quantum teleportation
Despite the science-fiction name, quantum teleportation does not beam any object across a room. It is a protocol for moving the unknown state of one qubit from a sender (call her Alice) to a receiver (call him Bob) without sending the qubit itself. Think of it less like a transporter and more like a very careful relay: Alice and Bob first share a pair of entangled qubits, prepared in advance. Later, when Alice has a mystery qubit whose state she does not know, she can hand that state over to Bob using only their shared entanglement plus two ordinary classical bits sent over a normal channel like the internet or a phone line.
Here is the mechanics, in plain terms. Alice interacts her mystery qubit with her half of the entangled pair and measures both, getting one of four possible two-bit outcomes. That measurement destroys the original state on her side, which is why teleportation does not violate the no-cloning rule: there is never a second copy, just a transfer. She sends those two bits to Bob, who applies one of four simple fixups to his entangled qubit. Once he does, his qubit now carries the exact state Alice started with. Crucially, Bob's qubit is useless until his classical bits arrive, so nothing travels faster than light and no information is delivered by entanglement alone.
Why bother, if you still have to send classical bits? Because the qubit's full state, an infinite continuum of possible amplitudes, is conveyed using only that shared entanglement and two bits, and no quantum channel between Alice and Bob is needed at the moment of transfer. That makes teleportation a core building block of quantum networks and future repeaters: rather than pushing fragile qubits down a long, lossy fiber, you distribute entanglement first and teleport states across it on demand.
Alice never learns alpha or beta; the protocol transfers the whole unknown state to Bob, and her copy is destroyed in the process.
Teleportation moves a quantum state, not matter, and not faster than light, since it cannot complete until the two classical bits arrive over an ordinary channel.