Trouble is, it turns out to be impossible to do that in quantum mechanics. It's not just that it's difficult or hard to do, it's genuinely forbidden by the laws of physics!
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Suppose Alice measures her remaining qubit in some basis |m>. The resulting conditional state for Bob is, up to normalization: a<m|0> |0> + b <m|1> |1>
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Ahah! This is very promising! If we simply choose the basis |m> to be the equal superposition states |+> = (|0>+|1>)/sqrt 2 and |-> = (|0>-|1>)/sqrt 2 then Bob will get the following conditional states: a|0>+b|1> a|0>-b|1>
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That is, Bob's state is just Z^z|psi>, where z is the outcome of a measurement in the |+>, |-> basis.
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And so the following quantum circuit teleports |psi> from Alice to Bob:pic.twitter.com/AfUe1ncMAa
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This is, in fact, the standard quantum teleportation protocol!
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This leaves something to be desired as discovery fiction. Still, it's a lot of fun, and think it's pretty good for Twitter!
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Particularly egregious: it doesn't tell us WHY you might suspect teleportation is possible in the first place. Though I wonder if some quantum person thinking hard about classical one-time pads might have discovered it, largely by following their nose.
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Anyway, this kind of discovery fiction can be a lot of fun, and going through this exercise certainly helped me understand teleportation better!
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