366 research outputs found

    Dynamics of SU(N)SU(N) Supersymmetric Gauge Theory

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    We study the physics of the Seiberg-Witten and Argyres-Faraggi-Klemm-Lerche-Theisen-Yankielowicz solutions of D=4D=4, N=2\mathcal{N}=2 and N=1\mathcal{N}=1 SU(N)SU(N) supersymmetric gauge theory. The N=1\mathcal{N}=1 theory is confining and its effective Lagrangian is a spontaneously broken U(1)N−1U(1)^{N-1} abelian gauge theory. We identify some features of its physics which see this internal structure, including a spectrum of different string tensions. We discuss the limit N→∞N\rightarrow\infty, identify a scaling regime in which instanton and monopole effects survive, and give exact results for the crossover from weak to strong coupling along a scaling trajectory. We find a large hierarchy of mass scales in the scaling regime, including very light WW bosons, and the absence of weak coupling. The light WW's leave a novel imprint on the effective dual magnetic theory. The effective Lagrangian appears to be inadequate to understand the conventional large NN limit of the confining N=1\mathcal{N}=1 theory.Comment: 28 pages, harvmac, 4 eps figures in separate uuencoded file. We have extended this paper considerably, adding new results, discussion and figures. In particular, we give exact formulas for masses and couplings along a scaling trajectory appropriate to the large NN limit. These formulas display a novel effect due to light electric WW bosons down to energy scales ∌e−N\sim e^{-N}, deep in the weak coupling magnetic regim

    Kodaira-Spencer Theory of Gravity and Exact Results for Quantum String Amplitudes

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    We develop techniques to compute higher loop string amplitudes for twisted N=2N=2 theories with c^=3\hat c=3 (i.e. the critical case). An important ingredient is the discovery of an anomaly at every genus in decoupling of BRST trivial states, captured to all orders by a master anomaly equation. In a particular realization of the N=2N=2 theories, the resulting string field theory is equivalent to a topological theory in six dimensions, the Kodaira--Spencer theory, which may be viewed as the closed string analog of the Chern--Simon theory. Using the mirror map this leads to computation of the `number' of holomorphic curves of higher genus curves in Calabi--Yau manifolds. It is shown that topological amplitudes can also be reinterpreted as computing corrections to superpotential terms appearing in the effective 4d theory resulting from compactification of standard 10d superstrings on the corresponding N=2N=2 theory. Relations with c=1c=1 strings are also pointed out.Comment: 178 pages, 20 figure

    Holomorphic Anomalies in Topological Field Theories

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    We study the stringy genus one partition function of N=2N=2 SCFT's. It is shown how to compute this using an anomaly in decoupling of BRST trivial states from the partition function. A particular limit of this partition function yields the partition function of topological theory coupled to topological gravity. As an application we compute the number of holomorphic elliptic curves over certain Calabi-Yau manifolds including the quintic threefold. This may be viewed as the first application of mirror symmetry at the string quantum level.Comment: 32 pages. Appendix by S.Kat

    Proofs of Two Conjectures Related to the Thermodynamic Bethe Ansatz

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    We prove that the solution to a pair of nonlinear integral equations arising in the thermodynamic Bethe Ansatz can be expressed in terms of the resolvent kernel of the linear integral operator with kernel exp(-u(theta)-u(theta'))/cosh[(1/2)(theta-theta')]Comment: 16 pages, LaTeX file, no figures. Revision has minor change

    Surface Operators in N=2 4d Gauge Theories

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    N=2 four dimensional gauge theories admit interesting half BPS surface operators preserving a (2,2) two dimensional SUSY algebra. Typical examples are (2,2) 2d sigma models with a flavor symmetry which is coupled to the 4d gauge fields. Interesting features of such 2d sigma models, such as (twisted) chiral rings, and the tt* geometry, can be carried over to the surface operators, and are affected in surprising ways by the coupling to 4d degrees of freedom. We will describe in detail a relation between the parameter space of twisted couplings of the surface operator and the Seiberg-Witten geometry of the bulk theory. We will discuss a similar result about the tt* geometry of the surface operator. We will predict the existence and general features of a wall-crossing formula for BPS particles bound to the surface operator.Comment: 25 pages, 4 figure

    Connections on the State-Space over Conformal Field Theories

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    Motivated by the problem of background independence of closed string field theory we study geometry on the infinite vector bundle of local fields over the space of conformal field theories (CFT's). With any connection we can associate an excluded domain DD for the integral of marginal operators, and an operator one-form ωΌ\omega_\mu. The pair (D,ωΌ)(D, \omega_\mu) determines the covariant derivative of any correlator of local fields. We obtain interesting classes of connections in which ωΌ\omega_\mu's can be written in terms of CFT data. For these connections we compute their curvatures in terms of four-point correlators, DD, and ωΌ\omega_\mu. Among these connections three are of particular interest. A flat, metric compatible connection \HG, and connections cc and cˉ\bar c having non-vanishing curvature, with cˉ\bar c being metric compatible. The flat connection cannot be used to do parallel transport over a finite distance. Parallel transport with either cc or cˉ\bar c, however, allows us to construct a CFT in the state space of another CFT a finite distance away. The construction is given in the form of perturbation theory manifestly free of divergences.Comment: 54pp. MIT-CTP-219

    Stokes matrices for the quantum differential equations of some Fano varieties

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    The classical Stokes matrices for the quantum differential equation of projective n-space are computed, using multisummation and the so-called monodromy identity. Thus, we recover the results of D. Guzzetti that confirm Dubrovin's conjecture for projective spaces. The same method yields explicit formulas for the Stokes matrices of the quantum differential equations of smooth Fano hypersurfaces in projective n-space and for weighted projective spaces.Comment: 20 pages. Introduction has been changed. Small corrections in the tex

    Higher S-dualities and Shephard-Todd groups

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    Abstract: Seiberg and Witten have shown that in N=2N=2 \mathcal{N}=2 SQCD with Nf = 2Nc = 4 the S-duality group PSL2\u2124PSL(2,Z) \mathrm{P}\mathrm{S}\mathrm{L}\left(2,\mathrm{\mathbb{Z}}\right) acts on the flavor charges, which are weights of Spin(8), by triality. There are other N=2N=2 \mathcal{N}=2 SCFTs in which SU(2) SYM is coupled to strongly-interacting non-Lagrangian matter: their matter charges are weights of E6, E7 and E8 instead of Spin(8). The S-duality group PSL2\u2124PSL(2,Z) \mathrm{P}\mathrm{S}\mathrm{L}\left(2,\mathrm{\mathbb{Z}}\right) acts on these weights: what replaces Spin(8) triality for the E6, E7, E8root lattices? In this paper we answer the question. The action on the matter charges of (a finite central extension of) PSL2\u2124PSL(2,Z) \mathrm{P}\mathrm{S}\mathrm{L}\left(2,\mathrm{\mathbb{Z}}\right) factorizes trough the action of the exceptional Shephard-Todd groups G4 and G8 which should be seen as complex analogs of the usual triality group S3 43WeylA2S3≃Weyl(A2) {\mathfrak{S}}_3\simeq \mathrm{Weyl}\left({A}_2\right) . Our analysis is based on the identification of S-duality for SU(2) gauge SCFTs with the group of automorphisms of the cluster category of weighted projective lines of tubular type. \ua9 2015, The Author(s)

    Analogue mouse pointer control via an online steady state visual evoked potential (SSVEP) brain-computer interface

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    The steady state visual evoked protocol has recently become a popular paradigm in brain–computer interface (BCI) applications. Typically (regardless of function) these applications offer the user a binary selection of targets that perform correspondingly discrete actions. Such discrete control systems are appropriate for applications that are inherently isolated in nature, such as selecting numbers from a keypad to be dialled or letters from an alphabet to be spelled. However motivation exists for users to employ proportional control methods in intrinsically analogue tasks such as the movement of a mouse pointer. This paper introduces an online BCI in which control of a mouse pointer is directly proportional to a user's intent. Performance is measured over a series of pointer movement tasks and compared to the traditional discrete output approach. Analogue control allowed subjects to move the pointer faster to the cued target location compared to discrete output but suffers more undesired movements overall. Best performance is achieved when combining the threshold to movement of traditional discrete techniques with the range of movement offered by proportional control

    Spontaneous Breaking of N=2 Global Supersymmetry

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    We study spontaneous supersymmetry breaking in N=2 globally supersymmetric theories describing a system of abelian vector multiplets. We find that the most general form of the action admits, in addition to the usual Fayet-Iliopoulos term, a magnetic Fayet-Iliopoulos term for the auxiliary components of dual vector multiplets. In a generic case, N=2 supersymmetry is broken down spontaneously to N=1. In some cases however, the scalar potential can drive the theory towards a N=2 supersymmetric ground state where massless dyons condense in the vacuum.Comment: 12 pages, LaTe
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