quantum computing with trapped ionscs191/fa08/lectures/lecture23... · innsbruck quantum processor...
TRANSCRIPT
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Hartmut HäffnerInstitute for Quantum Optics and Quantum InformationInnsbruck, Austria
Quantum computing with trapped ions
Berkeley, Nov 25th 2008
€$
SCALAQGATES
FWF SFB
IndustrieTirol
IQIGmbH
• Basics of ion trap quantum computing
• Measuring a density matrix
• Quantum gates
• Deutsch Algorithm
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000001010011
100011110011
Quantumprocessor
Cavity QED
Superconducting qubits
Trapped ions
Quantum dots
NMR
© A. Ekert
Which technology ?
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000001010011
100011110011
Quantumprocessor
Cavity QED
Superconducting qubits
Trapped ions
Quantum dots
NMR
© A. Ekert
Which technology ?
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Good things about ion traps:
Ions are excellent quantum memories; single qubit coherence times > 10 minutes have been demonstrated (Boulder 1991)
(
Ions can be controlled very well
Many ideas to scale ion traps
Bad things about ion traps:
Slow (~1 MHz)
Technically demanding
Why trapped ions ?
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The hardware
S1/2
P1/2
D5/2
Qubit
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Trapped ions form the quantum register
Innsbruck quantum processor
Trap electrodes
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• Scalable physical system, well characterized qubits
• Ability to initialize the state of the qubits
• Long relevant coherence times, much longer than gate operation time
• “Universal” set of quantum gates
• Qubitspecific measurement capability
DiVincenzo criteria
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1. Initialization in a pure quantum state P1/2 D5/2
=1s
S1/2
40Ca+
P1/2
S1/2
D5/2P1/2
S1/2
D5/2D5/2
S1/2
Experimental procedure
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1. Initialization in a pure quantum state P1/2 D5/2
=1s
S1/2
40Ca+
P1/2
S1/2
D5/2
Dopplercooling Sideband
cooling
P1/2
S1/2
D5/2D5/2
S1/2
Experimental procedure
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2. Quantum state manipulation on S1/2 – D5/2 transition
Quantum statemanipulation
1. Initialization in a pure quantum state P1/2
S1/2
D5/2D5/2
S1/2
Experimental procedure
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P1/2 D5/2
=1s
S1/2
40Ca+
1. Initialization in a pure quantum state:
2. Quantum state manipulation on S1/2 – D5/2 transition
P1/2
S1/2
D5/2
Dopplercooling Sideband
cooling
P1/2
S1/2
D5/2
Quantum statemanipulation
P1/2
Fluorescencedetection
3. Quantum state measurement by fluorescence detection
S1/2
D5/2
Experimental procedure
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P1/2 D5/2
=1s
S1/2
40Ca+
1. Initialization in a pure quantum state:
2. Quantum state manipulation on S1/2 – D5/2 transition
P1/2
S1/2
D5/2
Dopplercooling Sideband
cooling
P1/2
S1/2
D5/2
Quantum statemanipulation
P1/2
Fluorescencedetection
3. Quantum state measurement by fluorescence detection
S1/2
D5/2
Experimental procedure
5µm
50 experiments / s
Repeat experiments100200 times
Spatially resolveddetection withCCD camera
Two ions:
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Ds
tate
pop
ulat
ion
Rabi oscillations
P1/2
S1/2
D5/2D5/2
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Ds
tate
pop
ulat
ion
Rabi oscillations
P1/2
S1/2
D5/2D5/2
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Ds
tate
pop
ulat
ion
Rabi oscillations
P1/2
S1/2
D5/2D5/2
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The phase ...
+
++ =
+
++e =ωt
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The phase ...
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The phase ...
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CCD
Paul trap
Fluorescencedetection
electrooptic deflector
coherentmanipulation of qubits
dichroicbeamsplitter
inter ion distance: ~ 4 µm
addressing waist: ~ 2 µm
< 0.1% intensity on neighbouring ions
10 8 6 4 2 0 2 4 6 8 100
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
Exc
itatio
nDeflector Voltage (V)
D
Addressing single qubits
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Memory errors:
Bitflips
Dephasing
Operationial errors
technical imperfections …
Decoherence mechanisms
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Ramsey Experiment
= 15.9 ms
π / 2 π / 2Ramsey Time
Dephasing of qubits
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Zeeman shift
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106 s
101 s
103 s
104 s
103 s
101 s
Single qubit gates
Two qubit gates (Geometric phase gates)
T
Single qubit coherence (magnetic field sensitive)
S
Coherence of the motion
105 s
102 s
100 s
102 s
Two qubit gates (CiracZoller approach)
T
Realized time scales
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qubit
Raman transitions:
Excited state
Ground state
Long lived qubits
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Raman transitions:
Excited state
Ground state
Long lived qubits
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From: C. Langer et al., PRL 95, 060502 (2005), NIST
Level scheme of 9Be+:
Long lived qubits
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From: C. Langer et al., PRL 95, 060502 (2005), NIST
Long lived qubits
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106 s
101 s
103 s
104 s
103 s
101 s
Single qubit gates
Two qubit gates (Geometric phase gates)
T
Single qubit coherence (magnetic field sensitive)
S
Coherence of the motion
105 s
102 s
100 s
102 s
Two qubit gates (CiracZoller approach)
T
Realized time scales
Single qubit coherence (magnetic field insensitive)
S
Single qubit coherence (magnetic field insensitive + RF drive)
S
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The common motionacts as the quantumbus.
Having the qubits interact
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50 µm
The common motionacts as the quantumbus.
Having the qubits interact
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harmonic trap
……
Ion motion
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harmonic trap
…
2levelatom joint energy levels
…
Ion motion
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carrier
carrier and sidebandRabi oscillationswith Rabi frequencies
LambDicke parameter
Coherent manipulation
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• Introduction to quantum information
• Entangled states
• Teleportation
• Scaling of ion trap quantum computers
• Wiring up trapped ions
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…
… …
…
Generation of Bell states
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π
…
… …
…
Generation of Bell states
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π/2
…
… …
…
Generation of Bell states
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π…
… …
…
Generation of Bell states
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π…
… …
…
Bell states with atoms
9Be+: NIST (fidelity: 97 %)
40Ca+: Oxford (83%)
111Cd+: Ann Arbor (79%)
25Mg+: Munich
40Ca+: Innsbruck (99%)
Generation of Bell states
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Fluorescencedetection withCCD camera:
Coherent superposition or incoherent mixture ?
What is the relative phase of the superposition ?
Analysis of Bell states
Measurement of the density matrix:SSSDDS
DD SSSDDSDD
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A measurement yields the zcomponent of the Bloch vector
=> Diagonal of the density matrix
Measuring a density matrix
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A measurement yields the zcomponent of the Bloch vector
=> Diagonal of the density matrix
Rotation around the x or the yaxis prior tothe measurement yields the phase informationof the qubit.
Measuring a density matrix
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A measurement yields the zcomponent of the Bloch vector
=> Diagonal of the density matrix
=> coherences of the density matrix
Rotation around the x or the yaxis prior tothe measurement yields the phase informationof the qubit.
Measuring a density matrix
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SSSD
DSDD SSSDDSDD
SSSD
DSDD SSSDDSDD
SSSD
DSDD SSSDDSDD
Decoherence properties of qubits
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Bellstate survives
Roos et al., Science 304, 1478 (2004)
Measurementof the center ion
A “real” thought experiment
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Generalized Bell states
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656100 measurements~ 10 h measurement time
Genuine 8particle entanglement
Häffner et al., Nature 438, 643 (2005)
Generalized Bell states
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Quantum gates …
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control target
...allows the realization of a universal quantum computer !
Having the qubits interact
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control target
...allows the realization of a universal quantum computer !
Having the qubits interact
Most popular gates: CiracZoller gate (SchmidtKaler et al., Nature 422, 408 (2003)). Geometric phase gate (Leibfried et al., Nature 422, 412 (2003)). MølmerSørensen gate (Sackett et al., Nature 404, 256 (2000)).
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Control bit
Target bit
Target
A controlledNOT operation
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A controlledNOT operation
Ion 1:
Vibration:
Ion 2:
SWAP1SWAPControl qubit
Target qubit
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A controlledNOT operation
Ion 1
Vibration
Ion 2
SWAP1SWAPControl qubit
Target qubit
Ion 1
Ion 2
Pulse sequence:Laser frequencyPulse lengthOptical phase
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1
2
3
4
Composite phase gate (2π rotation)
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4
3
2
1
Action on |S,1> |D,2>
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0=ϕ 0=ϕ 2πϕ =
0 20 40 60 80 100 120 140 160 1800
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Time (µs)
D5/
2 e
xcita
tion
Single ion composite phase gate
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Time (µs)
T
D5/
2 e
xcita
tion
0 50 100 150 200 250 3000
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Phase gate
0.978 (5)
π/2π/2
Single ion composite CNOT gate
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A controlledNOT operation
Ion 1
Vibration
Ion 2
SWAP1SWAPControl qubit
Target qubit
Ion 1
Ion 2
Pulse sequence:Laser frequencyPulse lengthOptical phase
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OutputInput
Probability
Truth table of the CNOT
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prepare CNOT detect
Using a CNOT to create a Bell state
output
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Raman transitions between
Interaction of two ions via common motion.
n=0
n=1
MølmerSørensen gate
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Raman transitions between
Interaction of two ions via common motion.
MølmerSørensen gate
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Raman transitions between
Interaction of two ions via common motion.
MølmerSørensen gate
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bicromatic beam applied to both ions
Technical realization
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entangled ?
Entangling ions
J. Benhelm et al., Nature Physics 4, 463 (2008)
Theory: C. Roos, NJP 10, 013002 (2008)
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gate duration
average fidelity: 99.3 (2) %
entangled
measure entanglementvia parity oscillations
Entangling ions
J. Benhelm et al., Nature Physics 4, 463 (2008)
Theory: C. Roos, NJP 10, 013002 (2008)
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maximally entangled states
Gate concatenation
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Gate performance
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The MS gate operation is optimized by
• pulse shaping, minimizes offresonant excitation
• phase relation of amplitude modulated dualfrequency beam
C. Roos, NJP 10, 013002 (2008).
Optimization of the gate
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• Scalable physical system, well characterized qubits / ?
• Ability to initialize the state of the qubits
• Long relevant coherence times, much longer than gate operation time
• “Universal” set of quantum gates
• Qubitspecific measurement capability
Often neglected:
• exceptional fidelity of operations
• low error rate also for large quantum systems
• all requirements have to met at the same time
DiVincenzo criteria
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Cirac, Zoller, Kimble, Mabuchi Zoller, Tian, Blatt
Scaling of ion trap quantum computers
Its easy to have thousands of coherent qubits …but hard to control their interaction
Kielpinski, Monroe, Wineland
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The Michigan T trap
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An implementation of the Deutschalgoritm …
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Deutsch‘s problem: Introduction
Decide which class the coin is: False (equal sides) or Fair
A single measurement does NOT give the right answer
Front
Back
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Deutsch‘s problem: Mathematical formulation
4 possible coins are representend by 4 functions
false
fair0110f(1)
(
10 10f(0)
(
Case 4Case 3Case 2Case 1
BalancedConstant
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false
fair
ZCNOTCNOTNOTIDz + f(x)
)
0110f(1)
(
10 10f(0)
(
Case 4Case 3Case 2Case 1
BalancedConstant
Deutsch‘s problem: Mathematical formulation
4 possible coins are representend by 4 functions
Physically reversible process realized by a unitary transformation+
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Deutsch Jozsa quantum circuit
f1
f2
f3
f4
1000010000100001
1000010000010010
0100100000100001
0100100000010010
Ufn
x x
z f(x) + z
NOT
ID
CNOT
ZCNOT
Case Logic Quantum circuit Matrix
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Quantum analysis gives the right answer after a single measurement!
•D. Deutsch, R. Josza, Proc. R. Soc. London A439, 553 (1992)
D
•M. Nielsen, I. Chuang, QC and QI, Cambridge (2000)
M
Uf
x
z
x
z + f(x)
z
|0>
|1>
Deutsch Jozsa quantum circuit
π/2
π/2
π/2
π/2
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Uf
x
z
x
z + f(x)
z
|0>
|1>
No information in the second qubit
electronic qubit
motional qubit
π/2
π/2
π/2
π/2
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D5/2
729 nm
|1>
|0>
internal qubit
Qubits in 40Ca+
S1/2
motional qubit
|0>|1>1
n=0
2
computational subspace
|S,0>
|D,0>|D,1>
|S,1>
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Uf
x
z
x
z + f(x)
z
|0>
|1>
No information in the second qubit
electronic qubit
motional qubit
π/2
π/2
π/2
π/2
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Deutsch Jozsa quantum circuit
f1
f2
f3
f4
1000010000100001
1000010000010010
0100100000100001
0100100000010010
Ufn
x x
z f(x) + z
NOT
ID
CNOT
ZCNOT
Case Logic Quantum circuit Matrix
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Deutsch Jozsa: Realization
x x
z f(x) + z
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Deutsch Jozsa: Realization
x x
z f(x) + z
Swap Swap
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|S,0>
|D,0>|D,1>
|S,1>
3step composite SWAP operation
1
2
3
1
3
I. Chuang et al., Innsbruck (2002)
I
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Deutsch Jozsa: Realization
x x
z f(x) + z
Swap Swap
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Deutsch Jozsa: Realization
x x
z f(x) + z
Swap Swap
Phasegate
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1
2
3
4
Composite phase gate (2π rotation)
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4
3
2
1
Action on |S,1> |D,2>
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Deutsch Jozsa: Realization
x x
z f(x) + z
Swap Swap
Phasegate
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Deutsch Jozsa: Realization
x x
z f(x) + z
Swap Swap
Phasegate
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Deutsch Jozsa: Realization
x x
z f(x) + z
Swap Swap
Phasegate
Phasegate
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Deutsch Jozsa: Realization
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Deutsch Jozsa: Realization
Time (µs)
T
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Deutsch Jozsa: Result
0.986(4)
0
0.931(9)
0
0.90(1)
0
measured |<1|w>|2
1111expected |<1|w>|2
0.975(2)
0
0.975(4)
0
0.087(6)
0
0.019(6)
0
measured |<1|a>|2
1100expected |<1|a>|2
Case 4Case 3Case 2Case 1
BalancedConstant
S. Gulde et al., Nature 412, 48 (2003)
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• Basics of ion trap quantum computing
• Measuring a density matrix
• Quantum gates
• Deutsch Algorithm
Conclusions
Berkeley, Nov 25th 2008
€$
SCALAQGATES
FWF SFB
IndustrieTirol
IQIGmbH
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