Integrability in Three-Dimensional Gravity: Eigenfunction-Forced KdV Flows
Pith reviewed 2026-05-18 08:02 UTC · model grok-4.3
The pith
Chiral boundary conditions in three-dimensional gravity reduce to a forced KdV equation with forcing set by Schrödinger eigenfunctions.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Starting from the Chern-Simons formulation, consistent boundary conditions on a non-compact spatial slice lead to boundary dynamics described by the potential modified KdV hierarchy. The dynamics reduce to a forced KdV equation, where the forcing term is determined self-consistently by the eigenfunctions of the associated Schrödinger operator. Using the inverse scattering transform, the reflectionless sector is solved via the Gelfand-Levitan-Marchenko method, while the radiative sector exhibits universal dispersive decay. This framework unifies AdS3 boundary dynamics with integrable hierarchies and elucidates the roles of solitons and radiation in the dual conformal field theory.
What carries the argument
The forced KdV equation whose forcing term is supplied by the eigenfunctions of the Schrödinger operator associated with the boundary data; it encodes the reduction of the Chern-Simons boundary dynamics under the chosen chiral conditions.
If this is right
- The reflectionless sector admits exact multi-soliton solutions constructed by the Gelfand-Levitan-Marchenko method.
- The radiative sector decays dispersively in a universal manner independent of initial details.
- Solitons and radiation acquire distinct interpretations in the dual conformal field theory.
- The boundary evolution belongs to an integrable hierarchy that can be solved by standard inverse-scattering techniques.
Where Pith is reading between the lines
- The self-consistent forcing suggests a feedback loop in which boundary eigenstates influence and are influenced by the gravitational degrees of freedom.
- Analogous reductions may exist for other choices of boundary conditions or for gravity in higher dimensions.
- Methods developed for forced KdV flows could be imported to compute explicit time-dependent observables on the AdS3 boundary.
Load-bearing premise
The chosen chiral boundary conditions remain consistent under the full time evolution and permit an exact reduction of the boundary dynamics to the forced KdV hierarchy without additional constraints or anomalies.
What would settle it
An explicit computation of the time-evolved boundary fields starting from the Chern-Simons action that either reproduces the forced KdV equation with the claimed eigenfunction forcing term or produces a mismatch indicating an inconsistency or anomaly.
read the original abstract
We uncover a direct connection between three-dimensional gravity with chiral boundary conditions and a class of forced integrable systems. Starting from the Chern-Simons formulation, we derive consistent boundary conditions on a non-compact spatial slice, leading to boundary dynamics described by the potential modified KdV hierarchy. The dynamics reduce to a forced KdV equation, where the forcing term is determined self-consistently by the eigenfunctions of the associated Schr\"{o}dinger operator. Using the inverse scattering transform, the reflectionless sector is solved via the Gelfand-Levitan-Marchenko method, while the radiative sector exhibits universal dispersive decay. This framework unifies AdS$_3$ boundary dynamics with integrable hierarchies and elucidates the roles of solitons and radiation in the dual conformal field theory.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript claims that starting from the Chern-Simons formulation of three-dimensional gravity, consistent chiral boundary conditions on a non-compact spatial slice lead to boundary dynamics governed by the potential modified KdV hierarchy. These dynamics reduce to a forced KdV equation whose forcing term is fixed self-consistently by the eigenfunctions of the associated Schrödinger operator. The reflectionless sector is solved exactly via the Gelfand-Levitan-Marchenko method, while the radiative sector exhibits universal dispersive decay, thereby unifying AdS3 boundary dynamics with integrable hierarchies and their implications for the dual CFT.
Significance. If the reduction steps and boundary-condition consistency are rigorously established, the result would furnish an explicit integrable structure for chiral boundary dynamics in 3D gravity, supplying exact soliton and radiation solutions through inverse scattering that could clarify the holographic dictionary for boundary excitations. The use of standard Chern-Simons reduction and the Gelfand-Levitan-Marchenko method is a strength, but the self-consistent forcing introduces a non-standard closure that requires verification.
major comments (2)
- [Abstract and derivation paragraph] Abstract and derivation paragraph: the central claim that the chosen chiral boundary conditions remain invariant under the full time evolution generated by the potential modified KdV hierarchy is asserted rather than derived from the Chern-Simons equations of motion. For a non-compact slice, explicit cancellation of residual boundary terms at spatial infinity must be shown; the self-consistent forcing term may otherwise introduce a hidden constraint that is not automatically preserved under the inverse scattering transform.
- [Section on boundary dynamics reduction] Section on boundary dynamics reduction (near Eq. for the forced KdV): the reduction from the potential modified KdV hierarchy to the single forced KdV equation with forcing determined by Schrödinger eigenfunctions is presented as exact, yet no explicit check is given that the resulting system remains closed under the full hierarchy flows without generating additional anomalies or constraints at infinity.
minor comments (2)
- Notation for the Schrödinger operator L and its eigenfunctions should be introduced with explicit definitions and domain specifications before the inverse-scattering discussion to improve readability.
- A brief comparison with prior literature on integrable boundary dynamics in AdS3 (e.g., works on KdV in holographic contexts) would help situate the novelty of the self-consistent forcing mechanism.
Simulated Author's Rebuttal
We thank the referee for the careful reading and constructive comments on our manuscript. We address the major points raised below and have revised the manuscript to provide the requested explicit verifications while preserving the original derivations.
read point-by-point responses
-
Referee: [Abstract and derivation paragraph] Abstract and derivation paragraph: the central claim that the chosen chiral boundary conditions remain invariant under the full time evolution generated by the potential modified KdV hierarchy is asserted rather than derived from the Chern-Simons equations of motion. For a non-compact slice, explicit cancellation of residual boundary terms at spatial infinity must be shown; the self-consistent forcing term may otherwise introduce a hidden constraint that is not automatically preserved under the inverse scattering transform.
Authors: We appreciate the referee's emphasis on rigor for the non-compact case. The invariance follows from the Chern-Simons equations of motion together with the chosen boundary conditions, but we agree an explicit boundary-term calculation strengthens the presentation. In the revised manuscript we have inserted a new paragraph immediately after the derivation of the boundary dynamics that computes the residual terms at spatial infinity. These terms cancel identically once the self-consistent forcing (determined by the Schrödinger eigenfunctions) and the asymptotic decay of the fields are substituted, confirming that no hidden constraint arises and that the conditions remain preserved under the inverse scattering transform. revision: yes
-
Referee: [Section on boundary dynamics reduction] Section on boundary dynamics reduction (near Eq. for the forced KdV): the reduction from the potential modified KdV hierarchy to the single forced KdV equation with forcing determined by Schrödinger eigenfunctions is presented as exact, yet no explicit check is given that the resulting system remains closed under the full hierarchy flows without generating additional anomalies or constraints at infinity.
Authors: We thank the referee for this observation. The reduction is obtained directly from the boundary equations, and closure under the hierarchy is guaranteed by the underlying integrability; nevertheless, we have added an explicit verification subsection. Using the asymptotic behavior of the eigenfunctions on the non-compact slice, we show that higher flows applied to the forced KdV equation produce no additional boundary anomalies or constraints at infinity, because the forcing term evolves consistently with the same eigenfunctions. This check is now included near the forced-KdV equation. revision: yes
Circularity Check
Derivation from Chern-Simons to eigenfunction-forced KdV hierarchy is self-contained
full rationale
The paper derives consistent boundary conditions directly from the Chern-Simons formulation on a non-compact slice, leading to boundary dynamics that reduce to the potential modified KdV hierarchy and then to a forced KdV equation. The forcing term being determined self-consistently by the Schrödinger eigenfunctions is a physical feature of the setup rather than a definitional loop or fitted input renamed as prediction. No load-bearing step reduces by the paper's own equations to its inputs by construction, and the abstract presents the consistency under time evolution as derived from the starting formulation without reliance on unverified self-citations or smuggled ansatzes. The overall chain remains independent of the target result.
Axiom & Free-Parameter Ledger
axioms (2)
- domain assumption Chern-Simons formulation provides an equivalent description of 3D gravity
- standard math Inverse scattering transform applies to the forced KdV equation obtained
Lean theorems connected to this paper
-
IndisputableMonolith/Foundation/RealityFromDistinction.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
Starting from the Chern-Simons formulation, we derive consistent boundary conditions on a non-compact spatial slice, leading to boundary dynamics described by the potential modified KdV hierarchy. The dynamics reduce to a forced KdV equation, where the forcing term is determined self-consistently by the eigenfunctions of the associated Schrödinger operator.
-
IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
S± := −∂²x + (12π/c) L±
-
IndisputableMonolith/Foundation/AlexanderDuality.leanalexander_duality_circle_linking unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
Alexander duality circle linking forces D = 3
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
Classical central extension for asymptotic symmetries at null infinity in three spacetime dimensions
G. Barnich and G. Compere, “Classical central extension for asymptotic symmetries at null infinity in three spacetime dimensions,”Class.Quant.Grav.24(2007) F15–F23,gr-qc/0610130
work page internal anchor Pith review Pith/arXiv arXiv 2007
-
[2]
Aspects of the BMS/CFT correspondence
G. Barnich and C. Troessaert, “Aspects of the BMS/CFT correspondence,”JHEP1005(2010) 062, 1001.1541
work page internal anchor Pith review Pith/arXiv arXiv 2010
-
[3]
Entanglement entropy in Galilean conformal field theories and flat holography
A. Bagchi, R. Basu, D. Grumiller, and M. Riegler, “Entanglement entropy in Galilean conformal field theories and flat holography,”Phys.Rev.Lett.114(2015), no. 11, 111602,1410.4089
work page internal anchor Pith review Pith/arXiv arXiv 2015
-
[4]
Correspondence between Asymptotically Flat Spacetimes and Nonrelativistic Conformal Field Theories,
A. Bagchi, “Correspondence between Asymptotically Flat Spacetimes and Nonrelativistic Conformal Field Theories,”Phys.Rev.Lett.105(2010) 171601
work page 2010
-
[5]
A. Bagchi, S. Detournay, and D. Grumiller, “Flat-Space Chiral Gravity,”Phys.Rev.Lett.109(2012) 151301, 1208.1658
work page internal anchor Pith review Pith/arXiv arXiv 2012
-
[6]
Cosmic evolution from phase transition of 3-dimensional flat space
A. Bagchi, S. Detournay, D. Grumiller, and J. Simon, “Cosmic Evolution from Phase Transition of Three-Dimensional Flat Space,”Phys.Rev.Lett.111(2013) 181301,1305.2919
work page internal anchor Pith review Pith/arXiv arXiv 2013
-
[7]
Holographic positive energy theorems in three-dimensional gravity
G. Barnich and B. Oblak, “Holographic positive energy theorems in three-dimensional gravity,”Class. Quant. Grav.31(2014) 152001,1403.3835
work page internal anchor Pith review Pith/arXiv arXiv 2014
-
[8]
Notes on the BMS group in three dimensions: I. Induced representations
G. Barnich and B. Oblak, “Notes on the BMS group in three dimensions: I. Induced representations,”JHEP 1406(2014) 129,1403.5803
work page internal anchor Pith review Pith/arXiv arXiv 2014
-
[9]
Flat Holography: Aspects of the dual field theory
A. Bagchi, R. Basu, A. Kakkar, and A. Mehra, “Flat Holography: Aspects of the dual field theory,”JHEP 12(2016) 147,1609.06203
work page internal anchor Pith review Pith/arXiv arXiv 2016
-
[10]
Flat space holography and the complex Sachdev-Ye-Kitaev model,
H. Afshar, H. A. González, D. Grumiller, and D. Vassilevich, “Flat space holography and the complex Sachdev-Ye-Kitaev model,”Phys. Rev. D101(2020), no. 8, 086024,1911.05739
- [11]
-
[12]
D. Grumiller and M. Riegler, “Carrollian c functions and flat space holographic RG flows in BMS3/CCFT2,” Phys. Rev. D108(2023), no. 12, 126008,2309.11539
-
[13]
Infinite Conformal Symmetry in Two-Dimensional Quantum Field Theory,
A. Belavin, A. M. Polyakov, and A. Zamolodchikov, “Infinite Conformal Symmetry in Two-Dimensional Quantum Field Theory,”Nucl.Phys.B241(1984) 333–380
work page 1984
-
[14]
Conformal Invariance and Surface Critical Behavior,
J. L. Cardy, “Conformal Invariance and Surface Critical Behavior,”Nucl. Phys. B240(1984) 514–532
work page 1984
-
[15]
Operator content of two-dimensional conformally invariant theories,
J. L. Cardy, “Operator content of two-dimensional conformally invariant theories,”Nucl. Phys.B270(1986) 186–204
work page 1986
-
[16]
P. Rodríguez, D. Tempo, and R. Troncoso, “Mapping relativistic to ultra/non-relativistic conformal symmetries in 2D and finite √ T Tdeformations,”JHEP11(2021) 133,2106.09750
-
[17]
J. D. Brown and M. Henneaux, “Central Charges in the Canonical Realization of Asymptotic Symmetries: An Example from Three-Dimensional Gravity,”Commun. Math. Phys.104(1986) 207–226. – 26 –
work page 1986
-
[18]
The Large N Limit of Superconformal Field Theories and Supergravity
J. M. Maldacena, “The largeNlimit of superconformal field theories and supergravity,”Adv. Theor. Math. Phys.2(1998) 231–252,hep-th/9711200
work page internal anchor Pith review Pith/arXiv arXiv 1998
-
[19]
Microscopic Origin of the Bekenstein-Hawking Entropy
A. Strominger and C. Vafa, “Microscopic Origin of the Bekenstein-Hawking Entropy,”Phys. Lett.B379 (1996) 99–104,hep-th/9601029
work page internal anchor Pith review Pith/arXiv arXiv 1996
-
[20]
New Boundary Conditions for AdS3
G. Compère, W. Song, and A. Strominger, “New Boundary Conditions forAdS3,”JHEP1305(2013) 152, 1303.2662
work page internal anchor Pith review Pith/arXiv arXiv 2013
-
[21]
Boundary conditions for General Relativity on AdS$_{3}$ and the KdV hierarchy
A. Pérez, D. Tempo, and R. Troncoso, “Boundary conditions for General Relativity on AdS3 and the KdV hierarchy,”JHEP06(2016) 103,1605.04490
work page internal anchor Pith review Pith/arXiv arXiv 2016
-
[22]
Integrable systems with BMS$_{3}$ Poisson structure and the dynamics of locally flat spacetimes
O. Fuentealba, J. Matulich, A. Pérez, M. Pino, P. Rodríguez, D. Tempo, and R. Troncoso, “Integrable systems with BMS3 Poisson structure and the dynamics of locally flat spacetimes,”JHEP01(2018) 148, 1711.02646
work page internal anchor Pith review Pith/arXiv arXiv 2018
-
[23]
Revisiting the asymptotic dynamics of General Relativity on AdS$_3$
H. A. González, J. Matulich, M. Pino, and R. Troncoso, “Revisiting the asymptotic dynamics of General Relativity on AdS3,”JHEP12(2018) 115,1809.02749
work page internal anchor Pith review Pith/arXiv arXiv 2018
-
[24]
E. Ojeda and A. Pérez, “Boundary conditions for General Relativity in three-dimensional spacetimes, integrable systems and the KdV/mKdV hierarchies,”JHEP08(2019) 079,1906.11226
-
[25]
Integrable Systems and Spacetime Dynamics,
M. Cárdenas, F. Correa, K. Lara, and M. Pino, “Integrable Systems and Spacetime Dynamics,”Phys. Rev. Lett.127(2021), no. 16, 161601,2104.09676
-
[26]
Generalized Fefferman-Graham gauge and boundary Weyl structures,
G. Arenas-Henriquez, F. Diaz, and D. Rivera-Betancour, “Generalized Fefferman-Graham gauge and boundary Weyl structures,”JHEP02(2025) 007,2411.12513
-
[27]
D. Grumiller and W. Merbis, “Near horizon dynamics of three dimensional black holes,”SciPost Phys.8 (2020), no. 1, 010,1906.10694
-
[28]
Integrable ponderomotive system: cavitons are solitons,
D. Kaup, “Integrable ponderomotive system: cavitons are solitons,”Physical review letters59(1987), no. 18, 2063
work page 1987
-
[29]
On the interaction of langmuir waves with acoustic waves in plasmas,
A. Latifi and J. Leon, “On the interaction of langmuir waves with acoustic waves in plasmas,”Physics Letters A152(1991), no. 3-4, 171–178
work page 1991
-
[30]
Solution of an initial-boundary value problem for coupled nonlinear waves,
J. Leon and A. Latifi, “Solution of an initial-boundary value problem for coupled nonlinear waves,”Journal of Physics A: Mathematical and General23(1990), no. 8, 1385
work page 1990
-
[31]
A. Latifi, “A class of integrable nonlinear evolution equations driven exclusively by extrinsic quadratic effects,”Transactions in Theoretical and Mathematical Physics2(2025), no. 1, 8–21
work page 2025
-
[32]
Asymptotic permanent profile of the ion acoustic wave driven by the langmuir wave,
D. Kaup, A. Latifi, and J. Leon, “Asymptotic permanent profile of the ion acoustic wave driven by the langmuir wave,”Physics Letters A168(1992), no. 2, 120–126
work page 1992
-
[33]
A simple derivation of canonical structure and quasi-local hamiltonians in general relativity,
J. Kijowski, “A simple derivation of canonical structure and quasi-local hamiltonians in general relativity,” General Relativity and Gravitation29(1997), no. 3, 307–343
work page 1997
-
[34]
C.-C. M. Liu and S.-T. Yau, “Positivity of Quasilocal Mass,”Phys. Rev. Lett.90(2003) 231102, gr-qc/0303019
work page internal anchor Pith review Pith/arXiv arXiv 2003
-
[35]
Quasi-Local Energy-Momentum and Angular Momentum in GR: A Review Article,
L. B. Szabados, “Quasi-Local Energy-Momentum and Angular Momentum in GR: A Review Article,”Living Rev. Rel.7(2004) 4
work page 2004
-
[36]
Spacetime structure near generic horizons and soft hair,
D. Grumiller, A. Pérez, M. Sheikh-Jabbari, R. Troncoso, and C. Zwikel, “Spacetime structure near generic horizons and soft hair,”Phys. Rev. Lett.124(2020), no. 4, 041601,1908.09833
-
[37]
H. Adami, D. Grumiller, S. Sadeghian, M. Sheikh-Jabbari, and C. Zwikel, “T-Witts from the horizon,” JHEP04(2020) 128,2002.08346
-
[38]
Symmetries at null boundaries: two and three dimensional gravity cases,
H. Adami, M. M. Sheikh-Jabbari, V. Taghiloo, H. Yavartanoo, and C. Zwikel, “Symmetries at null boundaries: two and three dimensional gravity cases,”JHEP10(2020) 107,2007.12759
-
[39]
Chiral Massive News: Null Boundary Symmetries in Topologically Massive Gravity,
H. Adami, M. M. Sheikh-Jabbari, V. Taghiloo, H. Yavartanoo, and C. Zwikel, “Chiral Massive News: Null Boundary Symmetries in Topologically Massive Gravity,”JHEP05(2021) 261,2104.03992. – 27 –
- [40]
-
[41]
Symmetries at causal boundaries in 2D and 3D gravity,
H. Adami, P. Mao, M. M. Sheikh-Jabbari, V. Taghiloo, and H. Yavartanoo, “Symmetries at causal boundaries in 2D and 3D gravity,”JHEP05(2022) 189,2202.12129
-
[42]
Characteristic forms and geometric invariants,
S.-S. Chern and J. Simons, “Characteristic forms and geometric invariants,”Annals Math.99(1974) 48–69
work page 1974
-
[43]
The partition function of degenerate quadratic functional and Ray-Singer invariants,
A. S. Schwarz, “The partition function of degenerate quadratic functional and Ray-Singer invariants,”Lett. Math. Phys.2(1978) 247–252
work page 1978
-
[44]
(2+1)-dimensional gravity as an exactly soluble system,
E. Witten, “(2+1)-dimensional gravity as an exactly soluble system,”Nucl. Phys.B311(1988) 46
work page 1988
-
[45]
A stress tensor for anti-de sitter gravity,
V. Balasubramanian and P. Kraus, “A stress tensor for anti-de sitter gravity,”Communications in Mathematical Physics208(1999), no. 2, 413–428
work page 1999
-
[46]
The large-n limit of superconformal field theories and supergravity,
J. Maldacena, “The large-n limit of superconformal field theories and supergravity,”International journal of theoretical physics38(1999), no. 4, 1113–1133
work page 1999
-
[47]
Three-Dimensional Gravity Revisited
E. Witten, “Three-Dimensional Gravity Revisited,”0706.3359
work page internal anchor Pith review Pith/arXiv arXiv
-
[48]
Most general AdS_3 boundary conditions
D. Grumiller and M. Riegler, “Most general AdS3 boundary conditions,”JHEP10(2016) 023,1608.01308
work page internal anchor Pith review Pith/arXiv arXiv 2016
-
[49]
Integrals of nonlinear equations of evolution and solitary waves,
P. D. Lax, “Integrals of nonlinear equations of evolution and solitary waves,”Communications on pure and applied mathematics21(1968), no. 5, 467–490
work page 1968
-
[50]
The motion integrals for the KdV equation and related inverse problems,
M. Novitskii, “The motion integrals for the KdV equation and related inverse problems,”Inverse problems 12(1996), no. 1, 55
work page 1996
-
[51]
A Simple model of the integrable Hamiltonian equation,
F. Magri, “A Simple model of the integrable Hamiltonian equation,”J. Math. Phys.19(1978) 1156–1162
work page 1978
-
[52]
P. J. Olver,Applications of Lie groups to differential equations, vol. 107. Springer Science & Business Media, 1993
work page 1993
-
[53]
Water wave propagation over uneven bottoms,
M. W. Dingemans, “Water wave propagation over uneven bottoms,”Delft University of Technology, TU Delft(1994)
work page 1994
-
[54]
Water wave propagation over uneven bottoms–part1–linear wave propagation,
M. Dinguemans, “Water wave propagation over uneven bottoms–part1–linear wave propagation,”Advanced Series on Ocean Engineering13(1997)
work page 1997
-
[55]
M. W. Dingemans,Water wave propagation over uneven bottoms (in 2 parts), vol. 13. World Scientific, 1997
work page 1997
-
[56]
A. Fokas and A. Latifi, “The nonlinear schr\" odinger equation with forcing involving products of eigenfunctions,”Open Communications in Nonlinear Mathematical Physics2(2022)
work page 2022
-
[57]
The korteweg–de vries equation with forcing involving products of eigenfunctions,
A. Fokas and A. Latifi, “The korteweg–de vries equation with forcing involving products of eigenfunctions,” J. Of Math. Phy., Anal., Geom19(2023)
work page 2023
-
[58]
On the determination of a differential equation from its spectral function,
I. M. Gel’fand and B. M. Levitan, “On the determination of a differential equation from its spectral function,”Izvestiya Rossiiskoi Akademii Nauk. Seriya Matematicheskaya15(1951), no. 4, 309–360
work page 1951
-
[59]
Concerning the theory of a differential operator of the second order,
V. Marchenko, “Concerning the theory of a differential operator of the second order,” inDoklady Akad. Nauk SSSR.(NS), vol. 72, pp. 457–460. 1950
work page 1950
-
[60]
Method for solving the korteweg-devries equation,
C. S. Gardner, J. M. Greene, M. D. Kruskal, and R. M. Miura, “Method for solving the korteweg-devries equation,”Physical review letters19(1967), no. 19, 1095
work page 1967
-
[61]
Solitons and the inverse scattering transform,
H. Segur, “Solitons and the inverse scattering transform,” tech. rep., 1980
work page 1980
-
[62]
M. J. Ablowitz and H. Segur,Solitons and the inverse scattering transform. SIAM, 1981
work page 1981
-
[63]
L. D. Faddeev and L. A. Takhtajan,Hamiltonian methods in the theory of solitons, vol. 23. Springer, 1987
work page 1987
-
[64]
P. G. Drazin and R. S. Johnson,Solitons: an introduction, vol. 2. Cambridge university press, 1989
work page 1989
-
[65]
O. Babelon, D. Bernard, and M. Talon,Introduction to classical integrable systems. Cambridge University Press, 2003
work page 2003
-
[66]
V. A. Marchenko,Sturm-Liouville operators and applications, vol. 373. American Mathematical Soc., 2011. – 28 –
work page 2011
-
[67]
Expectation value of composite field $T{\bar T}$ in two-dimensional quantum field theory
A. B. Zamolodchikov, “Expectation value of composite field T anti-T in two-dimensional quantum field theory,”hep-th/0401146
work page internal anchor Pith review Pith/arXiv arXiv
-
[68]
On space of integrable quantum field theories
F. A. Smirnov and A. B. Zamolodchikov, “On space of integrable quantum field theories,”Nucl. Phys. B 915(2017) 363–383,1608.05499
work page internal anchor Pith review Pith/arXiv arXiv 2017
-
[69]
$T \bar{T}$-deformed 2D Quantum Field Theories
A. Cavaglià, S. Negro, I. M. Szécsényi, and R. Tateo, “T¯T-deformed 2D Quantum Field Theories,”JHEP10 (2016) 112,1608.05534
work page internal anchor Pith review Pith/arXiv arXiv 2016
-
[70]
Moving the CFT into the bulk with $T\bar T$
L. McGough, M. Mezei, and H. Verlinde, “Moving the CFT into the bulk withTT,”JHEP04(2018) 010, 1611.03470
work page internal anchor Pith review Pith/arXiv arXiv 2018
-
[71]
An integrable Lorentz-breaking deformation of two-dimensional CFTs
M. Guica, “An integrable Lorentz-breaking deformation of two-dimensional CFTs,”SciPost Phys.5(2018), no. 5, 048,1710.08415
work page internal anchor Pith review Pith/arXiv arXiv 2018
-
[72]
$T\bar T$-deformations in closed form
G. Bonelli, N. Doroud, and M. Zhu, “T¯T-deformations in closed form,”JHEP06(2018) 149,1804.10967
work page internal anchor Pith review Pith/arXiv arXiv 2018
-
[73]
Holography at finite cutoff with a $T^2$ deformation
T. Hartman, J. Kruthoff, E. Shaghoulian, and A. Tajdini, “Holography at finite cutoff with aT2 deformation,”JHEP03(2019) 004,1807.11401
work page internal anchor Pith review Pith/arXiv arXiv 2019
-
[74]
The $T\overline T$ deformation of quantum field theory as random geometry
J. Cardy, “TheTTdeformation of quantum field theory as random geometry,”JHEP10(2018) 186, 1801.06895
work page internal anchor Pith review Pith/arXiv arXiv 2018
-
[75]
The $\textrm{T}\bar{\textrm{T}}$ perturbation and its geometric interpretation
R. Conti, S. Negro, and R. Tateo, “TheTTperturbation and its geometric interpretation,”JHEP02(2019) 085,1809.09593
work page internal anchor Pith review Pith/arXiv arXiv 2019
-
[76]
Heating up holography for single-traceJ¯Tdeformations,
L. Apolo and W. Song, “Heating up holography for single-traceJ¯Tdeformations,”JHEP01(2020) 141, 1907.03745
-
[77]
Solving a family of $T\bar{T}$-like theories
B. Le Floch and M. Mezei, “Solving a family ofT¯T-like theories,”1903.07606
work page internal anchor Pith review Pith/arXiv arXiv 1903
-
[78]
Infinite pseudo-conformal symmetries of classicalT¯T,J ¯TandJ T a - deformed CFTs,
M. Guica and R. Monten, “Infinite pseudo-conformal symmetries of classicalT¯T,J ¯TandJ T a - deformed CFTs,”SciPost Phys.11(2021), no. 4, 078,2011.05445
-
[79]
TTdeformation of classical Liouville field theory,
M. Leoni, “TTdeformation of classical Liouville field theory,”JHEP07(2020), no. 07, 230,2005.08906
-
[80]
Correlation functions of CFTs on a torus with aTTdeformation,
S. He and Y. Sun, “Correlation functions of CFTs on a torus with aTTdeformation,”Phys. Rev. D102 (2020), no. 2, 026023,2004.07486
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.