Abstract

An amplification reaction may become sensitive enough only after its background-positive probability has already exceeded the permitted limit. We study this timing conflict for an explicit finite-resource birth–immigration source: zz active units grow at rate (b+gz)(1z/R)(b+gz)(1-z/R) until an aggregate detection threshold hh is reached, a blank starts empty, and a loaded reaction starts with a Poisson number of units. A deadline is acceptable when the blank-positive probability is at most 1%1\% and the missed-call probability at most 5%5\%. At threshold five, Poisson mean four, b=0.01b=0.01 and g=1g=1 per minute, capacities five, six and seven admit no acceptable deadline at all, capacity eight admits one but none on a 0.10.1-minute observation grid, and capacity nine is the least grid-feasible capacity. Capacity ten is feasible at every deadline in [3.15,3.30][3.15,3.30] minutes, and remains feasible for every fixed rate vector within 2%2\% of nominal, every loading mean at least 3.993.99 and every actual deadline in [3.19,3.21][3.19,3.21] minutes. These statements, including the source law, the monotonicity arguments and the rational exponential enclosures, are verified in Lean 4. A uniform rescaling of all rates cannot create a window; a state-dependent resource change can. We then analyse arbitrarily large thresholds through the independent holding times of the count chain and the beta–gamma algebra. If the capacity exceeds the threshold by a margin that grows without bound, depletion becomes a common additive delay and the undepleted design rules apply after re-centering. If the margin is a fixed number mm of units, the last births near exhaustion add an independent Gamma(m+1)\mathop{\mathrm{Gamma}}(m+1) delay in logarithmic time, and the limiting error tradeoff depends only on b/gb/g, the loading mean and mm: with these parameters, at most two units of headroom leave no window, three or more do. For every threshold h108h\ge10^{8} we prove, with explicit constants and without any hh-state computation, that capacity hh has no acceptable deadline while capacity 2h2h has one at an explicit time; the certified instances at threshold five are therefore not an artefact of small counts or of reactions that are positive at time zero. Numerical Laplace inversion at h=108h=10^{8} confirms the bounds. The large-threshold results are conventional proofs and are identified as such. The model is an effective one; no clinical calibration or specific molecular capacity intervention is established.