119685691
Gravitational actions in two dimensions and the Mabuchi functional
Abstract The Mabuchi energy is an interesting geometric functional on the space of Kahler metrics that plays a crucial role in the study of the geometry of Kahler manifolds. We show that this functional, as well as other related geometric actions, contribute to the effective gravitational action when a massive scalar field is coupled to gravity in two dimensions in a small mass expansion. This yields new theories of two-dimensional quantum gravity generalizing the standard Liouville models.
15378515
A model for gauge theories with Higgs fields
We discuss in details a simple, purely bosonic, quantum field theory belonging to larger class of models with the following properties: (a) They are asymptotically free, with a dynamically generated mass scale. (b) They have a space of parameters which gets quantum corrections drastically modifying the classical singularity structure. The quantum theory can have massless solitons, Argyres-Douglas-like CFTs, exhibit confinement, etc ... (c) The physics can, to a large extent, be worked out in models with a large number of supersymmetries as well as in purely bosonic ones. In the former case, exact BPS mass formulas can be derived, brane constructions and embedding in M theory do exist. (d) The models have an interesting 1/N expansion, and it is possible to define a double scaling limit in the sense of the ``old'' matrix models when approaching the singularities in parameter space. These properties make these theories very good toy models for four dimensional gauge theories with Higgs fields, and provide a framework where the effects of breaking supersymmetry can be explicitly studied. In our model, we work out in details the quantum space of parameters. We obtain the non-local lagrangian description of the Argyres-Douglas-like CFT, and show that it admits a strongly coupled fixed point. We also explicitly demonstrate property (d). The possibility of defining such double scaling limits was not anticipated on the gauge theory side, and could be of interest to understand the gauge theory/string theory correspondence.
16567547
Exact multiplets of spontaneously broken discrete global symmetries: The example of N=2 SUSY QCD
In these notes, we emphasize the r\^ole of spontaneous broken global discrete symmetries acting on the moduli space of $N=2$ susy Yang-Mills theories and show how they can be used, together with the BPS condition, as a spectrum generating symmetry. In particular, in the strong-coupling region, all BPS states come in multiplets of this broken symmetry. This played a key r\^ole in the determination of the strong-coupling spectra.
15116130
Galois symmetries in super Yang-Mills theories
Classifying the phases of gauge theories is hindered by the lack of local order parameters. In particular, the standard Wilson's and 't Hooft's non-local order parameters are known to be insufficient to explain the existence of the plethora of phases that are found in supersymmetric gauge theories. Motivated by these observations, we reanalyze the concept of gauge symmetry breaking using Galois theory. Unlike the ordinary classical notion of unbroken gauge group, the Galois symmetry makes sense in the full quantum theory and must be a phase invariant. The algebraic structure underlying the space of vacua of supersymmetric gauge theories, that we have developed recently, is precisely designed to allow a rigorous mathematical implementation of these ideas.
6368521
Planar diagrams and Calabi-Yau spaces
Large N geometric transitions and the Dijkgraaf-Vafa conjecture suggest a deep relationship between the sum over planar diagrams and Calabi-Yau threefolds. We explore this correspondence in details, explaining how to construct the Calabi-Yau for a large class of Mmatrix models, and how the geometry encodes the correlators. We engineer in particular two-matrix theories with potentials W (X; Y ) that reduce to arbitrary functions in the commutative limit. We apply the method to calculate all correlators htr X p i and htr Y p i in models of the form W (X; Y )= V (X )+ U(Y ) XY and W (X; Y )= V (X )+ YU (Y 2 )+ XY 2 . The solution of the latter example was not known, but when U is a constant we are able to solve the loop equations, nding a precise match with the geometric approach. We also discuss special geometry in multi-matrix models, and we derive an important property, the entanglement of eigenvalues, governing the expansion around classical vacua for which the matrices do not commute.
18522220
The BPS spectra and superconformal points in massive N = 2 supersymmetric QCD
We present a detailed study of the analytic structure, BPS spectra and superconformal points of the N = 2 susy SU(2) gauge theories with Nf = 1, 2, 3 massive quark hypermultiplets. We compute the curves of marginal stability with the help of the explicit solutions for the low-energy effective actions in terms of standard elliptic functions. We show that only a few of these curves are relevant. As a generic example, the case of Nf = 2 with two equal bare masses is studied in depth. We determine the precise existence domains for each BPS state, and show how they are compatible with the RG flows. At the superconformal point, where two singularities coincide, we prove that (for Nf = 2) the massless spectrum consists of four distinct BPS states and is S-invariant. This is due to the monodromy around the superconformal point being S, providing strong evidence for exact S-duality of the SCFT For all Nf, we compute the slopes ω of the β-functions at the fixed point couplings and show that they are related to the anomalous dimensions α of u = 〈trƒ2〉 by ω = 2(α − 1).
121963535
Bosonization techniques on algebraic curves and conformal field theories
The bosonization of b‐c systems is studied with conformal weight λ on Riemann surfaces in which the moduli space is parametrized by the branch points (algebraic curves). Besides being interesting in itself, the problem is related to perturbative string theories and to nonfree conformal field theories on the complex plane with the insertion of certain spin fields called the twist fields. The method of λ‐differentials is proposed, which allows a complete treatment of the b‐c systems on algebraic curves with local Abelian monodromy group. It can be nevertheless applied also to more general algebraic curves allowing the computation of the Green’s functions and shedding some light about the structure of the twist fields in the general case. The connections between our formalism and the solutions of the Riemann monodromy problem, used to find out the conformal blocks of conformal field theories, are pointed out.
119268708
On a field theoretical model of polymeric $2s-$plats and some of its consequences
The main subject of this work is the statistical mechanics of a system of N polymer rings linked together. The link that arises in this way is constrained to be in the form of a 2s-plat, where 2s is the fixed number of maxima and minima of the polymer trajectories along one chosen direction. Plats appear very often in nature, in particular in the DNA of living organisms. The topological states of the link are distinguished using the Gauss linking number. This is a relatively weak link invariant in the case of a general link, but its efficiency improves when 2s-plats are considered as it will be proved here. Using field theoretical methods, a nonperturbative expression of the partition function of the system is achieved. In its final form, this partition function is equivalent to that of a multi-layer electron gas. Such quasi-particle systems are studied in connection with several interesting applications, including high-Tc superconductivity and topological quantum computing. It is shown that the topological constraints acting on the polymer rings generate two and three-body forces acting on the monomers. These forces interphere with the non-topological two-body forces to which monomers are subjected in a solution, enhancing for instance the attraction between the monomers. What is remarkable is the appearance of three-body forces of topological origin. It is shown that these three-body interactions have nonvanishing contributions when three or more rings are entangled together.
15099856
Topologically nontrivial sectors of the Maxwell field theory on algebraic curves
Abstract In this paper a large family of nondegenerate metrics is derived on general algebraic curves. In this way, it is possible to treat many differential equations arising in quantum mechanics and field theories on Riemann surfaces as differential equations on the complex sphere. The case of the Maxwell field theories on curves with Z n group of automorphisms is studied in details. These curves are particularly important because they cover the entire moduli space spanned by the Riemann surfaces of genus g ≤ 2. All the classical solutions of the Maxwell equations are explicitly constructed. Also the examples of the scalar fields and of an electron immersed in a constant magnetic field will be briefly investigated.
62788967
On a possible approach to general field theories with nonpolynomial interactions
In this work a class of massive scalar field theories with self-interactions described by a general potential is studied. Under the sole condition that the potential admits the Fourier representation, it is shown that such theories may be mapped into a standard field theory, in which the interaction of the new fields is a polynomial of fourth degree. With some restrictions, this mapping allows the perturbative treatment of models that are otherwise intractable with standard field theoretical methods. 
A nonperturbative approach to these theories is attempted. The original scalar field is integrated out exactly at the price of introducing auxiliary vector fields. The latter are treated in a mean field theory approximation. The singularities that arise after the elimination of the auxiliary fields are cured using the dimensional regularization. The expression of the counterterms to be subtracted is computed.
122396324
Polymer topology and Chern-Simons field theory
Abstract In this paper the statistical mechanical problem of two topologically linked polymers is related to a topological Ginzburg-Landau model coupled to two Chern-Simons field theories. The Chern-Simons fields play the role of propagators of the topological interactions. The effects of the topological constraints is investigated using the method of effective potential in one-loop approximation.