Abstract:Using Seiberg-Witten theory it is known that the dynamics of N = 2 supersymmetric SU (n) Yang-Mills theory is determined by a Riemann surface Σ n . In particular the mass formula for BPS states is given by the periods of a special differential on Σ n . In this note we point out that the surface Σ n can be obtained from the quotient of a symmetric n-monopole spectral curve by its symmetry group. Known results about the Seiberg-Witten curves then implies that these monopoles are related to the A (1) n−1 Toda lat… Show more
“…One way to construct this space is to consider its simply connected double cover and then mod by the cyclic symmetry of two monopoles -Z 2 . We will now describe a procedure due to Sutcliffe [16] which relates the spectral curves to the curves associated with d = 4 super Yang-Mills theory. We recall the spectral curve for two monopoles…”
The coulomb branch of N = 4 supersymmetric Yang-Mills gauge theories in d = 2 + 1 is studied. A direct connection between gauge theories and monopole moduli spaces is presented. It is proposed that the hyper-Kähler metric of supersymmetric N = 4 SU(N) Yang-Mills theory is given by the charge N centered moduli space of BPS monopoles in SU(2). The theory is compared to N = 2 supersymmetric Yang-Mills theory in four dimensions through compactification on a circle of the latter. It is found that rational maps are appropriate to this comparison. A BPS mass formula is also written for particles in three dimensions and strings in four dimensions.
“…One way to construct this space is to consider its simply connected double cover and then mod by the cyclic symmetry of two monopoles -Z 2 . We will now describe a procedure due to Sutcliffe [16] which relates the spectral curves to the curves associated with d = 4 super Yang-Mills theory. We recall the spectral curve for two monopoles…”
The coulomb branch of N = 4 supersymmetric Yang-Mills gauge theories in d = 2 + 1 is studied. A direct connection between gauge theories and monopole moduli spaces is presented. It is proposed that the hyper-Kähler metric of supersymmetric N = 4 SU(N) Yang-Mills theory is given by the charge N centered moduli space of BPS monopoles in SU(2). The theory is compared to N = 2 supersymmetric Yang-Mills theory in four dimensions through compactification on a circle of the latter. It is found that rational maps are appropriate to this comparison. A BPS mass formula is also written for particles in three dimensions and strings in four dimensions.
“…It seems likely that this elliptic k = 2 solution corresponds to hyperbolic 2-monopoles with gauge group SU(2), via the Braam-Austin construction. More generally, for k > 2 one may speculate that discrete-Toda solutions correspond to hyperbolic k-monopoles with C k cyclic symmetry, since this is what happens for Euclidean monopoles (Sutcliffe 1996).…”
Section: Reduction To a Discrete Toda Systemmentioning
Monopoles on hyperbolic 3-space were introduced by Atiyah in 1984. This article describes two integrable systems which are closely related to hyperbolic monopoles: a one-dimensional lattice equation (the Braam-Austin or discrete Nahm equation), and a soliton system in (2+1)-dimensional anti-deSitter space-time.
“…Following [11] we can identify the world volume theory of strings as coming from 10d SYM theory via the dimensional reduction. Moreover there is one to one correspondence between the equation defining the ground state in the SUSY σ model and the Nahm equations describing the monopole moduli space.Finally to get the Toda equation in the brane terms we use the observation [12] that the spectral curve for SL(N,C) Toda system coincides with the one for the cyclic N-monopoles. The spectral curve for the cyclic N-monopole follows from the generic spectral curve…”
Section: Let Us Find Now the Interpretation Of The Equation Of Motionmentioning
We suggest the brane interpretation of the integrable dynamics behind the exact solution to the N=2 SUSY YM theory.Degrees of freedom of the Calogero type integrable system responsible for the appearance of the spectral Riemann surfaces originate from the collective coordinates of the dynamical branes. The second Whitham type integrable system corresponds to the low energy scattering of branes similar to the scattering of the magnetic monopoles.
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