Characterize the computational boundary for correlated thermal baths

Derive an analogue of the local calibration parameter \(\chi_{\max}\) that characterizes computational simulability and resource generation for general correlated thermal baths, beyond the independent local Markov-bath setting.

Background

The paper establishes an exact computational boundary, expressed through the maximum local parameter χi=(1pe(i))T2(i)/T1(i)1\chi_i=(1-p_e^{(i)})T_2^{(i)}/T_1^{(i)}-1, for independent local Markov baths. In that setting, nonpositive values at every location guarantee efficient classical simulation of all monitored branches, whereas a positive value at one repeatedly accessible location enables universal quantum computation.

The authors note that correlations between qubits sharing a common thermal bath can generate a positive short-time resource margin even when every local χi\chi_i is nonpositive. Consequently, the local parameters T1T_1, T2T_2, and pep_e do not capture the collective computational resource, motivating a characterization of the appropriate boundary for general correlated baths.

References

Local values of $T_1$, $T_2$, and $p_e$, defined from the diagonal rates and local dephasing, do not reveal this collective route, and no analogue of $chi_{\max}$ is known for general correlated baths.

Environmental records unlock universal quantum computation from thermal decoherence  (2609.16460 - Cao et al., 15 Sep 2026) in Discussion and outlook