Construction of Metaplectic Representations of $$SL_2(\mathbb {Z}_{2^n})$$ and Twisted Magnetic Translations

Unitary metaplectic representations of the group $$\varvec{SL}_{\textbf{2}}(\mathbb {Z}_{\textbf{2}^{\varvec{n}}})$$ are necessary to describe the time evolution of $$\textbf{2}^{\varvec{n}}$$ -dimensional quantum systems, such as systems involving n qubits. It is shown that in order for the metaplectic property to be fulfilled, an increase in the dimensionality of the involved n-qubit Hilbert spaces, from $$\textbf{2}^{\varvec{n}}$$ to $$\textbf{2}^{\textbf{2}{\varvec{n}}}$$ , is necessary. Thus we construct the general matrix form of such representations based on the magnetic translations of the diagonal subgroup $$\varvec{HW}_{\textbf{2}{\varvec{n}}} \otimes \varvec{HW}_{\textbf{2}{\varvec{n}}}$$ . Comparisson with other approaches on this problem of the literature are discussed.

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Publication Details

Journal
International Journal of Theoretical Physics
Published
2025-10-27
DOI
https://doi.org/10.1007/s10773-025-06103-5
Primary Topic
Advanced Topics in Algebra
Type
article
Field-Weighted Citation Impact
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article

Construction of Metaplectic Representations of $$SL_2(\mathbb {Z}_{2^n})$$ and Twisted Magnetic Translations

E. Floratos, I. Tsohantjis, Kimon Manolas
International Journal of Theoretical Physics
Advanced Topics in Algebra
article

Construction of Metaplectic Representations of $$SL_2(\mathbb {Z}_{2^n})$$ and Twisted Magnetic Translations

E. Floratos, I. Tsohantjis, Kimon Manolas
article en

Abstract

Unitary metaplectic representations of the group $$\varvec{SL}_{\textbf{2}}(\mathbb {Z}_{\textbf{2}^{\varvec{n}}})$$ are necessary to describe the time evolution of $$\textbf{2}^{\varvec{n}}$$ -dimensional quantum systems, such as systems involving n qubits. It is shown that in order for the metaplectic property to be fulfilled, an increase in the dimensionality of the involved n-qubit Hilbert spaces, from $$\textbf{2}^{\varvec{n}}$$ to $$\textbf{2}^{\textbf{2}{\varvec{n}}}$$ , is necessary. Thus we construct the general matrix form of such representations based on the magnetic translations of the diagonal subgroup $$\varvec{HW}_{\textbf{2}{\varvec{n}}} \otimes \varvec{HW}_{\textbf{2}{\varvec{n}}}$$ . Comparisson with other approaches on this problem of the literature are discussed.

International Journal of Theoretical PhysicsVol. 64(11)
National and Kapodistrian University of Athens (GR), Academy of Athens (GR)
Openalex Percentile: Top 62%
Advanced Topics in Algebra
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