Three coupling inputs show where the product-state determinant crosses the boundary. Exact arithmetic here means exact results for the stated model inputs; measured inputs still carry uncertainty and significant-figure limits.

highlighted = computed this step

Uncoupled plus-plus stays product

The off row keeps four equal probabilities. Its determinant magnitude is 0.

det=0,n=0|\det|=0,\quad n=0
Uncoupled source rowThe product flag follows the zero determinant.state1/2 zerozero1/2 zeroone1/2 onezero1/2 oneonestate1/2 zerozero1/2 zeroone1/2 onezero1/2 oneoneIuncoupled001/2P=1/4011/2P=1/4101/2P=1/4111/2P=1/4det = 0

Two CNOT inputs cross the determinant boundary

The two coupled rows use different target inputs, but both make a nonzero determinant magnitude.

rowdetnoff00zero121one121\begin{array}{c|c|c}\text{row}&|\det|&n\\\text{off}&0&0\\\text{zero}&\frac{1}{2}&1\\\text{one}&\frac{1}{2}&1\\\end{array}
CNOT target-zero rowThe middle row renders the first non-product case.state1/sqrt(2) zerozero0 zeroone1/sqrt(2) onezero0 oneonestate1/sqrt(2) zerozero0 zeroone0 onezero1/sqrt(2) oneoneCNOTcouple001/sqrt(2)P=1/2010P=0100P=0111/sqrt(2)P=1/2det = 1/2not product

The target-one row is a separate checked input

Changing the target input does not reuse a caption. The CNOT row is checked again from its own source state.

det=12,n=1|\det|=\frac{1}{2},\quad n=1
CNOT target-one rowThe final row renders its own checked table.state0 zerozero1/sqrt(2) zeroone0 onezero1/sqrt(2) oneonestate0 zerozero1/sqrt(2) zeroone1/sqrt(2) onezero0 oneoneCNOTcouple000P=0011/sqrt(2)P=1/2101/sqrt(2)P=1/2110P=0det = -1/2not product