Dice Question Streamline Icon: https://streamlinehq.com

Finiteness criterion for the invariant algebra of system plus quantum reference frame

Determine a necessary and sufficient condition, ideally expressed in terms of the spectral multiplicity function m_{U_R} of the compactly stabilised quantum reference frame (U_R, E, H_R), that characterizes precisely when the invariant von Neumann algebra (M_S ⊗ B(H_R))^{Ad(U_S ⊗ U_R)} is finite for a general symmetry group G = ℝ × H with H compact and a faithful normal KMS state on M_S at inverse temperature β. In particular, ascertain whether the integrability condition ∫_ℝ e^{−β ξ} m_{U_R}(ξ) dξ < ∞ is also necessary, or identify the exact criterion that holds beyond the sufficiency established in Theorem \ref{thm:type_change}.

Information Square Streamline Icon: https://streamlinehq.com

Background

The paper proves that the invariant algebra of system and quantum reference frame observables, (M_S ⊗ B(H_R)){Ad(U_S ⊗ U_R)}, is semifinite under natural assumptions, and finite under a sufficient condition involving the spectral multiplicity function m_{U_R} of the quantum reference frame: ∫ℝ e{−β ξ} m{U_R}(ξ) dξ < ∞. This condition has a physical interpretation in terms of the thermal properties of the quantum reference frame and is analogous to nuclearity conditions in quantum field theory.

However, the authors only establish sufficiency of this condition in the general setting. They note that, outside a special case (trivial H and M_S a type III₁ factor) where necessity holds, the algebra need not be a factor and multiple traces may exist, leaving open whether the given integrability condition is necessary or whether a sharper, necessary-and-sufficient criterion can be formulated.

References

"It should be noted that we only prove that Eq. eq:type_change_condition is a sufficient condition for finiteness of the algebra of invariants, but in general not a necessary one. This is due to the fact that in general one does not expect (M_S\otimes B(H_R)){\Ad(U_S\otimes U_R)} to be a factor. Hence, even though by the theorem above this algebra is semifinite and the trace constructed in the proof is a semifinite trace, it need not be a unique trace (up to rescaling) on this algebra. Therefore, even when this trace is not in fact finite, that does not mean that no trace on this algebra can be a finite trace. It is therefore conceivable that, even when Eq. eq:type_change_condition is not satisfied, the algebra of invariant operators may still be a finite von Neumann algebra. While we do not rule out the possibility of formulating a sufficient and necessary condition of a similar nature to Eq. eq:type_change_condition, we shall leave this open for now."

Quantum reference frames, measurement schemes and the type of local algebras in quantum field theory (2403.11973 - Fewster et al., 18 Mar 2024) in Section 5.2 (Type reduction for invariant operators), after Theorem \ref{thm:type_change}