2021
DOI: 10.1007/978-3-030-80209-7_17
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Group Actions and Monotone Metric Tensors: The Qubit Case

Abstract: In recent works, a link between group actions and information metrics on the space of faithful quantum states has been highlighted in particular cases. In this contribution, we give a complete discussion of this instance for the particular case of the qubit.

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Cited by 3 publications
(17 citation statements)
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“…From the results in [17] we know that there are at least 3 monotone metric tensors for which this construction is possible for any finite-level quantum system. Moreover, from the results in [21] we know that in the case of a two-level quantum systems, the Lie groups GL(H) and T * U(H) are the only Lie groups for which the construction described above is actually possible. Here, we want to understand if the group actions of GL(H) and T * U(H) found in [21] can be extended from a 2-level quantum system to a system with an arbitrary, albeit finite, number of levels.…”
Section: Lie Groups and Monotone Quantum Metric Tensorsmentioning
confidence: 99%
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“…From the results in [17] we know that there are at least 3 monotone metric tensors for which this construction is possible for any finite-level quantum system. Moreover, from the results in [21] we know that in the case of a two-level quantum systems, the Lie groups GL(H) and T * U(H) are the only Lie groups for which the construction described above is actually possible. Here, we want to understand if the group actions of GL(H) and T * U(H) found in [21] can be extended from a 2-level quantum system to a system with an arbitrary, albeit finite, number of levels.…”
Section: Lie Groups and Monotone Quantum Metric Tensorsmentioning
confidence: 99%
“…At this purpose, it is important to recall all those properties, shared by GL(H) and T * U(H) and by their actions, that are at the heart of the results of [17,21]. First of all, both GL(H) and T * U(H) contain the Lie group U(H) as a Lie subgroup, and contain the elements λI with λ > 0 and I the identity operator on H. Then, all the (transitive) actions of both GL(H) and T * U(H) on S (H) appearing in the analysis of [17,21] arise as a sort of normalization of suitable (transitive) actions on P(H). Specifically, if G denotes either GL(H) or T * U(H), then every G-action δ on S (H) can be written as…”
Section: Lie Groups and Monotone Quantum Metric Tensorsmentioning
confidence: 99%
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