2021
DOI: 10.22331/q-2021-06-08-470
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The group structure of dynamical transformations between quantum reference frames

Abstract: Recently, it was shown that when reference frames are associated to quantum systems, the transformation laws between such quantum reference frames need to be modified to take into account the quantum and dynamical features of the reference frames. This led to a relational description of the phase space variables of the quantum system of which the quantum reference frames are part of. While such transformations were shown to be symmetries of the system's Hamiltonian, the question remained unanswered as to wheth… Show more

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Cited by 32 publications
(28 citation statements)
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“…• We elucidate why the perspective-neutral approach to quantum frame covariance, further developed here, is not in general equivalent to the purely perspective-dependent approaches [48,[65][66][67][68]71,72]. The latter start with a fixed subsystem Hilbert space in a given internal quantum frame perspective that is not in general compatible with gauge-invariance under the symmetry group.…”
Section: Summary Of the Resultsmentioning
confidence: 98%
See 2 more Smart Citations
“…• We elucidate why the perspective-neutral approach to quantum frame covariance, further developed here, is not in general equivalent to the purely perspective-dependent approaches [48,[65][66][67][68]71,72]. The latter start with a fixed subsystem Hilbert space in a given internal quantum frame perspective that is not in general compatible with gauge-invariance under the symmetry group.…”
Section: Summary Of the Resultsmentioning
confidence: 98%
“…The isomorphism maps the state |φ(e) R ∈ H i ⊗ H j , which is invariant under ρ i (g)⊗ρ j (g), to an element M φ(e) ∈ Hom( Hj , H i ) which is necessarily invariant under the action of g. This shows that the G-equivariant subspace Hom G ( Hj , H i ) of Hom( Hj , H i ) is non trivial, where the G-equivariant subspace is the space of all maps M ∈ Hom( Hj , H i ) such that ρ i (g)M = M ρj (g) for all g ∈ G. Due to the irreducibility of the representations involved, Schur's lemma entails that H j ∼ = Hi . For an irrep H i ⊗ H j ∼ = H i ⊗ Hi the specific form of |φ(e) i follows directly from the fact that M φ(e) ∈ Hom( Hj , H i ) ∼ = Hom(H i , H i ) is proportional to the identity matrix and applying the explicit isomorphism Hom(H i , H i ) → H i ⊗ Hi yields a state |φ(e) i of the form given in Equation (68). The extension to reducible representations requires Example 1.…”
Section: Left-right Systems Of Coherent Statesmentioning
confidence: 99%
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“…If spacetime is defined in terms of such quantum reference frames, then it inherits their quantum properties. While this statement still needs to be made more precise, and work on this is in progress, recent preliminary results showed that the associated symmetry group defining transformations between quantum reference frames is a more general group than that of Galilei symmetries [56].…”
Section: Discussionmentioning
confidence: 99%

Double Quantization

Gubitosi,
Lizzi,
Relancio
et al. 2021
Preprint
Self Cite
“…[29,30] extend the formalism to the special relativistic regime, applying it to concrete problems in Relativistic Quantum Information. Other works [31,32,33] have focussed on the group properties of QRFs both in discrete and in continuous-variable systems. A time version of QRFs, also related to the Page-Wootters mechanism [34,35], has been introduced in Ref.…”
Section: Introductionmentioning
confidence: 99%