Abstract:The implications of N = 1 superconformal symmetry for four dimensional quantum field theories are studied. Superconformal covariant expressions for two and three point functions of quasi-primary superfields of arbitrary spin are found and connected with the operator product expansion. The general formulae are specialised to cases involving a scalar superfield L, which contains global symmetry currents, and the supercurrent, which contains the energy momentum tensor, and the consequences of superconformal Ward … Show more
“…However the enlarged symmetry group of a SCFT imposes additional constraints. In particular, J I and T µ become primary operators and their three-point function T µ (z 2 )T ν (z 3 )J I (z 1 ) is uniquely determined up to an overall constant by superconformal symmetry [60]. This immediately implies that Tr(RRF I ) and Tr(F I ) are proportional to each other, with a constant that's universal for any SCFT.…”
A simple explanation of the flavor hierarchies can arise if matter fields interact with a conformal sector and different generations have different anomalous dimensions under the CFT. However, in the original study by Nelson and Strassler many supersymmetric models of this type were considered to be 'incalculable' because the R-charges were not sufficiently constrained by the superpotential. We point out that nearly all such models are calculable with the use of a-maximization. Utilizing this, we construct the simplest vector-like flavor models and discuss their viability. A significant constraint on these models comes from requiring that the visible gauge couplings remain perturbative throughout the conformal window needed to generate the hierarchies. However, we find that there is a small class of simple flavor models that can evade this bound.
“…However the enlarged symmetry group of a SCFT imposes additional constraints. In particular, J I and T µ become primary operators and their three-point function T µ (z 2 )T ν (z 3 )J I (z 1 ) is uniquely determined up to an overall constant by superconformal symmetry [60]. This immediately implies that Tr(RRF I ) and Tr(F I ) are proportional to each other, with a constant that's universal for any SCFT.…”
A simple explanation of the flavor hierarchies can arise if matter fields interact with a conformal sector and different generations have different anomalous dimensions under the CFT. However, in the original study by Nelson and Strassler many supersymmetric models of this type were considered to be 'incalculable' because the R-charges were not sufficiently constrained by the superpotential. We point out that nearly all such models are calculable with the use of a-maximization. Utilizing this, we construct the simplest vector-like flavor models and discuss their viability. A significant constraint on these models comes from requiring that the visible gauge couplings remain perturbative throughout the conformal window needed to generate the hierarchies. However, we find that there is a small class of simple flavor models that can evade this bound.
“…Starting from the expressions of [18], where soft parameters are expressed in terms of two-point functions of hidden-sector operators, we will show, utilizing the general formalism of [24], that the approximate superconformal symmetry provides powerful constraints on the form of such terms. Our strategy is to use the (kinematically constrained) form of three-point functions in N = 1 superconformal theories to extract the OPE of the first two operators with the third.…”
We develop a systematic and general approach to study the effective Higgs Lagrangian in a supersymmetric framework in which the Higgs fields in the visible sector couple weakly to another sector. The extra sector may be strongly coupled in general. It is assumed to be superconformal in the ultraviolet, but develop a mass-gap with supersymmetry breaking in the infrared. The main technique used in our approach is that of the operator product expansion (OPE). By using OPE methods we are able to compute the parameters in the Higgs Lagrangian to quadratic order and make general statements that are applicable to many classes of models. Not only does this approach allow us to understand the traditional problems plaguing simple models from a different perspective, it also reveals new possibilities for solutions of these problems. The methods and results of our work should be useful in constructing a viable and natural model of physics beyond the Standard Model.
“…These relations define a projective multiplet, following the four-dimensional terminology [9]. Associated with φ(z, w) is its smile-conjugateφ 34) which is also a projective multiplet. Ifφ(z, w) = φ(z, w), the projective superfield is called real.…”
“…The concept of superconformal Killing vectors [28,29,30,31,32,21,33], has proved to be extremely useful for various studies of superconformal theories in four and six dimensions, see e.g. [34,35,36]. This paper is organized as follows.…”
Within the supertwistor approach, we analyse the superconformal structure of 4D N = 2 compactified harmonic/projective superspace. In the case of 5D superconformal symmetry, we derive the superconformal Killing vectors and related building blocks which emerge in the transformation laws of primary superfields. Various off-shell superconformal multiplets are presented both in 5D harmonic and projective superspaces, including the so-called tropical (vector) multiplet and polar (hyper)multiplet. Families of superconformal actions are described both in the 5D harmonic and projective superspace settings. We also present examples of 5D superconformal theories with gauged central charge.
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