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From worldline to quantum superconformal mechanics with/without oscillatorial terms: D(2,1;α)D(2,1;\alpha) and sl(2∣1)sl(2|1) models

I.E. Cunha; N.L. Holanda; F. Toppan

Dados da publicação

Autores
I.E. Cunha; N.L. Holanda; F. Toppan
Tipo
Nota de Física
Status
Publicado
Data de publicação
20/02/2017
Descrição
In this paper we quantize superconformal $\sigma$-models defined by worldline supermultiplets. \par Two types of superconformal mechanics, with and without a DFF term, are considered. \par Without a DFF term (Calogero potential only) the supersymmetry is unbroken. \par The models with a DFF term correspond to deformed (if the Calogero potential is present) or undeformed oscillators. For these (un)deformed oscillators the classical invariant superconformal algebra acts as a spectrum-generating algebra of the quantum theory.\par Besides the $osp(1|2)$ examples, we explicitly quantize the superconformally-invariant worldine $\sigma$-models defined by the ${\cal N}=4$ $(1,4,3)$ supermultiplet (with $D(2,1;\alpha)$ invariance, for $\alpha\neq 0,1$) and by the ${\cal N}=2$ $(2,2,0)$ supermultiplet (with two-dimensional target and $sl(2|1)$ invariance). The parameter $\alpha$ is the scaling dimension of the $(1,4,3)$ supermultiplet and, in the DFF case, has a direct interpretation as a vacuum energy. In the DFF case, for the $sl(2|1)$ models, the scaling dimension $\lambda$ is quantized (either $\lambda=\frac{1}{2}+{\mathbb Z}$ or $\lambda={\mathbb Z}$). The ordinary two-dimensional oscillator is recovered from $\lambda=-\frac{1}{2}$. The spectrum of the theory is decomposed into an infinite set of lowest weight representations of $sl(2|1)$. Surprisingly, extra fermionic raising operators, not belonging to $sl(2|1)$, allow to construct the whole spectrum from a single (for $\lambda=\frac{1}{2}+{\mathbb Z}$) bosonic vacuum.
Ano
2016
Número
CBPF-NF-006/16
Vínculo com tese
Não
Vínculo com bolsa
Não
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