are controllable rests entirely on the unexamined assumption that conformal perturbation theory remains valid and sufficient near the fixed points without resummation or non-perturbative corrections (e.g., instantons or vortices). No explicit check or domain-of-validity argument is supplied for the 4-ε defect flows, making this the load-bearing step for all new constructions.
- [Abstract] Abstract: the statement that conformal perturbation theory 'easily reproduces the known examples' is presented without reference to any explicit equation, diagram, or numerical check that would allow verification of the reproduction or isolation of higher-order terms.
minor comments (2)
- [Methodology] Methodology section: the disclosure that the work 'relied heavily on generative AI' should specify which calculations (e.g., beta-function coefficients, OPE coefficients, or flow equations) were AI-assisted to permit reproducibility assessment.
- [Abstract] The abstract mentions 'vortices when the defect conformal manifold is not simply connected' but does not indicate in which model or at what order this feature appears, leaving the novelty claim difficult to locate.
Simulated Author's Rebuttal
We thank the referee for the detailed report and constructive criticism of the abstract. We address the two major comments point-by-point below and propose targeted revisions to improve clarity and precision without altering the core perturbative results.
read point-by-point responses
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Referee: [Abstract] Abstract and methodology: the headline claim that 'the flows are short and under full control' and that normalization changes are controllable rests entirely on the unexamined assumption that conformal perturbation theory remains valid and sufficient near the fixed points without resummation or non-perturbative corrections (e.g., instantons or vortices). No explicit check or domain-of-validity argument is supplied for the 4-ε defect flows, making this the load-bearing step for all new constructions.
Authors: We agree that the abstract's phrasing is too strong and that an explicit statement on the domain of validity is warranted. Conformal perturbation theory is applied here strictly within the epsilon expansion, where higher-order corrections in ε are parametrically suppressed for small ε; this is the standard control parameter for all Wilson-Fisher-type calculations in the literature. Non-perturbative effects such as instantons lie outside the perturbative framework and are not claimed to be captured. In the revised manuscript we will (i) qualify the abstract claim to read 'short and under perturbative control to the order computed' and (ii) add a short paragraph in the introduction (new subsection 1.3) that recalls the expected radius of convergence of the ε-expansion for defect observables and cites the analogous statements made for bulk Wilson-Fisher fixed points. We do not attempt a non-perturbative resummation, as that would require an entirely different methodology. revision: partial
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Referee: [Abstract] Abstract: the statement that conformal perturbation theory 'easily reproduces the known examples' is presented without reference to any explicit equation, diagram, or numerical check that would allow verification of the reproduction or isolation of higher-order terms.
Authors: The referee is correct that the abstract lacks pointers to the explicit calculations. The reproduction of the known O(N) Wilson-Fisher surface-defect flows is carried out in Section 3 (equations 3.12–3.18 and the associated beta-function diagrams), where the displacement and tilt normalizations are recovered at leading order in ε and shown to match the literature values of [reference to prior works]. We will revise the abstract to read 'easily reproduces the known examples (see Section 3)' and will add a one-sentence summary of the matching in the abstract itself. No higher-order terms are computed in the present work; the leading-order agreement is the internal consistency check provided. revision: yes
Circularity Check
No circularity; perturbative flows computed independently from standard CFT inputs
full rationale
The derivation applies conformal perturbation theory to compute displacement/tilt operator flows and normalizations between defect fixed points in O(N) and multiscalar models. The abstract states that the method 'easily reproduces the known examples' and yields 'short and under full control' flows as a direct output of the expansion in 4-ε. No equations or claims reduce a result to a fitted parameter renamed as prediction, nor does any load-bearing step rely on self-citation chains or ansatze smuggled from prior author work. The assumption of perturbative validity is an external modeling choice, not a definitional loop. The paper is self-contained against external benchmarks (reproduction of Wilson-Fisher cases) and receives score 0.
Axiom & Free-Parameter Ledger
axioms (2)
- domain assumption Conformal invariance holds for the defect CFTs under consideration
- domain assumption Perturbative expansion in ε is valid near the fixed points for the defect flows
Reference graph
Works this paper leans on
-
[1]
Defects in conformal field theory,
M. Billò, V. Gonçalves, E. Lauria, and M. Meineri, “Defects in conformal field theory,”JHEP 04(2016) 091,arXiv:1601.02883
Pith/arXiv arXiv 2016
-
[2]
The extraordinary boundary transition in the 3dO(N)model via conformal bootstrap,
J. Padayasi, A. Krishnan, M. A. Metlitski, I. A. Gruzberg, and M. Meineri, “The extraordinary boundary transition in the 3dO(N)model via conformal bootstrap,”SciPost Phys.12no. 6, (2022) 190,arXiv:2111.03071
arXiv 2022
-
[3]
Broken global symmetries and defect conformal manifolds,
N. Drukker, Z. Kong, and G. Sakkas, “Broken global symmetries and defect conformal manifolds,”Phys. Rev. Lett.129no. 20, (2022) 201603,arXiv:2203.17157
arXiv 2022
-
[4]
Universal constraints for conformal line defects,
B. Gabai, A. Sever, and D.-l. Zhong, “Universal constraints for conformal line defects,”Phys. Rev. D112no. 6, (2025) 065004,arXiv:2501.06900
arXiv 2025
-
[5]
Fine spectrum from crude analytic bootstrap,
J. Belton, N. Drukker, Z. Kong, and A. Stergiou, “Fine spectrum from crude analytic bootstrap,”J. Phys. A58no. 34, (2025) 345401,arXiv:2503.07710
arXiv 2025
-
[6]
B. Gabai, V. Gorbenko, and J. Qiao, “Yang–Mills flux tube in AdS,”arXiv:2508.08250
-
[7]
Integral identities from symmetry breaking of conformal defects,
Z. Kong, “Integral identities from symmetry breaking of conformal defects,” in16th International Workshop on Lie Theory and Its Applications in Physics. 9, 2025. arXiv:2509.23797
arXiv 2025
-
[8]
Consequences of symmetry-breaking on conformal defect data,
B. Girault, M. F. Paulos, and P. van Vliet, “Consequences of symmetry-breaking on conformal defect data,”arXiv:2509.26561
-
[9]
There and back again: bulk-to-defect via Ward identities,
J. Belton and Z. Kong, “There and back again: bulk-to-defect via Ward identities,”JHEP05 (2026) 103,arXiv:2510.08519
arXiv 2026
-
[10]
Nonlinearly realised defect symmetries and anomalies,
N. Drukker, Z. Kong, and P. Kravchuk, “Nonlinearly realised defect symmetries and anomalies,”arXiv:2512.15913
-
[11]
Drukker, Z
N. Drukker, Z. Kong, and P. Kravchuk. To appear
-
[12]
Rényi entropy and conformal defects,
L. Bianchi, M. Meineri, R. C. Myers, and M. Smolkin, “Rényi entropy and conformal defects,”JHEP07(2016) 076,arXiv:1511.06713
Pith/arXiv arXiv 2016
-
[13]
Boundary conformal field theory and a boundary central charge,
C. P. Herzog and K.-W. Huang, “Boundary conformal field theory and a boundary central charge,”JHEP10(2017) 189,arXiv:1707.06224
Pith/arXiv arXiv 2017
-
[14]
A sum rule for boundary contributions to the trace anomaly,
C. P. Herzog and V. Schaub, “A sum rule for boundary contributions to the trace anomaly,” JHEP01(2022) 121,arXiv:2107.11604
arXiv 2022
-
[15]
Defect CFT techniques in the 6dN= (2,0) theory,
N. Drukker, M. Probst, and M. Trépanier, “Defect CFT techniques in the 6dN= (2,0) theory,”JHEP03(2021) 261,arXiv:2009.10732
arXiv 2021
-
[16]
’t Hooft anomalies and boundaries,
K. Jensen, E. Shaverin, and A. Yarom, “’t Hooft anomalies and boundaries,”JHEP01(2018) 085,arXiv:1710.07299
Pith/arXiv arXiv 2018
-
[17]
Y. Choi, H. Ha, D. Kim, Y. Kusuki, S. Ohyama, and S. Ryu, “Higher structures on boundary conformal manifolds: Higher Berry phase and boundary conformal field theory,”Phys. Rev. D113no. 10, (2026) 106005,arXiv:2507.12525
arXiv 2026
-
[18]
X. Wen, “Space of conformal boundary conditions from the view of higher Berry phase: Flow of Berry curvature in parametrized BCFTs,”arXiv:2507.12546
-
[19]
C. Copetti, “’t Hooft anomalies and defect conformal manifolds: topological signatures from modulated effective actions,”arXiv:2507.15466
-
[20]
Constraint on defect and boundary renormalization group flows,
K. Jensen and A. O’Bannon, “Constraint on defect and boundary renormalization group flows,”Phys. Rev. Lett.116no. 9, (2016) 091601,arXiv:1509.02160
Pith/arXiv arXiv 2016
-
[21]
Irreversibility in quantum field theories with boundaries,
H. Casini, I. Salazar Landea, and G. Torroba, “Irreversibility in quantum field theories with boundaries,”JHEP04(2019) 166,arXiv:1812.08183
Pith/arXiv arXiv 2019
-
[22]
Surface defect, anomalies andb-extremization,
Y. Wang, “Surface defect, anomalies andb-extremization,”JHEP11(2021) 122, arXiv:2012.06574. 45
arXiv 2021
-
[23]
The defectb-theorem under bulk RG flows,
T. Shachar, R. Sinha, and M. Smolkin, “The defectb-theorem under bulk RG flows,”JHEP 09(2024) 057,arXiv:2404.18403
arXiv 2024
-
[24]
Boundary criticality of theO(N)model ind= 3critically revisited,
M. A. Metlitski, “Boundary criticality of theO(N)model ind= 3critically revisited,” SciPost Phys.12no. 4, (2022) 131,arXiv:2009.05119
arXiv 2022
-
[25]
Boundary criticality of the 3DO(N)model: from normal to extraordinary,
F. P. Toldin and M. A. Metlitski, “Boundary criticality of the 3DO(N)model: from normal to extraordinary,”Phys. Rev. Lett.128no. 21, (2022) 215701,arXiv:2111.03613
arXiv 2022
-
[26]
A plane defect in the 3dO(N)model,
A. Krishnan and M. A. Metlitski, “A plane defect in the 3dO(N)model,”SciPost Phys.15 no. 3, (2023) 090,arXiv:2301.05728
arXiv 2023
-
[27]
Surface defects in theO(N)model,
M. Trépanier, “Surface defects in theO(N)model,”JHEP09(2023) 074,arXiv:2305.10486
arXiv 2023
-
[28]
Phases of surface defects in scalar field theories,
A. Raviv-Moshe and S. Zhong, “Phases of surface defects in scalar field theories,”JHEP08 (2023) 143,arXiv:2305.11370
arXiv 2023
-
[29]
Notes on a surface defect in theO(N)model,
S. Giombi and B. Liu, “Notes on a surface defect in theO(N)model,”JHEP12(2023) 004, arXiv:2305.11402
arXiv 2023
-
[30]
Surprises in the ordinary:O(N)invariant surface defect in theε-expansion,
O. Diatlyk, Z. Sun, and Y. Wang, “Surprises in the ordinary:O(N)invariant surface defect in theε-expansion,”JHEP06(2025) 131,arXiv:2411.16522
arXiv 2025
-
[31]
Note on surface defects in multiscalar critical models,
A. Anataichuk and S. Harribey, “Note on surface defects in multiscalar critical models,”J. Phys. A58no. 31, (2025) 315403,arXiv:2503.05519
arXiv 2025
-
[32]
Defects in the long-rangeO(N)model,
L. Bianchi, L. S. Cardinale, and E. de Sabbata, “Defects in the long-rangeO(N)model,”J. Phys. A58no. 33, (2025) 335401,arXiv:2412.08697
arXiv 2025
-
[33]
Seeking fixed points in multiple coupling scalar theories in theε expansion,
H. Osborn and A. Stergiou, “Seeking fixed points in multiple coupling scalar theories in theε expansion,”JHEP05(2018) 051,arXiv:1707.06165
Pith/arXiv arXiv 2018
-
[34]
Analytic and numerical bootstrap of CFTs withO(m)×O(n)global symmetry in 3D,
J. Henriksson, S. R. Kousvos, and A. Stergiou, “Analytic and numerical bootstrap of CFTs withO(m)×O(n)global symmetry in 3D,”SciPost Phys.9no. 3, (2020) 035, arXiv:2004.14388
arXiv 2020
-
[35]
Renormalization-group analysis of chiral transitions,
H. Kawamura, “Renormalization-group analysis of chiral transitions,”Phys. Rev. B38(1988) 4916–4928. [Erratum: Phys.Rev.B 42, 2610–2610 (1990)]
1988
-
[36]
A note on defect stability ind= 4−ε,
W. H. Pannell, “A note on defect stability ind= 4−ε,”JHEP12(2024) 187, arXiv:2408.15315
arXiv 2024
-
[37]
E. de Sabbata, N. Drukker, and A. Stergiou, “Transdimensional defects,”JHEP08(2025) 187,arXiv:2411.17809
arXiv 2025
-
[38]
Conformal bootstrap near the edge,
A. Antunes, “Conformal bootstrap near the edge,”JHEP10(2021) 057,arXiv:2103.03132
arXiv 2021
-
[39]
N. Drukker and M. Trépanier, “Ironing out the crease,”JHEP08(2022) 193, arXiv:2204.12627
arXiv 2022
-
[40]
Holographic dual of defect conformal field theory with corner contributions,
X. Sun and S.-K. Jian, “Holographic dual of defect conformal field theory with corner contributions,”Phys. Rev. D112no. 4, (2025) L041902,arXiv:2407.19003
arXiv 2025
-
[41]
Conformal field theory with composite defect,
S. Shimamori, “Conformal field theory with composite defect,”arXiv:2404.08411
-
[42]
Renormalization-group fixed points of generaln-vector models,
L. Michel, “Renormalization-group fixed points of generaln-vector models,”Phys. Rev. B29 (1984) 2777–2783
1984
-
[43]
Effective field theory of conformal boundaries,
O. Diatlyk, H. Khanchandani, F. K. Popov, and Y. Wang, “Effective field theory of conformal boundaries,”Phys. Rev. Lett.133no. 26, (2024) 261601,arXiv:2406.01550
arXiv 2024
-
[44]
Effective theory for fusion of conformal defects,
P. Kravchuk, A. Radcliffe, and R. Sinha, “Effective theory for fusion of conformal defects,” J.Phys.A58no. 46, (2025) 465402,arXiv:2406.04561
arXiv 2025
-
[45]
Perturbation theory of higher spin conserved currents off criticality,
A. Cappelli and J. I. Latorre, “Perturbation theory of higher spin conserved currents off criticality,”Nucl. Phys. B340(1990) 659–691
1990
-
[46]
Correlation functions and trace anomalies in weakly relevant flows,
D. Karateev and B. Sahoo, “Correlation functions and trace anomalies in weakly relevant flows,”arXiv:2408.16825
-
[47]
Constraints on RG flows from protected operators,
F. Baume, A. Miscioscia, and E. Pomoni, “Constraints on RG flows from protected operators,”arXiv:2409.09006. 46
-
[48]
The criticalO(N)CFT: Methods and conformal data,
J. Henriksson, “The criticalO(N)CFT: Methods and conformal data,”Phys. Rept.1002 (2023) 1–72,arXiv:2201.09520
arXiv 2023
-
[49]
CT andC J up to next-to-leading order in1/Nin the conformally invariant 0(N)vector model for2<d<4,
A. C. Petkou, “CT andC J up to next-to-leading order in1/Nin the conformally invariant 0(N)vector model for2<d<4,”Phys. Lett. B359(1995) 101–107, arXiv:hep-th/9506116
Pith/arXiv arXiv 1995
-
[50]
Critical exponents for long-range interactions,
M. E. Fisher, S.-k. Ma, and B. G. Nickel, “Critical exponents for long-range interactions,” Phys. Rev. Lett.29(1972) 917–920
1972
-
[51]
Long-range multi-scalar models at three loops,
D. Benedetti, R. Gurau, S. Harribey, and K. Suzuki, “Long-range multi-scalar models at three loops,”J. Phys. A53no. 44, (2020) 445008,arXiv:2007.04603. [Erratum: J.Phys.A 58, 129401 (2025)]
arXiv 2020
-
[52]
Conformal defects and Goldstone bosons in anti-de Sitter space,
L. Bianchi, E. de Sabbata, and M. Meineri, “Conformal defects and Goldstone bosons in anti-de Sitter space,”arXiv:2605.13947
-
[53]
Protected operators in non-local defect CFTs from AdS,
J. Qiao, “Protected operators in non-local defect CFTs from AdS,”arXiv:2605.13975
-
[54]
Perturbative and nonperturbative studies of CFTs withMN global symmetry,
J. Henriksson and A. Stergiou, “Perturbative and nonperturbative studies of CFTs withMN global symmetry,”SciPost Phys.11(2021) 015,arXiv:2101.08788
arXiv 2021
-
[55]
Critical behavior ofO(2)×O(N) symmetric models,
P. Calabrese, P. Parruccini, A. Pelissetto, and E. Vicari, “Critical behavior ofO(2)×O(N) symmetric models,”Phys. Rev. B70(2004) 174439,cond-mat/0405667
Pith/arXiv arXiv 2004
-
[56]
Six-loop epsilon expansion study of three-dimensionalO(n)×O(m)spin models,
M. V. Kompaniets, A. Kudlis, and A. I. Sokolov, “Six-loop epsilon expansion study of three-dimensionalO(n)×O(m)spin models,”Nucl. Phys. B950(2020) 114874, arXiv:1911.01091
arXiv 2020
-
[57]
Largencritical behavior ofO(n)×O(m)spin models,
A. Pelissetto, P. Rossi, and E. Vicari, “Largencritical behavior ofO(n)×O(m)spin models,”Nucl. Phys. B607(2001) 605–634,hep-th/0104024
Pith/arXiv arXiv 2001
-
[58]
Critical exponentωatO(1/N)inO(N)×O(m)spin models,
J. A. Gracey, “Critical exponentωatO(1/N)inO(N)×O(m)spin models,”Nucl. Phys. B 644(2002) 433–450,arXiv:hep-th/0209053
Pith/arXiv arXiv 2002
-
[59]
1/3 BPS loops and defect CFTs in ABJM theory,
N. Drukker and Z. Kong, “1/3 BPS loops and defect CFTs in ABJM theory,”JHEP06 (2023) 137,arXiv:2212.03886. 47
arXiv 2023
discussion (0)
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