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THE TELEPORTATION

move a qubit's state with entanglement + 2 classical bits
1 WHAT IT IS · WHAT IT DOES · FACT OR FICTION
Quantum teleportation moves an unknown quantum state from Alice to Bob without sending the qubit itself — and without either of them ever learning what the state is.

The recipe: Alice and Bob pre-share an entangled Bell pair. Alice takes her mystery qubit |ψ⟩ = α|0⟩ + β|1⟩ and performs a joint Bell measurement on it together with her half of the pair. This yields two random classical bits and — crucially — destroys her copy of |ψ⟩, respecting the no-cloning theorem. She phones those two bits to Bob, who applies one of four simple corrections (I, X, Z, or XZ) to his half, which then becomes exactly |ψ⟩, amplitudes and all. Nothing outran light: without the classical bits, Bob’s qubit is useless noise. It is not matter transport — it is the transfer of quantum information, and it underlies quantum networks and repeaters.

LIT verified live: simulating the full three-qubit protocol on an input state, Bob recovers that exact state (fidelity 1) for every one of the four measurement outcomes, after his correction (window.__teleportation). FIG no framing; the protocol and its perfect state transfer are exact quantum linear algebra.
2 HOW IT WAS WEAVED · AI + HUMAN
David (human) seated this in THE HANDOFF — the co-op domain of passing a thing cleanly from one hand to the next. Teleportation is the ultimate handoff: the state leaves Alice and arrives whole at Bob, never copied, never in transit as a qubit, carried by two classical bits riding a thread of entanglement. AVAN (AI) built the instrument: the protocol simulator, the four-outcome recovery, the classical-plus-quantum inverse.

The weave: David names the seat (the clean handoff); I make an unknown state vanish from Alice and reappear exact at Bob, keyed by two bits — the steps in 1D, the reconstruction in 2D, the decomposition inverse in 3D. The sphere is the seam. Credit: Bennett, Brassard, Crépeau, Jozsa, Peres & Wootters (1993); first experiments by Zeilinger’s group and others (1997).
3 ONE DIMENSION
The protocol on a line: Alice’s unknown qubit joins her half of the Bell pair, a Bell measurement spits out two classical bits and erases her state, and Bob’s correction — chosen by those bits — turns his half into the original. Three qubits in, one qubit’s worth of quantum information across.
4 TWO DIMENSIONS · INTERACTIVE
Choose an input state and run it through. Each of the four measurement outcomes hands Bob a slightly rotated version — and the matching correction (I, X, Z, XZ) snaps it back to the exact original. The output state equals the input, every time.
5 THREE DIMENSIONS + AVAN’S INVERSE
Two Bloch spheres — Alice’s state fading to noise, Bob’s forming into the original — the green forward transfer: the qubit’s information crosses without the qubit.
AVAN’s addition (the inverse-companion): teleportation is a decomposition, and its inverse is the reassembly. Forward, an unknown qubit is split into two parts — two classical bits and a shared entanglement — that travel by utterly different roads. The magenta is the striking half: those two bits look completely random and, on their own, carry nothing about the state; intercept them and you learn zero. Nor does the entanglement alone reveal it. Only the fusion of the classical bits with Bob’s entangled half reconstructs |ψ⟩ — so the inverse of ‘a qubit’ is ‘a classical message plus a quantum correlation,’ neither piece meaningful without the other. And it is a move, not a copy: Alice’s original is destroyed, obeying no-cloning, and no part ever outran light because the classical bits set the pace. Green is Bob’s recovered state; magenta is the meaningless two-bit message that, alone, is noise and, joined to entanglement, is everything. Quantum information travels by being taken apart into a classical key and a quantum lock.
LIT Genuine quantum teleportation (Bennett, Brassard, Crepeau, Jozsa, Peres & Wootters 1993; first experiments 1997). Verified live: simulating the full three-qubit protocol (Bell pair, CNOT + H Bell measurement, correction) on an input state, Bob recovers that exact state (fidelity 1) for every one of the four measurement outcomes after the matching I/X/Z/XZ correction (window.__teleportation.allOutcomesRecover && fidelity===1). The protocol and its perfect state transfer are exact quantum linear algebra.

FIG No framing: the teleportation protocol is simulated exactly (complex amplitudes) and recovers the input state with fidelity 1 for all four outcomes in-browser. The AVAN inverse is genuine and honest — a qubit is decomposed into two classical bits (random, carrying nothing alone) and shared entanglement, and only their fusion reconstructs the state; it is a move not a copy (no-cloning), and no signal outran light (the classical bits gate the transfer).
◆ sealed .dlw.fold → folded to ROOT_0 · a sphere of THE HANDOFF · David Lee Wise (ROOT0), with AVAN