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State Exclusion

Abstract

Details of the task of quantum state exclusion.

Keywords:State ExclusionState DiscriminationPOVMsgames.

State Exclusion Overview

In a state exclusion task, a referee has a set of states {ρx}N, x{1,,N}\{\rho_{x} \}^{N}, ~ x \in \{1, \ldots ,N\} and sends one state from the set, with probability pxp_{x}, to a player. The player then performs a general NN outcome measurement on the state, as described by a positive operator-valued measure (POVM) {Tg}g=1N\{T_{g}\}_{g=1}^{N}, where Tg0T_g\ge0 g\forall\,g and gTg=I\sum_gT_g=\mathbb{I}. From this measurement, the player outputs a label g{1,,N}g \in \{1, \ldots , N\}. The player wins the task if gxg \neq x and fail if g=xg=x. Namely, they win if they successfully exclude the state by outputting a label that was not associated to the sent state; the player fails if they output the label associated to the sent state (Caves et al. (2002), Pusey et al. (2012), Bandyopadhyay et al. (2014)).

1-State Exclusion

If the player outputs a single label gg such that gxg \neq x with certainty, this is conclusive 1-state exclusion. This occurs if the player is able to find a POVM such that

tr[Txρx]=0    x{1,,N}.\textrm{tr} \big[ T_{x}\rho_{x}] = 0 ~ ~ \forall ~~ x \in \{1, \ldots ,N\}.

If the player gets the measurement outcome associated to TgT_{g}, they output gg knowing with certainty the referee could not have sent ρg\rho_{g}.

In general, a POVM may not exists that can perform conclusive state exclusion. Instead, state exclusion can be performed with some error, as given by the following SPD:

min  Perr=gNtr[Tgρg]Subject to:  gNTg=I,  Tg0  g,\begin{align*} \min &~~ P_{err} = \sum^{N}_{g} \textrm{tr} \big[T_{g} \rho_{g}] \\ \textrm{Subject to:}& ~ ~ \sum^{N}_{g} T_{g} = \mathbb{I}, ~~ T_{g} \geq 0 ~ \forall ~ g, \end{align*}

where PerrP_{err} is the probability of making an error when performing exclusion, meaning the probability of outputting the index g=xg=x.

k-State Exclusion

If the player outputs a set of kk labels, {gi}k\{ g_{i} \}^{k}, such that gix  gi{gi}kg_{i} \neq x ~ \forall ~ g_{i} \in \{g_{i}\}^{k} with certainty, this is conclusive kk-state exclusion. There are (Nk)N \choose k different sets of kk labels the player could exclude, corresponding to all the different subsets of {1,,N}\{1,\ldots,N\} of length kk. Therefore, when performing kk-state exclusion the player aims to find a POVM with (Nk)N \choose k elements such that each measurement outcome allows the player to exclude a subset of states from {ρx}N\{\rho_{x} \}^{N} of length kk.

k-State Exclusion as 1-State Exclusion

All kk-state exclusion tasks can be recast as 1-state exclusion tasks by reformulating the set {ρx}N\{\rho_{x}\}^{N} Bandyopadhyay et al. (2014). Conceptually, this means all kk-state exclusion tasks have a 1-state exclusion task that they are dual to, allowing all state exclusion tasks to be studied under the 1-state exclusion framework.

Let Y(N,k)Y_{(N, k)} be the set of all subsets of the integers {1,2,...,N}\{1,2,...,N\} of length kk. The player aims to measure a POVM on a state σ{ρx}N\sigma \in \{ \rho_{x} \}^{N}, given to them by the referee, and output a set of labels YY(N,k)Y \in Y_{(N,k)} such that σ{ρy}yY\sigma \notin \{ \rho_{y} \}_{y \in Y}. Such a measurement will be a POVM with a=(Nk)a = {N \choose k} terms as there are aa subsets of {1,2,...,N}\{1,2,...,N\} of length kk. For each elements of this POVM, S={Sl}l=1aS = \{S_{l}\}^{a}_{l=1}, the following equation must hold,

tr[SYρy]=0  y  Y.\textrm{tr}\big[S_{Y}\rho_{y}] = 0 ~ \forall ~y~ \in~ Y.

By defining

ρY=yYρy,\rho_{Y} = \sum_{y \in Y} \rho_{y},

the kk-state exclusion task can be expressed as the following set of equations

tr[SYρY]=0  YY(N,K).\textrm{tr} \big[ S_{Y} \rho_{Y}] = 0 ~\forall~Y \in Y_{(N,K)}.

This is now the same form as the 1-state exclusion task conditions. This is the dual 1-state exclusion task to the kk-state exclusion task.

Using the dual 1-state exclusion task, kk-state exclusion can also now be formulated as an SPD:

min  Perrk=Ytr[SYρY]Subject to:  iNSi=I,  Si0  i,\begin{align*} \min & ~~ P^{k}_{err} = \sum_{Y} \textrm{tr}[S_{Y}\rho_{Y}] \\ \textrm{Subject to:}& ~ ~ \sum^{N}_{i} S_{i} = \mathbb{I}, ~~ S_{i} \geq 0 ~ \forall ~ i, \end{align*}

where Perrk>0P^{k}_{err} > 0 if no POVM to conclusively perform kk-state exclusion exists.

Sub-Channel Exclusion

A closely related task to state exclusion is sub-channel exclusion. Consider a collection of completely-positive trace non-increasing linear maps, Ψ={Ψx}x=1N\Psi = \{\Psi_{x}\}_{x=1}^N, such that x=1NΨx\sum_{x=1}^N \Psi_{x} is a channel. This collection is called a quantum instrument, and each map Ψx\Psi_{x} is called a sub-channel.

In sub-channel exclusion, a player has a reference state ρ\rho that they send to the referee. The referee then measures ρ \rho using the instrument and returns the post-measurement state to the player. The player measures a POVM on the state and outputs a label g{1,,N}g \in \{1, \ldots ,N\}. They succeed if they output a label of a sub-channel that was not applied. As before, the player can output the label of a sub-channel not applied with certainty, they can output kk labels, {gi}i=1k\{ g_{i} \}^{k}_{i=1}, or they can output kk labels with certainty.

References
  1. Caves, C. M., Fuchs, C. A., & Schack, R. (2002). Conditions for compatibility of quantum-state assignments. Physical Review A, 66(6). 10.1103/physreva.66.062111
  2. Pusey, M. F., Barrett, J., & Rudolph, T. (2012). On the reality of the quantum state. Nature Physics, 8(6), 475–478. 10.1038/nphys2309
  3. Bandyopadhyay, S., Jain, R., Oppenheim, J., & Perry, C. (2014). Conclusive exclusion of quantum states. Physical Review A, 89(2). 10.1103/physreva.89.022336