REVIEW 3 major objections 5 minor 62 references
Non-Abelian target space duals of Thurston geometries
T0 review · 3 major / 5 minor · reviewed 2026-08-16 · deepseek-v4-flash
Pith's one-line read The paper constructs explicit non-Abelian T-dual backgrounds for the Euclidean and Lorentzian Thurston geometries that admit a freely and transitively acting isometry subgroup, and checks their one-loop conformal invariance.
desk verdict Novel catalogue of non-Abelian T-duals for Thurston geometries, but the free-action classification in Tables 5–6 has verifiable counterexamples, so the affected dual backgrounds and the self-duality claim are not currently supported. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The machinery is Poisson-Lie T-duality on a semi-Abelian Drinfeld double. A Drinfeld double is a Lie group whose Lie algebra splits into two maximally isotropic subalgebras with respect to an ad-invariant bilinear form; here one factor is the non-Abelian isometry subalgebra, a Bianchi-type algebra, and the other is Abelian. The duality is implemented by the formula $\widetilde{E}(\tilde g) = (E_0 + \widetilde{\Pi}(\tilde g))^{-1}$, where $E_0$ is the constant $\sigma$-model matrix at the unit element and $\widetilde{\Pi}$ is the Poisson structure on the dual group. The key supporting classification is the list, in Tables 5 and 6, of three-dimensional Lie subalgebras of the Killing-vector algebra whose action on the Thurston manifold is free and transitive; this uses the invertibility of the matrix $A^\mu_a$ in equation (3.1).
What would settle it
Recompute the determinant $\det A^\mu_a$ for each subalgebra in Tables 5 and 6, in particular the $S^3$ subalgebra where the paper states $\det A = 1/\sin x$; if any determinant vanishes at a point where the paper claims transitivity, or if a subalgebra with free transitive action is missing, the corresponding entry in Tables 7 and 8 fails as a valid dual or the catalogue is incomplete.
Extended reading notes
Core claim
The central discovery is that the non-Abelian duals of the Euclidean and Lorentzian Thurston geometries are obtained by taking the isometry Lie subalgebra that acts freely and transitively on the target manifold as one half of a Drinfeld double, with an Abelian Lie algebra as the other half. For each admissible subalgebra, the paper constructs the constant matrix $E_0(e)$ that encodes the original geometry as a $\sigma$-model, performs the Poisson-Lie duality transformation, and obtains a dual background consisting of a metric and a B-field. In total, eight dual models are given for the Euclidean geometries and twelve for the Lorentzian ones. The paper further checks the one-loop $\beta$-function equations and finds that, among the duals, only those of $E^3$ with respect to $VII_0$, of the Lorentz Sol with respect to $VI_0$, and all duals of $M^3$ satisfy these conformal invariance conditions.
Load-bearing premise
The catalogue rests on the assertion that the three-dimensional subalgebras listed in Tables 5 and 6 are exactly the subalgebras of the isometry Lie algebras that act freely and transitively on the Thurston manifolds; this is checked through determinant conditions such as $\det A = 1/\sin x$ that are stated but not derived in the text.
Editorial extensions
If this is right
- Each listed dual pair in Tables 7 and 8 gives an explicit non-Abelian T-dual background of a Thurston geometry, complete with metric and B-field.
- For geometries whose isometry group is larger than the manifold, multiple inequivalent duals exist, one per admissible subalgebra; the Minkowski geometry $M^3$ yields the largest family, corresponding to all Bianchi algebras except $VI_a$, $VII_a$, and $IX$.
- The dual of $M^3$ with respect to the $III$ subalgebra is non-Abelian self-dual: after a coordinate change the metric is again $M^3$, with a B-field whose field strength vanishes.
- The duals of $M^3$ with respect to the $VI_0$ and $VII_0$ subalgebras have curvature singularities at $r=\pm\gamma$ and $r=\pm\epsilon$, showing that non-Abelian T-duality can map a geometry with no curvature singularity to one with two singularities.
- Only the duals of $E^3/VII_0$, Lorentz Sol/$VI_0$, and all duals of $M^3$ satisfy the one-loop conformal invariance equations; the other dual backgrounds in Tables 7 and 8 do not.
Reading between the lines
- If the classification of free-transitive subalgebras is complete, the same recipe could be applied to the broader moduli of Lorentzian left-invariant metrics on three-dimensional Lie groups, producing dual backgrounds beyond the Thurston list.
- The appearance of curvature singularities in duals of $M^3$ suggests a general phenomenon: non-Abelian duality need not preserve regularity, and a smooth geometry can be mapped to a singular string background; one could test whether adding a nontrivial dilaton gradient resolves these singularities.
- The method depends on free-transitive isometry subgroups, so geometries with only non-free transitive actions, such as coset spaces, would require the generalized-coset or double-field-theory framework; extending the catalogue to those cases could cover the excluded geometries like $S^3$, where transitivity fails at $\sin x=0$.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. This paper applies Poisson-Lie (PL) T-duality to the Euclidean and Lorentzian Thurston geometries. The authors compute Killing vectors, identify three-dimensional subalgebras of the isometry algebras that they claim act freely and transitively on the corresponding manifolds, and for each admissible subalgebra they construct a semi-Abelian Drinfeld double with an Abelian dual. Using the standard PL T-duality formulas of Section 2, they produce explicit dual sigma-model backgrounds, giving the constant matrix E0(e), coordinate transformations, dual metrics, and B-fields in Tables 7 and 8. A worked example for the Lorentz Sol geometry is presented in Section 4.1, and Section 5 examines one-loop conformal invariance of selected original and dual backgrounds, including a claimed non-Abelian self-duality of the M3 geometry.
Significance. If the catalogue of dual backgrounds were correct, the paper would provide a useful systematic set of non-Abelian duals for a well-known family of homogeneous three-dimensional geometries, with explicit and checkable data. The Lorentz Sol worked example is a genuine strength: the coordinate transformations do map the Killing vectors to the left-invariant vector fields, the E0 matrix reproduces the stated metric, and the dual backgrounds follow from formula (2.11). The explicit tables of E0 matrices, coordinate transformations, metrics, and B-fields are also valuable. However, the central classification of free and transitive actions in Tables 5 and 6 contains concrete errors, and several of the invalid rows are used to construct dual backgrounds in Table 8. The central claim is therefore not currently established.
major comments (3)
- [§3, Tables 5 and 6] The 'Free action' column is not checked pointwise, and several 'Yes' entries violate the free-action criterion (3.1). For the M3 geometry in Table 4, the Killing vectors satisfy k1=-(y∂x+x∂y), k2=-(z∂x+x∂z), and k4=z∂y−y∂z, so all three vanish at the origin p=(0,0,0). Consequently, in Table 6 the M3/III generator T1=-k2 vanishes at p, the M3/IV generator T2=k1+k4 vanishes at p, and the M3/V generators T1=-k1 and T2=k2+k4 both vanish at p. Since a vector field vanishing at p generates a one-parameter subgroup that fixes p, none of these actions is free; in addition, the tangent span at p has rank below three, so they are not transitive either. The same defect occurs in Table 5: H3/VII0 has T3=k4 vanishing on the z-axis, E3/IX has determinant zero at the origin, and E1×S2/IX has T2=0 at (y,z)=(π/2,0). These rows should be marked 'No' for free action, and the claim that all listed subgroups act freely and transitively is false.
- [§4, Tables 7 and 8] The dual backgrounds for M3/III, M3/IV, and M3/V listed in Table 8 are constructed from rows that fail the free and transitive condition, so they are not legitimate outputs of the Section 2 construction. In these cases the target manifold cannot be identified with the group G via a global diffeomorphism, and the use of formula (2.11) as a global dual is unjustified; at best, the algebraic expression could define a local dual away from the zero set of the vector fields. In particular, the claimed non-Abelian self-duality of M3/III in Section 5, equations (5.6)–(5.7), rests on an invalid row and should be removed or re-derived with a genuinely free action.
- [§3, Tables 5 and 6 (completeness)] The paper asserts completeness of the subalgebra classification, for example that M3 admits all Bianchi subalgebras except VIa, VIIa, and IX, but no derivation or determinant tabulation is provided for the free and transitive columns. The concrete errors identified above show that the enumeration cannot be taken at face value. A systematic calculation, or at least a table of det A for each row with the relevant parameter ranges, is required to establish both the 'free' and 'transitive' entries and the exhaustiveness of the list.
minor comments (5)
- [§4, first paragraph] There is a typo: 'non-Ablelian' should be 'non-Abelian'.
- [§5] There are typos in the bullets: 'filed' should be 'field' and 'the the' should be 'the'.
- [Tables 7 and 8] Several entries are difficult to read because of cramped formatting and ambiguous parentheses; for example, the Nil row in Table 7 appears to contain a fraction l2/l4 in the constant matrix, and the fSL(2,R) rows contain long unseparated expressions. Please reformat these tables with clearer notation and define all parameters (α0, β, ρ, λ, γ, σ, a, b) and their allowed ranges.
- [§3] The text says 'It can simply shown' and 'isomeric symmetries' in the introduction; these should be corrected.
- [§5, conformal invariance] The statement that 'only E3 and S3 are only the solutions' contains a double 'only'; please rephrase.
Circularity Check
No circularity: E0 is the standard input datum and the dual backgrounds are genuine outputs of formula (2.11).
full rationale
The derivation chain is: compute Killing vectors (Tables 3-4), classify three-dimensional subalgebras acting freely and transitively (Tables 5-6), choose E0(e) so that the Thurston metric is reproduced in group coordinates via (2.13), and then compute the dual background from the PL T-duality formula (2.11) with an Abelian dual. The only fitted object, E0(e), is the standard initial datum of the construction; it encodes the input metric and is not presented as a prediction. The dual metrics and B-fields in Tables 7-8 are new outputs of (2.11), and no equation identifies them with an input by construction. The M3/III self-duality is verified by the explicit coordinate transformation (5.6), not assumed. Self-citations [29,45,51] supply standard Drinfeld-double commutators or prior AdS classifications; they are not load-bearing because the mixed brackets follow from (2.4) and the dual computation is displayed. The free-action verification in Section 3 is asserted (e.g., det A = 1/sin x) rather than derived, and the skeptic's vanishing-Killing-vector examples may indicate misclassification; but these are correctness risks in the input classification, not circular reductions of outputs to inputs.
Assumptions & free parameters
free parameters (1)
- Subalgebra family parameters (alpha0, beta, rho, lambda, gamma, sigma, a, b)
assumptions (4)
- domain assumption Drinfeld double and Poisson-Lie T-duality formalism, specifically formulas (2.2), (2.8)-(2.11), taken from Klimcik and Severa.
- standard math Classification of three-dimensional real Lie algebras, the Bianchi types I-IX, with structure constants as in [38].
- domain assumption The metrics and lists of Thurston geometries in Tables 1-2 are taken from prior literature [5-7] and are correct.
- domain assumption The one-loop beta-function equations (5.3)-(5.5) are the correct conformal invariance conditions for the sigma-model, and the dilaton field can be chosen freely for each background.
Cite this review
Pith. "Pith review of Non-Abelian target space duals of Thurston geometries." pith.science (2026). https://pith.science/paper/KZRDR2A2
@misc{pith2026250501797,
author = {Pith},
title = {Pith review of: Non-Abelian target space duals of Thurston geometries},
year = {2026},
howpublished = {\url{https://pith.science/paper/KZRDR2A2}},
note = {Machine review of arXiv:2505.01797}
}
abstract
In this study, we proceed to investigate the Thurston geometries from the point of view of their Poisson-Lie (PL) T-dualizability. First of all, we find all subalgebras of Killing vectors that generate group of isometries acting freely and transitively on the three-dimensional target manifolds, where the Thurston metrics are defined. It is shown that three-dimensional Lie subalgebras are isomorphic to the Bianchi type algebras. We take the isometry subgroup of the metric as the first subgroup of Drinfeld double. In order to investigate the non-Abelian T-duality, the second subgroup must be chosen to be Abelian. Accordingly, the non-Abelian target space duals of these geometries are found via PL T-duality approach in the absence of $B$-field. We also comment on the conformal invariance conditions of the T-dual $\sigma$-models under consideration.
Reference graph
Works this paper leans on
-
[1]
W. P. Thurston, The geometry and topology of three-manifolds, (1980, http://www.msri.org/publications/books/gt3m/)
work page 1980
-
[2]
W. P. Thurston, Three-dimensional manifolds, Kleinian groups and hyperbolic geometry, Bull. American Math. Soc., New Series, 6 (1982) 357
work page 1982
-
[3]
W. P. Thurston,Three-dimensional geometry and topology, Vol. 1 (Princeton University Press, Princeton NJ, 1997)
work page 1997
-
[4]
Scott, The geometries of 3-manifolds,Bull
P. Scott, The geometries of 3-manifolds,Bull. London Math. Soc. 15 (1983) 401
work page 1983
-
[5]
G. C. Wick, Properties of Bethe-Salpeter wave functions,Phys. Rev. 96 (1954) 1124
work page 1954
-
[6]
Brief Note on Thurston Geometries in 3D Quadratic Curvature Theories
G. Alkac and D. Olgu Devecioglu, Brief note on Thurston geometries in 3D quadratic curvature theories,Phys. Rev. D 105 (2022) 064023, arXiv:2108.13695 [hep-th]
work page Pith review arXiv 2022
-
[7]
M. Boucetta and A. Chakkar, The moduli spaces of Lorentzian left-invariant metrics on threedimensional unimodular simply connected Lie groups,J. Korean Math. Soc. 59 (2022) 651
work page 2022
-
[8]
M. Boucetta and A. Chakkar, The isometry groups of Lorentzian three-dimensional uni- modular simply connected Lie groups,Rev. Un. Mat. Argentina63 (2022) 353. 28
work page 2022
Show all 62 references
-
[9]
Flores-Alfonso, C
D. Flores-Alfonso, C. S. Lopez-Monsalvo and M. Maceda, Thurston geometries in three- dimensional new massive gravity,Phys. Rev. Lett.127 (2021) 061102, arXiv:2104.00754 [gr-qc]
2021 arXiv
-
[10]
A. H. Taub, Empty space-times admitting a three parameter group of motions,Annals Math. 53 (1951) 472
1951
-
[11]
Kantowski and R
R. Kantowski and R. K. Sachs, Some spatially homogeneous anisotropic relativistic cos- mological models, J. Math. Phys.7 (1966) 443
1966
-
[12]
H. V. Fagundes, Relativistic cosmologies with closed, locally homogeneous spatial sec- tions, Phys. Rev. Lett.54 (1985) 1200
1985
-
[13]
Cadeau and E
C. Cadeau and E. Woolgar, New five-dimensional black holes classified by horizon ge- ometry, and a Bianchi VI braneworld, Class. Quant. Grav. 18 (2001) 527, arXiv:gr- qc/0011029
2001
-
[14]
Hassaine, New black holes of vacuum Einstein equations with hyperscaling violation and Nil geometry horizons,Phys
M. Hassaine, New black holes of vacuum Einstein equations with hyperscaling violation and Nil geometry horizons,Phys. Rev. D 91 (2015) 084054, arXiv:1503.01716 [hep-th]
2015 arXiv
-
[15]
Bravo-Gaete and M
M. Bravo-Gaete and M. Hassaine, Thermodynamics of dyonic black holes with Thurston horizon geometries, Phys. Rev. D97 (2018) 024020, arXiv:1710.02720 [hep-th]
2018 arXiv
-
[16]
Naderi and A
F. Naderi and A. Rezaei-Aghdam, New five-dimensional Bianchi type magnetically charged hairy topological black hole solutions in string theory,Eur. Phys. J. C79 (2019) 995, arXiv:1905.11302 [hep-th]
2019 arXiv
-
[17]
Flores-Alfonso, C
D. Flores-Alfonso, C. S. Lopez-Monsalvo and M. Maceda, Gravitational waves from Thurston geometries, Phys. Rev. D110 (2024) 024063, arXiv:2311.12985 [gr-qc]
2024 arXiv
-
[18]
Gegenberg, S
J. Gegenberg, S. Vaidya and J. F. Vazquez-Poritz, Thurston geometries from eleven dimensions, Class. Quant. Grav.19 (2002) L199, arXiv:hep-th/0205276
2002 arXiv
-
[19]
Gegenberg and G
J. Gegenberg and G. Kunstatter, Using 3D string-inspired gravity to understand the Thurston conjecture, Class. Quant. Grav.21 (2004) 1197, arXiv:hep-th/0306279
2004 arXiv
-
[20]
Klimcik and P
C. Klimcik and P. Severa, Dual non-Abelian duality and the Drinfeld double,Phys. Lett. B 351 (1995) 455, arXiv:hep-th/9502122
1995 arXiv
-
[21]
C.Klimcik, Poisson-LieT-duality, Nucl. Phys. (Proc. Suppl.) B46(1996)116, arXiv:hep- th/9509095
1996
-
[22]
Buscher, A symmetry of the string background field equations,Phys
T. Buscher, A symmetry of the string background field equations,Phys. Lett. B 194 (1987) 59; Path-integral derivation of quantum duality in nonlinear sigma-models,Phys. Lett. B 201 (1988) 466. 29
1987
-
[23]
X. C. de la Ossa and F. Quevedo, Duality symmetries from non-abelian isometries in string theory,Nucl. Phys. B 403 (1993) 377, arXiv:hep-th/9210021; A. Giveon and M. Rocek, On nonabelian duality, Nucl. Phys. B 421 (1994) 173, arXiv:hep-th/9308154; E. Alvarez, L. Alvarez-Gaume ...
1993 arXiv
-
[24]
V. G. Drinfeld,Quantum groups, in Proc. Intern. Cong. Math., Berkeley (1986) vol.1, Amer. Math. Soc. (1987), pp. 798-820
1986
-
[25]
Alekseev, C
A. Alekseev, C. Klimčík and A. A. Tseytlin, Quantum Poisson-Lie T-duality and WZNW model, Nucl. Phys. B 458 (1996) 430, arXiv:hep-th/9509123
1996 arXiv
-
[26]
Tyurin and R
E. Tyurin and R. von Unge, Poisson-Lie T-duality: the path-integral derivation,Phys. Lett. B 382 (1996) 233, arXiv:hep-th/9512025
1996 arXiv
-
[27]
Sfetsos, Poisson-Lie T-duality and supersymmetry,Nucl
K. Sfetsos, Poisson-Lie T-duality and supersymmetry,Nucl. Phys. (Proc. Suppl.)B 56 (1997) 302, arXiv:hep-th/9611199; Poisson-Lie T-duality beyond the classical level and the renormalization group,Phys. Lett. B432 (1998) 365, arXiv:hep-th/9803019
1997 arXiv
-
[28]
M. A. Lledo and V. S. Varadarajan,SU (2) Poisson-Lie T duality,Lett. Math. Phys.45 (1998) 247, arXiv:hep-th/9803175
1998 arXiv
-
[29]
M. A. Jafarizadeh and A. Rezaei-Aghdam, Poisson-Lie T-duality and Bianchi type alge- bras, Phys. Lett. B458 (1999) 477, arXiv:hep-th/9903152
1999 arXiv
-
[30]
S.MajidandE.J.Beggs, Poisson-LieT-dualityforquasitriangularLiebialgebras, Comm. Math. Phys. 220 (2001) 455
2001
-
[31]
Bossard and N
A. Bossard and N. Mohammedi, Poisson-Lie duality in the string effective action,Nucl. Phys. B 619 (2001) 128, arXiv:hep-th/0106211
2001 arXiv
-
[32]
Hlavaty and L
L. Hlavaty and L. Snobl, Classification of Poisson-Lie T-dual models with two- dimensional targets, Mod. Phys. Lett. A17 (2002) 429, arXiv:hep-th/0110139; Poisson- Lie T-plurality of three-dimensional conformally invariant sigma models,J. High Energy Phys. 05 (2004) 010, arXiv...
2002 arXiv
-
[33]
Eghbali and A
A. Eghbali and A. Rezaei-Aghdam, Poisson Lie symmetry and D-branes in WZW model on the Heisenberg Lie groupH4, Nucl. Phys. B 899 (2015) 165, arXiv:1506.06233 [hep- th]
2015 arXiv
-
[34]
Eghbali, L
A. Eghbali, L. Mehran-nia and A. Rezaei-Aghdam, BTZ black hole from Poisson-Lie T- dualizable sigma models with spectators,Phys. Lett. B772 (2017) 791, arXiv:1705.00458 [hep-th]. 30
2017 arXiv
-
[35]
Eghbali, Exact conformal field theories from mutually T-dualizableσ-models, Phys
A. Eghbali, Exact conformal field theories from mutually T-dualizableσ-models, Phys. Rev. D 99 (2019) 026001, arXiv:1812.07664 [hep-th]
2019 arXiv
-
[36]
Eghbali, R
A. Eghbali, R. Naderi and A. Rezaei-Aghdam, T-dualization of Gödel string cosmologies via Poisson-Lie T-duality approach, Eur. Phys. J. C 81 (2021) 68, arXiv:2002.00675 [hep-th]
2021 arXiv
-
[37]
Sakatani and Y
Y. Sakatani and Y. Satoh, On quantum Poisson-Lie T-duality of WZNW models,J. High Energy Phys. 01 (2024) 150, arXiv:2311.18530 [hep-th]
2024 arXiv
-
[38]
F. B. Estabrook, H. D. Wahlquist and C. G. Behr, Dyadic analysis of spatially ho- mogeneous world models, J. Math. Phys. 9 (1968) 497; G. F. R. Ellis and M. A. H. MacCallum, A class of homogeneous cosmological models, Commun. Math. Phys. 12 (1969) 108; M. Ryan and L. Shepley,H...
1968
-
[39]
Hassler, Poisson-Lie T-duality in Double Field Theory, Phys
F. Hassler, Poisson-Lie T-duality in Double Field Theory, Phys. Lett. B 807 (2020) 135455, arXiv:1707.08624 [hep-th]; S. Demulder, F. Hassler, G. Piccinini and D. C. Thompson, Generalised cosets, J. High Energy Phys. 09 (2020) 044, arXiv:1912.11036 [hep-th]
2020 arXiv
-
[40]
Hlavaty and M
L. Hlavaty and M. Turek, Nonabelian dualization of plane wave backgrounds,J. Mod. Phys. 3 (2012) 1088, arXiv:1201.5939 [hep-th]
2012 arXiv
-
[41]
Hlavaty and I
L. Hlavaty and I. Petr, New solvable sigma models in plane-parallel wave background, Int. J. Mod. Phys. A29 (2014) 1450009, arXiv:1308.0153 [hep-th]
2014 arXiv
-
[42]
Hlavaty and I
L. Hlavaty and I. Petr, Plane-parallel waves as duals of the flat background, Class. Quantum Grav. 32 (2015) 035005, arXiv:1406.0971 [hep-th]
2015 arXiv
-
[43]
Petrasek, L
F. Petrasek, L. Hlavaty and I. Petr, Plane-parallel waves as duals of the flat background II: T-duality with spectators,Class. Quantum Grav.34 (2017) 155003, arXiv:1612.08015 [hep-th]
2017 arXiv
-
[44]
Hlavaty, I
L. Hlavaty, I. Petr and F. Petrasek, Plane-parallel waves as duals of the flat back- ground III: T-duality with torsionless B-field,Class. Quantum Grav.35 (2018) 075012, arXiv:1711.08688 [hep-th]
2018 arXiv
-
[45]
Eghbali, R
A. Eghbali, R. Naderi and A. Rezaei-Aghdam, Non-Abelian T-duality ofAdSdd≤3 fami- lies by Poisson-Lie T-duality,Eur. Phys. J. C82 (2022) 580, arXiv:2111.07700 [hep-th]
2022 arXiv
-
[46]
Ramirez,AdS2 geometries and non-Abelian T-duality in non-compact spaces,J
A. Ramirez,AdS2 geometries and non-Abelian T-duality in non-compact spaces,J. High Energy Phys. 10 (2021) 020, arXiv:2106.09735 [hep-th]
2021 arXiv
-
[47]
Grϕn and S
ϕ. Grϕn and S. Hervik,Einstein’s general theory of relativity: with modern applications in cosmology,New York: Springer, (2007). 31
2007
-
[48]
Nakahara,Geometry, Topology and Physics, 2nd Edition, IOP, Bristol and Philadel- phia (2003)
M. Nakahara,Geometry, Topology and Physics, 2nd Edition, IOP, Bristol and Philadel- phia (2003)
2003
-
[49]
Snobl and L
L. Snobl and L. Hlavaty, Classification of 6-dimensional real Drinfeld doubles,Int. J. Mod. Phys. A17 (2002) 4043, arXiv:math/0202210
2002 arXiv
-
[50]
Patera and P
J. Patera and P. Winternitz, Subalgebras of real three- and four-dimensional Lie algebras, J. Math. Phys.18 (1977) 1449
1977
-
[51]
Hlavaty and L
L. Hlavaty and L. Snobl, Classification of 6-dimensional real Manin triples, arXiv:math/0202209
-
[52]
Bugden, Non-abelian T-folds,J
M. Bugden, Non-abelian T-folds,J. High Energy Phys.03 (2019) 189, arXiv:1901.03782 [hep-th]
2019 arXiv
-
[53]
Oliynyk, V
T. Oliynyk, V. Suneeta and E. Woolgar, A gradient flow for worldsheet nonlinear sigma models, Nucl. Phys. B 739 (2006) 441, arXiv:hep-th/0510239
2006 arXiv
-
[54]
Papadopoulos and E
G. Papadopoulos and E. Witten, Scale and conformal invariance in 2d σ-models, with an application to N = 4 supersymmetry, J. High Energy Phys. 03 (2025) 056, arXiv:2404.19526 [hep-th]
2025 arXiv
-
[55]
Sfetsos, K
K. Sfetsos, K. Siampos and D. C. Thompson, Renormalization of Lorentz non-invariant actions and manifest T-duality,Nucl. Phys. B827 (2010) 545, arXiv:0910.1345 [hep-th]
2010 arXiv
-
[56]
Klimcik, Affine Poisson and affine quasi-Poisson T-duality,Nucl
C. Klimcik, Affine Poisson and affine quasi-Poisson T-duality,Nucl. Phys. B939 (2019) 191, arXiv:1809.01614 [hep-th]
2019 arXiv
-
[57]
C. G. Callan, D. Friedan, E. Martinec and M. J. Perry, String in background fields,Nucl. Phys. B 262 (1985) 593
1985
-
[58]
Sen, Heterotic string in an arbitrary background field,Phys
A. Sen, Heterotic string in an arbitrary background field,Phys. Rev. D32 (1985) 2102
1985
-
[59]
Sen, Equations of motion for the heterotic string theory from the conformal invariance of the sigma model,Phys
A. Sen, Equations of motion for the heterotic string theory from the conformal invariance of the sigma model,Phys. Rev. Lett.55 (1985) 1846
1985
-
[60]
Tseytlin, Conformal anomaly in a two-dimensional sigma model on a curved back- ground and strings,Phys
A. Tseytlin, Conformal anomaly in a two-dimensional sigma model on a curved back- ground and strings,Phys. Lett. B178 (1986) 34
1986
-
[61]
C.M.HullandK.Townsend, Stringeffectiveactionsfromsigma-modelconformalanoma- lies, Nucl. Phys. B 301 (1988) 197
1988
-
[62]
Horowitz and D
G. Horowitz and D. Welch, String theory formulation of the three-dimensional black hole, Phys. Rev. Lett.71 (1993) 328. 32
1993
Reviewed August 16, 2026 · model on record in the stance chip above.
Discussion (0). Continue with ORCID to comment.