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Postponing the choice: advantage of deferred measurements in quantum information processing

C. Carmeli, T. Heinosaari, A. Toigo

TL;DR

This work analyzes whether deferring the choice of a second quantum measurement can outperform fixed joint measurements or universal cloning. It develops a unified framework for three strategies—fixed joint meters, approximate cloning, and sequential measurements with deferred choices—under depolarizing noise and, in extended form, allows negative noise parameters. The authors derive exact compatibility regions (CR) for nonnegative noise and extended regions (ECR) for negative noise, showing that equivalences between strategies hold under certain conditions (e.g., MU bases or unbiasedness) but can fail for overnoisy devices, with explicit optimal joint devices provided at boundary points. The methodology relies on Weyl-Heisenberg covariance and symmetrization to obtain covariant joint instruments, yielding insights into the structure and limitations of deferred-measurement approaches with practical implications for quantum information processing where measurement freedom is constrained.

Abstract

Simultaneously implementing two arbitrary quantum measurements on the same system is impossible. The consequence of this limitation is that selecting one measurement actively excludes other possibilities. Two incompatible choices can then be forced together only at the cost of adding enough noise to the measurements. An intriguing alternative is to postpone the choice, or part of it, until a later stage. We explore the advantages of this deferred decision-making and discover that the benefits critically depends on the assumptions about the forthcoming choice. In certain scenarios postponing the choice introduces no additional cost, while in others partial postponement can be effectively the same as full postponement.

Postponing the choice: advantage of deferred measurements in quantum information processing

TL;DR

This work analyzes whether deferring the choice of a second quantum measurement can outperform fixed joint measurements or universal cloning. It develops a unified framework for three strategies—fixed joint meters, approximate cloning, and sequential measurements with deferred choices—under depolarizing noise and, in extended form, allows negative noise parameters. The authors derive exact compatibility regions (CR) for nonnegative noise and extended regions (ECR) for negative noise, showing that equivalences between strategies hold under certain conditions (e.g., MU bases or unbiasedness) but can fail for overnoisy devices, with explicit optimal joint devices provided at boundary points. The methodology relies on Weyl-Heisenberg covariance and symmetrization to obtain covariant joint instruments, yielding insights into the structure and limitations of deferred-measurement approaches with practical implications for quantum information processing where measurement freedom is constrained.

Abstract

Simultaneously implementing two arbitrary quantum measurements on the same system is impossible. The consequence of this limitation is that selecting one measurement actively excludes other possibilities. Two incompatible choices can then be forced together only at the cost of adding enough noise to the measurements. An intriguing alternative is to postpone the choice, or part of it, until a later stage. We explore the advantages of this deferred decision-making and discover that the benefits critically depends on the assumptions about the forthcoming choice. In certain scenarios postponing the choice introduces no additional cost, while in others partial postponement can be effectively the same as full postponement.

Paper Structure

This paper contains 13 sections, 9 theorems, 109 equations, 5 figures, 2 tables.

Key Result

Theorem 1

Suppose $(s,t)\in [0,1]\times [0,1]$.

Figures (5)

  • Figure 1: The three different scenarios compared in the present investigation: (a) the target meters are fixed in advance and their approximate joint meter is tailored accordingly; (b) neither of the target meters is fixed in advance, and each of them is measured in a different approximate clone of the original state; (c) only the first target meter is fixed in advance, while the second one is decided after a measurement of the first has been performed.
  • Figure 2: The set of points $(s,t)\in [0,1]\times [0,1]$ (green square) and the compatibility regions $\textrm{CR} (\mathsf{Q},\mathsf{P})$ and $\textrm{CR} (I,I)$ given by Theorem \ref{['thm:QP+II']} (blue areas) in dimension $d=3$. Lighter blue denotes the set difference $\textrm{CR} (\mathsf{Q},\mathsf{P})\setminus\textrm{CR} (I,I)$. Points of the orange (respectively, red) curve attain the equalities in \ref{['eq:QP_comp']} (resp., \ref{['eq:II_comp']}).
  • Figure 3: The set of all admissible points for the pair of identity channels $(I,I)$ (dark green square) compared with the analogue set for \ref{['fig:squares_1']} a pair of sharp meters $(\mathsf{Q},\mathsf{P})$; \ref{['fig:squares_2']} a pair $(\mathsf{Q},I)$ in which $\mathsf{Q}$ is a sharp meter and $I$ is the identity channel. The light green areas are the differences between the two compared sets.
  • Figure 4: The extended compatibility regions $\textrm{ECR} (\mathsf{Q},\mathsf{P})$ and $\textrm{ECR} (I,I)$ given by Theorem \ref{['thm:QP+II_neg']} (blue areas) inside the respective sets of admissible points (green squares) in dimensions $d=2,3$. The lighter blue area is the set difference $\textrm{ECR} (\mathsf{Q},\mathsf{P})\setminus\textrm{ECR} (I,I)$. Points of the orange (respectively, red) curve attain the equalities in \ref{['eq:QP_comp_neg_1']}, \ref{['eq:QP_comp_neg_2']} (resp., \ref{['eq:II_comp_neg']}). The isolated colored points still belong to the boundary of $\textrm{ECR} (\mathsf{Q},\mathsf{P})$ or $\textrm{ECR} (I,I)$. For each $k=1,2$, we also plotted the line $s+t=(d^k-3)/(d^k-1)$ and the arc of the ellipse \ref{['eq:poly']} which lies below it.
  • Figure 5: The extended compatibility region $\textrm{ECR} (\mathsf{Q},I)$ given by Theorem \ref{['thm:main_neg']} (blue area) inside the set of all admissible points for the pair $(\mathsf{Q},I)$ (green rectangle) in dimensions $d=2,3$. The lighter colors denote the sets $\textrm{ECR} (\mathsf{Q},I)\setminus\textrm{ECR} (I,I)$ and $[m_1,m_2]\times [m_2,1]$. Points of the red curve attain the equalities in \ref{['eq:QI_comp_neg']} and the point with coordinates $(m_1,m_2)$ is highlighted. Of the two lines which appear in both graphs, one has equation $s+t=(d^2-3)/(d^2-1)$, while the other one is $t-2s=1$ in graph \ref{['fig:comp_neg_QI_1']} and $t-(d/2)s=1$ in graph \ref{['fig:comp_neg_QI_2']}. We also plotted the arcs of the ellipses \ref{['eq:poly']} and \ref{['eq:poly_neg']} which lie below these lines.

Theorems & Definitions (13)

  • Theorem 1
  • Theorem 2
  • Theorem 3
  • Theorem 4
  • Lemma 1: Symmetrization trick
  • proof
  • proof : Proof of Theorems \ref{['thm:main']} and \ref{['thm:main_neg']}
  • Proposition 1
  • Proposition 2
  • Proposition 3
  • ...and 3 more