Detector efficiency moves clicked counts across a floor. Exact arithmetic here means exact results for the stated model inputs; measured inputs still carry uncertainty and significant-figure limits.

highlighted = computed this step

Detector clicks must meet a count floor

Arriving photons stay fixed while the efficiency gate changes.

m=NclickNminm=N_{\text{click}}-N_{\min}
Below click floorHalf efficiency is below the floor.1/2clicked1/2misseddetector

Three efficiencies bracket the click floor

Two-thirds efficiency exactly meets the click floor; three-quarters passes it.

ηNclickmgate1262fail2380pass3491pass\begin{array}{c|c|c|c}\eta&N_{\text{click}}&m&\text{gate}\\\frac{1}{2}&6&-2&\text{fail}\\\frac{2}{3}&8&0&\text{pass}\\\frac{3}{4}&9&1&\text{pass}\\\end{array}
Click-floor boundaryThe middle row exactly reaches the floor.2/3clicked1/3misseddetector

The high-efficiency row clears the floor

Clicked plus missed still closes the arrival ledger.

m=1passm=1\quad \text{pass}
Above click floorThe high-efficiency detector clears the floor.3/4clicked1/4misseddetector