REVIEW
Two-Dimensional Gravity and Nonlinear Gauge Theory
High Energy Physics - Theory · Submitted 8 Dec 1993 · 27 references
Pith's verdict: A careful, honest synthesis of the author's own nonlinear-gauge-theory program; the classical gravity identifications check out, but the anomaly-free BRS claim in §2.5 is asserted rather than computed.
T0 · AI review
Why Pith says this
Highlight any text to comment on it.
Referee report
The paper
The paper claims
2D gravity is a gauge theory of a nonlinear Poincaré algebra.
The reading
What carries the argument
The load-bearing object is a nonlinear Lie algebra, defined by $[T_A,T_B]=W_{AB}(T)$ with $W_{AB}$ a polynomial in the generators and the generalized Jacobi identity $partial W_{[AB}/partial T_D,W_{C]D}=0$. The same functions $W_{AB}(Phi)$ are used as structure functions depending on scalar fields $Phi^A$, which is what makes the gauge transformation $delta h^A_mu=partial_mu c^A+(partial W_{BC}/partialPhi^A)h^B_mu c^C$, $deltaPhi^A=W^A{}_B(Phi)c^B$ close only on shell. The action $S=-frac12int d^2x,epsilon^{mu nu}[Phi^A R_{A mu nu}+(W_{BC}-Phi^Apartial W_{BC}/partialPhi^A)h^B_mu h^C_nu]$ is the machinery that turns an algebra choice into a gravity Lagrangian: its equations $D_muPhi^A=0$ and $epsilon^{mu nu}R_{A mu nu}=0$ become the torsion and curvature constraints of the gravity model. Because the algebra is open, the paper modifies the BRS transformation with a gauge-fixing fermion to get an on-shell nilpotent charge.
Extended reading notes
Core claim
The claim is that the first-order Lagrangian of two-dimensional $R^2$ gravity with dynamical torsion, $L_C=phi F_{01}-e alpha phi^2+varphi_a T_{01}{}^a-e beta varphi_a varphi^a-e gamma$, is exactly the general nonlinear gauge Lagrangian $L=-frac12 epsilon^{mu nu}[Phi^A R_{A mu nu}+(W_{BC}-Phi^A partial W_{BC}/partialPhi^A)h^B_mu h^C_nu]$ when the structure functions are those of the quadratically nonlinear Poincaré algebra $[P_a,P_b]=-epsilon_{ab}(alpha J J+beta eta^{cd}P_cP_d+gamma I)$. The gauge transformation (3.9) is likewise the nonlinear gauge transformation (2.16). Replacing the quadratic algebra by a general nonlinear Poincaré algebra $[P_a,P_b]=-epsilon_{ab}W(J)$ gives the generic dilaton gravity Lagrangian $L_S=-frac12epsilon^{mu nu}phi F_{mu nu}-frac12epsilon^{mu nu}varphi_a T_{mu nu}{}^a-eW(phi)$, and the supersymmetric extension gives the nonlinear super-Poincaré formulation of dilaton supergravity. The paper presents this as a Yang-Mills-like formulation: the hidden gauge symmetry includes diffeomorphisms and local Lorentz transformations, and the scalar fields $phi,varphi_a$ are the coadjoint partners of the gauge fields.
Load-bearing premise
The load-bearing premise is that the gauge-field transformation coefficient is fixed by $U^A{}_{BC}(Phi)=partial W_{BC}/partialPhi^A$, a choice imposed so that the composite parameter from the scalar commutator agrees with the one from the vector commutator; if a different consistent choice were possible, the transformation (2.16) and its matching to the gravity actions would change.
Original abstract
We review nonlinear gauge theory and its application to two-dimensional gravity. We construct a gauge theory based on nonlinear Lie algebras, which is an extension of the usual gauge theory based on Lie algebras. It is a new approach to generalization of the gauge theory. The two-dimensional gravity is derived from nonlinear Poincar{\' e} algebra, which is the new Yang-Mills like formulation of the gravitational theory. As typical examples, we investigate $R^2$ gravity with dynamical torsion and generic form of 'dilaton' gravity. The supersymmetric extension of this theory is also discussed.
The compiled record
The paper's own sentences, arranged, kept beside the review and separate from it. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
The abstract, sentence by sentence
We review nonlinear gauge theory and its application to two-dimensional gravity. We construct a gauge theory based on nonlinear Lie algebras, which is an extension of the usual gauge theory based on Lie algebras. It is a new approach to generalization of the gauge theory. The two-dimensional gravity is derived from nonlinear Poincar{\' e} algebra, which is the new Yang-Mills like formulation of the gravitational theory. As typical examples, we investigate $R^2$ gravity with dynamical torsion and generic form of 'dilaton' gravity. The supersymmetric extension of this theory is also discussed.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We review nonlinear gauge theory and its application to two-dimensional gravity. | background 0.67 | 0.40 | 0.08 | asserted 0.77 |
| s1 | We construct a gauge theory based on nonlinear Lie algebras, which is an extension of the usual gauge theory based on Lie algebras. | contribution 0.81 | 0.91 | 0.10 | asserted 1.00 |
| s2 | It is a new approach to generalization of the gauge theory. | contribution 0.55 | 0.31 | 0.08 | asserted 1.00 |
| s3 | The two-dimensional gravity is derived from nonlinear Poincar{\' e} algebra, which is the new Yang-Mills like formulation of the gravitational theory. | contribution 0.53 | 0.78 | 0.40 | asserted 1.00 |
| s4 | As typical examples, we investigate $R^2$ gravity with dynamical torsion and generic form of 'dilaton' gravity. | contribution 0.96 | 0.88 | 0.10 | asserted 0.97 |
| s5 | The supersymmetric extension of this theory is also discussed. | contribution 0.99 | 0.68 | 0.05 | asserted 0.95 |
What was examined, and what was not
- arXiv listing abstract v1
- full text
- figures and tables
- references and citing sentences
- relations to other papers
- P abstract
- S sections
- T body sentences
- C citations
- R cross-paper relations
References
How later papers used it
82 later papers cite it
1 later paper by other authors is listed below: 1 used its method or tool.
Uses its method or tool 1 of 5 papers with this label
-
To deform the sCJT action [ref] to the most general 2d Carroll dilaton supergravity model, we express it as a gPSM (see, e.g., [ref] ) and then use the rigidity of gPSMs [ref] , which are 2d topological, non-linear gauge theories [ref] .
Carroll dilaton supergravity in two dimensions (2024) · gPSM formulation · 0.93
How the literature uses it
70 arXiv papers cite this in 95 sentences
Papers citing it · 57 sentences without a confident label
Builds on it 4 papers
-
In this paper we provide a generalization of the two-dimensional Poisson sigma model in [ref] as to include fermionic worldsheet zero-forms facilitating the mapping of target space differential forms to vertex operators of worldsheet form degree zero.
2D sigma models and differential Poisson algebras · Introduction · 1.00
-
Nambu sigma model.— Generalizing the well-known Poisson sigma model [ref] to $p>1$, we propose the following Nambu sigma model: [equation] We note the appearance of two types of metrics $G$ and $G̃$, as well as auxiliary fields $η$ and $η̃$.
Nambu-Sigma model and effective membrane actions · Introduction · 0.98
-
Building in part on [ref] , we propose in section [ref] that the bulk model in question is a particular “Poisson sigma model” [ref] , which can be rewritten as a 2d dilaton gravity [ref] with potential [equation] which results in classical solutions with dS$_2$ and AdS$_2$ regions.
Dynamical actions and q-representation theory for double-scaled SYK · Introduction · 0.86
Uses its method or tool 5 papers
-
Our work is structured as follows * In section [ref] we study the classical solutions (subsection [ref]), and symmetry algebra (subsection [ref]) of the q-Schwarzian and match these to the classical limits of the known bulk descriptions of Liouville gravity and sinh dilaton gravity. * In section [ref] we prove that the theories are exactly dual by formulating the bulk theory in terms of a topological Poisson-sigma model [ref] .
The q-Schwarzian and Liouville gravity · Introduction · 0.93
-
To deform the sCJT action [ref] to the most general 2d Carroll dilaton supergravity model, we express it as a gPSM (see, e.g., [ref] ) and then use the rigidity of gPSMs [ref] , which are 2d topological, non-linear gauge theories [ref] .
Carroll dilaton supergravity in two dimensions · gPSM formulation · 0.93
-
The tools used to reach this aim are the gauge theoretic formulation of dilaton gravity [ref] as a PSM [ref] , combined with a Brown–Henneaux type of analysis [ref] , and, independently, the Euclidean path integral formulation [ref] , combined with heat kernel methods [ref] .
$AdS_2$ holography is (non-)trivial for (non-)constant dilaton · Introduction · 1.00
Compares with it 1 paper
-
Simultaneously, it constitutes a nonlinear type of gauge theory, which in contrast to topological prototypes like the Poisson Sigma Model [ref] has propagating degrees of freedom.
Lie Algebroid Yang Mills with Matter Fields · Introduction · 0.83
Cites it as background 27 papers
-
There are two ways to quantize a Poisson manifold depending on whether the starting point is the Poisson bracket [ref] or the two-dimensional Poisson sigma model [ref] .
2D sigma models and differential Poisson algebras · Introduction · 0.99
-
It is closely related to a specific type of non-linear gauge theory [ref] , a Poisson-sigma model (PSM) [ref] .
Poisson-sigma model for 2D gravity with non-metricity · Introduction · 0.81
-
An ordinary Poisson structure induces a two-dimensional topological sigma model, due to Ikeda, Schaller and Strobl [ref] , for which Cattaneo and Felder [ref] devised an Alexandrov-Kontsevich-Schwarz-Starobinsky [ref] path integral quantization scheme that reproduces Kontsevich's star product formula in trivial topology [ref] .
Differential Poisson Sigma Models with Extended Supersymmetry · Introduction · 0.98
Discussion
Disagree with the review, or know something it missed? Leave a comment, highlight any passage above to comment on it, or challenge this review formally.