Abstract¶
Details of the task of quantum state exclusion.
State Exclusion Overview¶
In a state exclusion task, a referee has a set of states and sends one state from the set, with probability , to a player. The player then performs a general outcome measurement on the state, as described by a positive operator-valued measure (POVM) , where and . From this measurement, the player outputs a label . The player wins the task if and fail if . 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 such that with certainty, this is conclusive 1-state exclusion. This occurs if the player is able to find a POVM such that
If the player gets the measurement outcome associated to , they output knowing with certainty the referee could not have sent .
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:
where is the probability of making an error when performing exclusion, meaning the probability of outputting the index .
k-State Exclusion¶
If the player outputs a set of labels, , such that with certainty, this is conclusive -state exclusion. There are different sets of labels the player could exclude, corresponding to all the different subsets of of length . Therefore, when performing -state exclusion the player aims to find a POVM with elements such that each measurement outcome allows the player to exclude a subset of states from of length .
k-State Exclusion as 1-State Exclusion¶
All -state exclusion tasks can be recast as 1-state exclusion tasks by reformulating the set Bandyopadhyay et al. (2014). Conceptually, this means all -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 be the set of all subsets of the integers of length . The player aims to measure a POVM on a state , given to them by the referee, and output a set of labels such that . Such a measurement will be a POVM with terms as there are subsets of of length . For each elements of this POVM, , the following equation must hold,
By defining
the -state exclusion task can be expressed as the following set of equations
This is now the same form as the 1-state exclusion task conditions. This is the dual 1-state exclusion task to the -state exclusion task.
Using the dual 1-state exclusion task, -state exclusion can also now be formulated as an SPD:
where if no POVM to conclusively perform -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, , such that is a channel. This collection is called a quantum instrument, and each map is called a sub-channel.
In sub-channel exclusion, a player has a reference state that they send to the referee. The referee then measures using the instrument and returns the post-measurement state to the player. The player measures a POVM on the state and outputs a label . 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 labels, , or they can output labels with certainty.
- 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
- Pusey, M. F., Barrett, J., & Rudolph, T. (2012). On the reality of the quantum state. Nature Physics, 8(6), 475–478. 10.1038/nphys2309
- Bandyopadhyay, S., Jain, R., Oppenheim, J., & Perry, C. (2014). Conclusive exclusion of quantum states. Physical Review A, 89(2). 10.1103/physreva.89.022336