The joint probability table shows same-bit correlation while each single bit remains uncertain. Exact arithmetic here means exact results for the stated model inputs; measured inputs still carry uncertainty and significant-figure limits.

highlighted = computed this step

Only two joint outcomes have probability

The joint measurement distribution has probability one half on zero-zero and one half on one-one. The crossed outcomes have probability zero.

outcomeP0,0120,101,001,112\begin{array}{c|c}\text{outcome}&P\\\lvert 0,0\rangle&\frac{1}{2}\\\lvert 0,1\rangle&0\\\lvert 1,0\rangle&0\\\lvert 1,1\rangle&\frac{1}{2}\end{array}
Bell correlationsThe entanglement table carries the same probabilities.001/sqrt(2)P=1/2010P=0100P=0111/sqrt(2)P=1/2det = 1/2not product

The bit values always match in this basis

Add the rows where the two bit values match. The same-bit probability is one, even though each individual bit is still uncertain.

Psame=12+12=1P_{\text{same}} = \frac{1}{2} + \frac{1}{2} = 1
Bell correlationsThe same-bit rows are the two nonzero cells.001/sqrt(2)P=1/2010P=0100P=0111/sqrt(2)P=1/2det = 1/2not product

The table separates joint and marginal facts

The joint table says both bits match. It does not say either single qubit had a known value before measurement.

outcomePsame?0,01210,1001,0001,1121\begin{array}{c|c|c}\text{outcome}&P&\text{same?}\\\lvert 0,0\rangle&\frac{1}{2}&1\\\lvert 0,1\rangle&0&0\\\lvert 1,0\rangle&0&0\\\lvert 1,1\rangle&\frac{1}{2}&1\end{array}
Bell correlationsThe displayed nonzero cells are exactly the same-bit rows.001/sqrt(2)P=1/2010P=0100P=0111/sqrt(2)P=1/2det = 1/2not product