4 ms·
Yup, that solution also works. I completely missed it. It's even a bit more flexible, in that the A-to-Receiver edge could be flipped or turned into a broadcast
by Strilanc 11y ago
Yup, that solution also works. I completely missed it. It's even a bit more flexible, in that the A-to-Receiver edge could be flipped or turned into a broadcast-from-third-party without breaking the solution.
I did generate the puzzle by trying to find a network that forced the superdense bell pair coding + cleanup, so it's a bit embarassing that there's another solution. Maybe it's just always possible to flip the cleanup into an intermediate decoding and re-encoding.
As for the rendering: do you use noscript? The latex is rendered with mathjax. I put a note at the top of the page when scripts are disabled... but it might fail to show up in some cases. Knowing those cases would be useful (maybe if you unblocked the blog but not the mathjax cdn?).
- amluto 11y agoI'm using plain ol' Firefox on Linux. I just refreshed and it rendered correctly. Go figure. I'll try to find some time this afternoon to re-read the flat coding thing now that the math is there. But I'm a bit confused -- if I have a one-qubit state that's restricted to the set of states that are linear combinations of ±|0> ± |1>, then are only two such states up to global phase, and those states are orthogonal, so I can just measure without loss and treat it as a classical bit. Am I missing something? It's a neat puzzle, though, and I imagine that there are variants with very interesting solutions.
- Strilanc 11y ago> if I have a one-qubit state that's restricted to the set of states that are linear combinations of ±|0> ± |1>, then are only two such states up to global phase, and those states are orthogonal, so I can just measure without loss and treat it as a classical bit. Am I missing something? It's not a one-qubit state limited to ±|0> ± |1>, it's a two-qubit state limited to a|00> + b|01> + c|10> d|11> where a^2+b^2+c^2+d^2 = 1 and a,b,c,d are real. Also the state can be entangled with other qubits, as long the non-180-degree phase information is not between the various a's, b's, c's, and d's. For example, if you have the state (1/2 |000> - 1/sqrt(2) |010> + i/2 |101>)(|00> + |11>), then you can copy the first two qubits into the bell pair on one side then pull them out on the receiving side to end up in the state 1/2 |00000> - 1/sqrt(2) |01001> + i/sqrt(2) |10110>. E.g. see this circuit doing just that: http://i.imgur.com/wlcVAZG.png http://i.imgur.com/wlcVAZG.png Glad you liked the puzzle.