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Linear algebra 18 Quantum teleportation © Tim Byrnes What is quantum teleportation? ψ The aim of quantum teleportation is to send an unknown quantum state held by Alice to Bob At the end of the proces.

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18 Quantum teleportation

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What is quantum teleportation?

ψ

The aim of quantum teleportation is to send an unknown quantum state held by Alice to Bob

At the end of the process Bob should have the unknown quantum state

Alice and Bob never need to know what the state is

Initial state

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What is quantum teleportation?

ψ

The aim of quantum teleportation is to send an unknown quantum state held by Alice to Bob

At the end of the process Bob should have the unknown quantum state

Alice and Bob never need to know what the state is

Final state

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What quantum teleportation is and is not

ψ

The atom itself doesn’t disintegrate and get sent somewhere So its not

quite like the Star Trek-like teleporter

But the quantum state is the most fundamental representation of the

state, and if the qubits are atoms, then they are fundamentally identical

So if you say the quantum state is the most basic reality, then it is quite

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Why is teleportation amazing?

There is an emphasis on the fact that Alice and Bob do not know the state Why is this important?

If Alice knew what the state was, she could just tell Bob what the state is, and Bob could make that state No need for

teleportation

Hi Bob My state is Can you make it there?α =i/ 2,β = 3 / 2

Sure thing, I’ll do it right away

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Measuring an unknown state

Even if Alice didn’t know her state initially, couldn’t she just figure this out and tell Bob?

With only one copy of the state, it is impossible to figure out an unknown state There are an

infinity of basis choices that could be made, and since the measurement outcome is random,

this doesn’t give much information

e.g Measuring gives the outcome All this says for sure is that ψ = α 0 + β 1 1 β ≠ 0

I measured it and I got Not sure what the state is but why don’t you just make that?

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Theoretical limit to estimate state

ψ ψ ψ

It was shown that even with the fanciest possible measurements, the best estimate

you can get of N unknown copies of a state is fidelity

For one qubit N=1, the best fidelity is F=2/3=0.666

If Alice doesn’t know her state its impossible to just tell Bob exactly what it is with one copy

est

ψ

My best guess of the

Massar & Popescu Phys Rev Lett 74, 1259 (1995)

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The teleportation circuit

The teleportation circuit allows you to overcome this and (under ideal conditions) get perfect transfer of the state!

Alice

Bob

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The teleportation circuit

The main steps of the teleportation circuit are

Alice

Bob

1 Entanglement generation

2 Measurement in Bell basis

3 Classical correction

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Part 1: Entanglement generation

The first part of the circuit produces an entangled state

Working through the circuit step by step we have

T0

T = ψ

Time T0:

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Part 1: Entanglement generation

0 1

H H

= +

= −

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Part 1: Entanglement generation

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Part 2: Measurement in Bell basis

The next part of the circuit is an example of what was

seen in Lecture 14

A unitary in front of a measurement makes a

measurement in a different basis

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Part 2: Measurement in Bell basis

We can also just work this out step by step as before

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Part 2: Measurement in Bell basis

Applying the Hadmard

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Part 2: Measurement in Bell basis

Now we measure the qubits in the basis

Here it is easiest to write the state before the

measurement in terms of the four measurement

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Part 2: Measurement in Bell basis

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Part 3: Classical correction

After the measurement we have

We can see already that the teleportation is nearly there

For the 00 outcome it actually is already working, but for the other cases Bob

gets a state that is almost the state, but with an extra bit flip (01 case) or a phase

flip (10 case), or both (11 case)

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Part 3: Classical correction

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Part 3: Classical correction

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What have we achieved?

Bob has received Alice’s state without any knowledge of what the state is Neither Alice nor

Bob needs to know what the state is (of course its fine if they know what the state is, they

just do not need to know)

The main things that are needed are:

1) Entangled qubits between Alice and Bob

2) Alice needs to tell Bob what measurement outcomes she got (classical communication)

The fidelity of the transfer is (ideally) perfect, F=1 This is better than any state estimation

method

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Superluminal teleportation?

ψ

Provided that the entanglement can be set up before,

there is no reason that this could not work over

arbitrary distances

Then couldn’t we teleport states between different

stars separated across the universe?

The thing that spoils this is that Alice and Bob need to

do the classical correction step

This cannot travel faster than the speed of light, so it is

not really possible to complete the teleportation faster

than the speed of light

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