Simultaneous identification capacity of the qubit depolarizing channel without product-measurement restriction

Determine the simultaneous classical identification capacity of the qubit depolarizing channel under unrestricted decoding measurements (i.e., without imposing the complete product measurement constraint); establish whether this capacity equals the classical capacity C(N_p)=1−h(p/2); and ascertain whether entangled measurements can strictly improve identification rates over product measurements, including whether the capacity is achievable with product-state encodings and complete product measurements as in message transmission.

Background

The paper proves a matching achievability/converse for simultaneous identification over the qubit depolarizing channel when the decoder is restricted to complete product measurements, showing the capacity equals the classical capacity 1−h(p/2).

The authors highlight that this conclusion relies crucially on the product-measurement restriction and a reduction to a classical binary symmetric channel; for general (possibly entangled) measurements, such a reduction seems unavailable.

They note that in message transmission, King showed the depolarizing channel’s capacity is achieved with product-state inputs and product measurements, and ask whether an analogous statement holds for identification. They observe that even for two channel uses, while Bell measurements do not help, some partially/asymmetrically entangled measurements yield output distributions outside those of complete product measurements, leaving open whether entanglement can help.

References

The most important question stemming from our work is the following: Can one evaluate the simultaneous identification capacity of the qubit depolarizing channel without imposing the restriction of complete product measurements? Is the capacity in this case also equal to the classical capacity of the channel? In particular, can entangled measurements improve identification rates? In the case of message transmission, King showed that the capacity of the depolarizing channel is achievable using product-state inputs and complete product measurements. Whether an analogous statement holds for identification remains an important open question.

Strong converse bounds on the classical identification capacity of the qubit depolarizing channel  (2603.29987 - Ye et al., 31 Mar 2026) in Section 7: Summary and Open Questions