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**Nota de Física****Publicado**

# **A three-dimensional superconformal quantum mechanics with **sl(2∣1)sl(2|1)sl(2∣1)** dynamical symmetry**

**Ivan E. Cunha**

21/08/2019

[**Descargar PDF **1 MB](https://index.cbpf.br/files/publicacao/6ad2a767639f62b11adbd022/pdf) [**Contactar al responsable**](<mailto:toppan@cbpf.br?subject=A%20three-dimensional%20superconformal%20quantum%20mechanics%20with%20sl(2%7C1)%20dynamical%20symmetry>)

## **Datos de la publicación**

<dl>

<dt>Autores</dt>
<dd>Ivan E. Cunha</dd>

<dt>Tipo</dt>
<dd>Nota de Física</dd>

<dt>Estado</dt>
<dd>Publicado</dd>

<dt>Fecha de publicación</dt>
<dd>21/08/2019</dd>

<dt>Descripción</dt>
<dd>We construct a three-dimensional superconformal quantum mechanics (and its associated de Alfaro-Fubini-Furlan deformed oscillator) possessing an $sl(2|1)$ dynamical symmetry. At a coupling parameter $\beta\neq 0$ the Hamiltonian contains a $\frac{1}{r^2}$ potential and a spin-orbit (hence, a first-order differential operator) interacting term. At $\beta=0$ four copies of undeformed three-dimensional oscillators are recovered. The Hamiltonian gets diagonalized in each sector of total $j$ and orbital $l$ angular momentum (the spin of the system is $\frac{1}{2}$). The Hilbert space of the deformed oscillator is given by a direct sum of $sl(2|1)$ lowest weight representations. The selection of the admissible Hilbert spaces at given values of the coupling constant $\beta$ is discussed. The spectrum of the model is computed. The vacuum energy (as a function of $\beta$) consists of a recursive zigzag pattern. The degeneracy of the energy eigenvalues grows linearly up to $E\sim \beta$ (in proper units) and quadratically for $E&gt;\beta$. The orthonormal energy eigenstates are expressed in terms of the associated Laguerre polynomials and the spin spherical harmonics. The dimensional reduction of the model to $d=2$ produces two copies (for $\beta$ and $-\beta$, respectively) of the two-dimensional $sl(2|1)$ deformed oscillator. The dimensional reduction to $d=1$ produces the one-dimensional $D(2,1;\alpha)$ deformed oscillator, with $\alpha$ determined by $\beta$.</dd>

<dt>Año</dt>
<dd>2019</dd>

<dt>Número</dt>
<dd>CBPF-NF-002/19</dd>

<dt>Vínculo con tesis</dt>
<dd>No</dd>

<dt>Vínculo con beca</dt>
<dd>No</dd>

</dl>

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