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Simon Gartmann and Tranquillo Janisch

Theory

Quantum Teleportation: Concept

Definition: Transferring an unknown quantum state without transferring the physical carrier of information itself

Quantum Teleportation: Concept

Definition: Transferring an unknown quantum state without transferring the physical carrier of information itself

Means:

• Using non-local correlation

• Exchange of classical information

Quantum Teleportation: Protocol

1. Creation of an entangled pair shared between Alice and Bob

Quantum Teleportation: Protocol

1. Creation of an entangled pair shared between Alice and Bob

2. Alice does a two-qubit measurement identifying Bell states

Quantum Teleportation: Protocol

1. Creation of an entangled pair shared between Alice and Bob

2. Alice does a two-qubit measurement identifying Bell states

3. Feed-forward of the measurement result via a classical information channel from Alice to Bob

Quantum Teleportation: Circuit A

lice

B

ob

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Quantum Teleportation: Circuit

Hadamard gate:

CNOT:

Alic

e

Bo

b

Quantum Teleportation: Circuit

Four entangled Bell States

AND

Quantum Teleportation: Circuit A

lice

B

ob

Quantum Teleportation: Circuit

State to be teleported:

Bell-State:

Alic

e

Bo

b

Quantum Teleportation: Circuit

State to be teleported:

Bell-State:

Alic

e

Bo

b

Quantum Teleportation: Circuit

State to be teleported:

Bell-State:

After CNOT:

Alic

e

Bo

b

Quantum Teleportation: Circuit A

lice

B

ob

Quantum Teleportation: Circuit

Hadamardgate gives:

Alic

e

Bo

b

Quantum Teleportation: Circuit A

lice

B

ob

Quantum Teleportation: Circuit

Measurement: AND

Alic

e

Bo

b

Quantum Teleportation: Circuit

Measurement: AND

Thats the reason we need to feed-forward classical information!

Alic

e

Bo

b

Feed-forward

Nothing to do

Apply X

Apply Z

Apply X than Z

Mea

sure

men

t

Experimental Challenges

• Entanglement in macroscopic system

Experimental Challenges

• Entanglement in macroscopic system

• Distinguish bell-states in single shot

Experimental Challenges

• Entanglement in macroscopic system

• Distinguish bell-states in single shot

• Feed-forward of classical information in real time

Setup

Reminder: Transmon

Superconducting charge qubit

Figure: Wallraff et al., Strong coupling of a single photon to a superconducting qubit using circuit quantum electrodynamics, Nature 431, 162-167, 9.9.2004

Cg

Cj, Ej φ

Reminder: Transmon

Superconducting charge qubit

Frequency is tunable by

applying flux

Figure: Wallraff et al., Strong coupling of a single photon to a superconducting qubit using circuit quantum electrodynamics, Nature 431, 162-167, 9.9.2004

Cg

Cj, Ej φ

Reminder: Transmon

Superconducting charge qubit

Frequency is tunable by

applying flux

Resilient to charge noise

Figure: Wallraff et al., Strong coupling of a single photon to a superconducting qubit using circuit quantum electrodynamics, Nature 431, 162-167, 9.9.2004

Cg

Cj, Ej φ

Circuit implementation

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Circuit implementation Q1, Q2, Q3: Qubits

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Circuit implementation Q1, Q2, Q3: Qubits

R1, R2, R3: Resonators

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Circuit implementation Q1, Q2, Q3: Qubits

R1, R2, R3: Resonators

Red: Resonator input/output lines

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Circuit implementation Q1, Q2, Q3: Qubits

R1, R2, R3: Resonators

Red: Resonator input/output lines

Green: Microwave charge gate lines

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Circuit implementation Q1, Q2, Q3: Qubits

R1, R2, R3: Resonators

Red: Resonator input/output lines

Green: Microwave charge gate lines

Blue: flux-bias lines

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Process

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Process

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Read-out

JPA: Josephson parametric amplifier

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Read-out

HEMT: High electron mobility transistor

(amplifier)

JPA: Josephson parametric amplifier

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Read-out

RT: room temperature amplifier

HEMT: High electron mobility transistor

(amplifier)

JPA: Josephson parametric amplifier

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Read-out IF: Converts signal to intermediate frequency

RT: room temperature amplifier

HEMT: High electron mobility transistor

(amplifier)

JPA: Josephson parametric amplifier

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Read-out IF: Converts signal to intermediate frequency

RT: room temperature amplifier

HEMT: High electron mobility transistor

(amplifier)

JPA: Josephson parametric amplifier

• Qubits Q1/Q3 couple to resonators R1/R3.

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Read-out IF: Converts signal to intermediate frequency

RT: room temperature amplifier

HEMT: High electron mobility transistor

(amplifier)

JPA: Josephson parametric amplifier

• Qubits Q1/Q3 couple to resonators R1/R3.

• Measure amplitude and phase of the transmitted signal.

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Single-shot measurement

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Single-shot measurement • Single-shot measurement yields 1

data point.

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Single-shot measurement • Single-shot measurement yields 1

data point.

• Ideally cluster size << cluster

separation

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Single-shot measurement • Single-shot measurement yields 1

data point.

• Ideally cluster size << cluster

separation

• Achieved fidelity of 81.8%

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Feed-forward • Implemented with a field-

programmable gate array (FPGA)

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Feed-forward • Implemented with a field-

programmable gate array (FPGA)

• Total time delay for feed-forward

is 505 ns

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Feed-forward • Implemented with a field-

programmable gate array (FPGA)

• Total time delay for feed-forward

is 505 ns

• To avoid decoherence of Q3

during this, apply series of

dynamical decoupling pulses

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Results

Principal scheme

Each step causes fidelity losses.

Any delay can lead to decoherence.

Entangled state

preparation

Projective measurement

in Bell basis

Correction by single-qubit

rotations

Post-selection

• Measurement in Bell basis

Post-selection

• Measurement in Bell basis

• Determine whether result is or not

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Post-selection

• Measurement in Bell basis

• Determine whether result is or not

• Can post-select on other states by pre-rotating qubits (rotate other state to , , then measure it)

Post-selection

• Measurement in Bell basis

• Determine whether result is or not

• Can post-select on other states by pre-rotating qubits

• Time scale: 400 ns

Post-selection

• Measurement in Bell basis

• Determine whether result is or not

• Can post-select on other states by pre-rotating qubits

• Time scale: 400 ns

→No simultaneous distinction of all four Bell states and no feed-forward.

Post-selection process tomography

Average process fidelity: 72.0 ± 1.4 % Average state transfer fidelity: 81.7 ± 1.4 %

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Simultaneous deterministic measurement

• Measurement in Bell basis

Simultaneous deterministic measurement

• Measurement in Bell basis

• Distinguish between all 4 Bell states in real time.

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Simultaneous deterministic measurement

• Measurement in Bell basis

• Distinguish between all 4 Bell states in real time.

• Time scale: 600 ns

Simultaneous deterministic measurement

• Measurement in Bell basis

• Distinguish between all 4 Bell states in real time.

• Time scale: 600 ns

→ No feed forward

Simultaneous deterministic measurement process tomography

Average process fidelity: 65.5 ± 1.1 % (72.0 %) Average state transfer fidelity: 77.1 ± 1.2 % (81.7%)

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Full scheme

• Measurement in Bell basis

Full scheme

• Measurement in Bell basis

• Distinguish between all 4 Bell states in real time

Full scheme

• Measurement in Bell basis

• Distinguish between all 4 Bell states in real time

• Apply single-qubit rotation to Q3 if necessary

Full scheme

• Measurement in Bell basis

• Distinguish between all 4 Bell states in real time

• Apply single-qubit rotation to Q3 if necessary

• Time scale: 700 ns

Full scheme process tomography

Average process fidelity: 62.2 ± 0.3 % (65.5%) Average state transfer fidelity: 77.4 ± 0.2 % (77.1%)

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Results Comparison

Post-selection Simultaneous deterministic measurement

Full Classically expected

Average process fidelity

( 72.0 ± 1.4 ) % ( 65.5 ± 1.1 ) % ( 62.2 ± 0.3 ) % 1/2

Average state-transfer fidelity

( 81.7 ± 1.4 ) % ( 77.1 ± 1.2 ) % ( 77.4 ± 0.2 ) % 2/3

What was achieved?

• Realization of full deterministic quantum teleportation in a macroscopic system

– QM experiments on macroscopic scale

What was achieved?

• Realization of full deterministic quantum teleportation in a macroscopic system

– QM experiments on macroscopic scale

• Demonstrated a feed-forward implementation

– Application in error correction schemes

What was achieved?

• Realization of full deterministic quantum teleportation in a macroscopic system

– QM experiments on macroscopic scale

• Demonstrated a feed-forward implementation

– Application in error correction schemes

• Low transmission loss of superconducting waveguides

– Possibly allowing larger teleportation distances

Circuit implementation R1, R2, R3: Resonators

Q1, Q2, Q3: Qubits

Red: Resonator input/output lines

Green: Microwave charge gate lines

Blue: flux-bias lines

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013

Post-selection

Simultaneous deterministic measurement

Full scheme

Figures: Steffen et al., Deterministic quantum teleportation with feed-forward in a solid state system, Nature 500, 319–322, 15.8.2013