--- id: QuantumStandardQuantumLimit language: en section: quantum-physics source: Verification/QuantumStandardQuantumLimit.lean source_sha256: 408f63ff00145bc26d53a998b38c623f85feb98e2584afcc940d28ac8a688aac novelty: not-assessed status: reviewed --- # QuantumStandardQuantumLimit [Section](../quantum-physics/README.md) · [Lean](../../Verification/QuantumStandardQuantumLimit.lean) ## Scalar model and exact minimum In namespace `QuantumStandardQuantumLimit`, the prescribed real-valued expression is \[ V(I)=\operatorname{noiseVariance}(A,B,I)=\frac{A}{I}+BI, \qquad A>0,\quad B>0,\quad I>0. \] The names suggest measurement imprecision and back-action contributions as a function of intensity. The definition itself is scalar algebra: it introduces no random variables, stochastic processes, probability measure, variance operator, or covariance. Omitting a correlation term is an external modeling choice implicit in the formula, not a proved independence or zero-covariance fact. The exact identity \[ V(I)-2\sqrt{AB}=\frac{(\sqrt A-I\sqrt B)^2}{I} \] proves the nonstrict bound \(V(I)\ge 2\sqrt{AB}\). The unique positive optimizer is \(I_*=\sqrt{A/B}\), where the two contributions balance: \(A/I_*=BI_*\). The bound is attained at \(I_*\) and is strict for every other positive intensity. Positivity assumptions are essential to this stated domain; the definition also accepts other real arguments, but these theorems do not certify those cases. ## Conditional SQL-shaped bounds The physical parameters `hbar`, `m`, and `omega_m` are additional positive real numbers. Assuming the calibration inequality \[ \left(\frac{\hbar}{2m\omega_m}\right)^2\le AB, \] the module proves \[ \frac{\hbar}{m\omega_m}\le V(I),\qquad \sqrt{\frac{\hbar}{m\omega_m}}\le\sqrt{V(I)}. \] This calibration is a hypothesis, not a consequence of a formalized Heisenberg uncertainty relation or commutation relation. The square-root conclusion follows by monotonicity of `Real.sqrt`; its interpretation as a standard deviation needs the external variance interpretation of \(V\). The attained algebraic minimum is \(2\sqrt{AB}\); the possibly smaller calibrated bound is not asserted to be attained. Equality in the calibrated bound additionally requires saturation of the calibration inequality. ## Proof entry points All names below belong to `QuantumStandardQuantumLimit`. | Declaration | Result | | --- | --- | | `noiseVariance_gap_identity` | Exact square remainder for positive `A`, `B`, `I`. | | `noiseVariance_lower_bound` | Nonstrict lower bound `2 * Real.sqrt (A * B)`. | | `optimum_intensity_pos` | Positivity of `Real.sqrt (A / B)`. | | `noiseVariance_balance_at_optimum` | Equality of the two contributions at the optimizer. | | `noiseVariance_optimum_value` | Attainment of the algebraic lower bound. | | `noiseVariance_unique_min` | Equality holds exactly at `I = Real.sqrt (A / B)`. | | `noiseVariance_strict_away` | Strict bound when positive `I` differs from the optimizer. | | `sql_variance_bound` | Calibrated variance bound under all positivity and calibration hypotheses. | | `sql_standard_deviation_bound` | Square-root form under the same hypotheses. | `QuantumSQLFormalSuite` packages the gap, lower bound, attainment, balance, uniqueness, and two calibrated conclusions; `quantum_sql_master_suite` supplies its proof. There are no direct imports from other `Verification` modules. Dependencies are Mathlib real arithmetic, square roots, and algebraic tactics. ## Physical scope and use The reusable result is an exact optimization certificate for a supplied inverse-plus-linear noise model. Applying it to a detector requires justifying the formula, parameter units, positivity, and calibration for that detector. There is no Langevin equation, spectral-density model, susceptibility, noise filter, measurement bandwidth, or conversion of spectra to integrated variance. No hardware or simulator validation, device certification, or universal limit for all quantum measurement schemes follows. For physical context, [Clerk et al., *Introduction to quantum noise, measurement, and amplification* (2010), Sec. III.B, Eqs. (3.57)–(3.59), and Sec. V.E](https://clerkgroup.uchicago.edu/PDFfiles/RMP2010.pdf) discuss imprecision/back-action optimization using noise spectra and the role of correlations. Those spectral quantities are not identified with this module's scalar variance by a formal theorem. The reference supplies context, not a derivation of the calibration hypothesis. Scientific and formalization priority have not been assessed. ## Verification The module passed `verify`, `audit`, and integration as `QuantumPhysicsFullSuite.standard_quantum_limit`. Strict build, `verify-all`, independent axiom audit, the public regression tests without skips, and catalog checks passed. A compiler regression checks an asymmetric optimum, tight calibration, and counterexamples outside the hypotheses. See the [validation record](../VERIFICATION.en.md).