Preprint
How gently can a protected quantum memory be read? Rate limits on logical readout from the structure of the code
Dylan HendersoniD
Cogitan, Coppell, Texas, USA
August 21, 2026 · 10.5281/zenodo.21971432
Abstract
Quantum error-correcting codes protect logical information by hiding it from the environment; yet the same information must remain accessible to the experimenter. We quantify this tension for weak continuous readout of bosonic codes, to leading order in the measurement rate and in the single-mode Markovian limit. Reading a logical observable through a physical meter M at strength γ induces a logical decoherence that separates into two channels of distinct origin: a conjugate cost, dephasing of the partner logical operators, bounded below by the information-gain rate and saturating it for quantum-limited readouts; and a self cost, corruption of the very operator being read. Our central result is that the self cost is set by the structure of the code. Within the code space this is an exact operator identity, Γ_self ≥ 2γκ², nonperturbative in the within-codespace off-diagonal action κ of M and free of further hypotheses. A second and weaker contribution follows from the Knill–Laflamme residual of the back-action E = P⊥MP: leakage the code cannot correct forces any recovery, at any speed, to confuse the logical states, giving Γ_self ≥ ½γε²_KL. Together, Γ_self ≥ γ max(2κ², ½ε²_KL) − O(γ²/g) — the readability limit. The second term is a recovery-independent converse established as a rate at d = 2 for direct-return stabilizers and supported numerically beyond them; it saturates where the within-code term dominates and is loose by up to a factor of ~300 where it does not. The which-path part of the residual, by contrast, feeds only the conjugate cost. We verify both terms cell by cell across cat and Gottesman–Kitaev–Preskill (GKP) codes and map the readability–protection trade-off across the GKP lattice family; number-type codes, within the Hermitian meter menu considered here, are essentially unreadable-while-protected. The canonical phase measurement conventionally used to read number-phase codes is a POVM and lies outside this framework; whether the bound extends to POVM meters is left open. The consequence is that readout quality becomes a code-design objective: engineer the logical readout so that its back-action is an error the code already corrects — achieved exactly by symmetry for the cat parity readout, and to the controlled leading order for tuned modular meters.
Calculator
The readability limit for your own code and meter.
Your code's readability limit in a few seconds. Pick the code and the meter that reads it. Everything runs in your browser; nothing is sent anywhere.
Code
Its logical |0⟩ and |1⟩, in the basis you read
Meter
The Hermitian observable M you monitor
Optional: absolute rate, regime check, Fock cutoff+
Your limit
Γself ≥ 3.82 × 10⁻³ γ
The within-code term sets the limit: the meter rotates the logical state inside the code space. Its constant is exact, and in the paper's numerics, cells where it sets the rate sit within about 6% of it.
Within-code term · 2κ²
sets the limit3.82 × 10⁻³
exact operator identity
Knill–Laflamme term · ½εKL2
3.63 × 10⁻³
recovery-independent converse
All quantities+
- κ
- 0.0437
- |⟨0|M|1⟩|, the meter's action inside the code
- εKL2
- 7.25 × 10⁻³
- |Λ₀₁|² / Tr Λ, the uncorrectable part of the back-action
- 2κ² + ½εKL2
- 7.45 × 10⁻³
- additive form, leading order (direct-return stabilizers)
- ε0, ε1
- 0.706, 0.708
- leak amplitudes ‖E|μ⟩‖
- |Λ01|
- 0.0852
- overlap of the two leaked states
- Δm
- 3.9
- pointer shift ⟨0|M|0⟩ − ⟨1|M|1⟩
- Γconj / γ ≥
- 7.6
- conjugate cost Δm²/2, equal for a quantum-limited readout
- readability 𝒫 ≤
- 3980
- signal γΔm² over the self cost; compare within one meter type
- meter norm m
- 2.93
- on Fock levels n ≤ 7 (99.9% of the code)
- Fock cutoff
- 40
- converged to better than 10⁻⁶
What this covers
As in the paper: a logical qubit, Hermitian meters, weak continuous readout to leading order in γ/g, single mode, Markovian. The 2κ² term is an exact operator identity. The εKL term is a recovery-independent converse, proven for direct-return stabilizers and supported numerically beyond them; where it binds alone it can be loose by up to a factor of ~300. Canonical phase measurement is a POVM and is outside the framework. Computed in a truncated Fock basis, as the paper's code release does; it reproduces all twelve (code, meter) cells of the paper's bound table.
Cite this
If you use the calculator or the bound in your research, please cite the paper:
Henderson, D. (2026). How gently can a protected quantum memory be read? Rate limits on logical readout from the structure of the code. Zenodo. https://doi.org/10.5281/zenodo.21971432
@misc{henderson2026gently,
author = {Henderson, Dylan},
title = {How gently can a protected quantum memory be read? {Rate} limits on logical readout from the structure of the code},
year = {2026},
publisher = {Zenodo},
doi = {10.5281/zenodo.21971432},
url = {https://doi.org/10.5281/zenodo.21971432},
note = {Preprint}
}Where it stops
Leading order in the measurement rate, single-mode Markovian limit, and the framework cannot express canonical phase measurement — which is how number-phase codes are conventionally read.
The programme
Readout limits
How gently can a protected quantum memory be read, and what does that cost?