quantum devices with di ddi amond df td efects - u of t ...colloq/2012_2013/121108_lily... ·...
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Quantum devices ith di d d f twith diamond defects
Lilian ChildressBates College, TU Delft, Yale University McGill UniversityUniversity, McGill University
U i it f T tUniversity of TorontoNovember 8, 2012
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A few applications of diamond defect centers
Metrology
Stuttgart 2008Quantum information science
25 nm resolutionStuttgart 2008
Spin as sensorof electric and
Long‐lived nuclear spin quantum
2 qubit QC
of electric and magnetic fields, acceleration, time
Electronic spin mediates gates
memory
Harvard 2012
Subwavelength
Scanning magnetometer
,
And provides an optical
mediates gatesDelft 2012
2012
Optical devices Subwavelengthresolution
interface
Single photon
Stable emitter for fluorescence
source
Gottingen 2009
for fluorescence markersfor quantum repeaters
and quantum networks
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The quest for quantum bitsControllability vs coherence
•Solid state quantum systems •Atoms & molecules, isolated nuclear spins, photonsUCSB
Controllability vs coherence
spins, photonsUCSB
Harvard
InnsbruckStanford
Fast electrical or optical gating Typically short coherence times
Longest coherence times Excellent selection rules Difficult to prepare, control, and
•Impurity‐based electronic spins in solids
Inconsistent fabrication outcomes measure on fast timescales
Fast control possible with microfabricated gates
Long coherence times in spinless hosts
NV diamond: An interface between nuclear spins and photons
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The nitrogen‐vacancy center in diamond• Ground state electronic spin triplet
• Coherent interactions with proximal nuclear spinse‐e‐
Fast control ~ ns (electron) Excited
e‐e‐e‐e‐e
ns (electron)~ μs (nuclear)
Excited state S = 1
5 μm
• Optical transitions:preparation & detection of the electronic spinand the nuclear spins with which it interacts
Room temperaturesingle‐defect isolation,
Ground state S = 1
m 0
ms = ±1
cence
and the nuclear spins with which it interacts
ms = 0
lized
fluo
res
d t
Precession of a single 13C nuclear spin
Stuttgart, Harvard, UCSB, CanberraDutt et al. 2007
Normal data
fit
C nuclear spin
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The nitrogen‐vacancy center in diamond• Ground state electronic spin triplet
• Coherent interactions with proximal nuclear spins‐e‐
Fast control ( l ) Excited
an NMR moleculee‐e‐e‐e‐e‐
~ ns (electron)~ μs (nuclear)
Excited state S = 1
5 μm
• Optical transitions: single‐defect isolation, preparation & detection of the electronic spin
Spin S = 1 electronic ground
m 0
ms = ±1Higher fluorescence from ms = 0O ti l l i ti i t 0
Conventional approach: non‐resonant excitation
state ms = 0
Stuttgart, Harvard, UCSB, ANUeven at room temperature
Optical polarization into ms = 0
Enables measurements of a single NV spinCSB, ANUp
A new arena for exploring quantum phenomena and investigating applications
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The nitrogen‐vacancy center in diamond
The vision: • A few‐spin‐qubit register with
preparation, coherent control, andmeasurement• Scalability via optical connections
Spin‐photon entanglement
Quantum interference
entanglementTogan et al. 2010
Fast magnetic resonance based 1‐2 qubit gatesStuttgart, UCSB, Bates, Delft
Coincidence detection leaves spins entangled
a quantum channelLong coherence times
Stuttgart, Delft, Melbourne, Harvard
a quantum channel between the registers
,
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Outline
1. Optical spin readout
2 Two photon2. Two photon quantum
interference
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Outline
1. Optical spin readout
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Outline
1. Optical spin readout
Higher fluorescence from ms = 0Optical polarization into ms = 0
Conventional approach: non‐resonant excitation Excited state S = 1
Challenge: High fidelity preparation and
l h d fOptical polarization into ms 0
Time‐averaging or repetition* required!
Other approachese g Buckley et al
single‐shot detection of multiple spins ?
repetition required!
*Single shot readout of a nuclear spin, Neumann et al. Science 2010
Ground state ms = ±1
e.g. Buckley et al. Science 2010Our approach: resonant excitation
stateS = 1 ms = 0
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Resonant excitation of a single NV center at low temperature
Zero phonon
f0 f1line
Phonon side‐bandf1
f0
1
Excited state S = 1Excite
DetectSpin‐selective transitions
Detectf0only excited from ms= 0 ground statef1only excited from ms = ± 1 ground state f0
f1
Ground state ms = ±1ms = ±1
Mostly spin‐conserving transitionsSome spin‐mixing within the excited state
Optical pumping mechanism
0
stateS = 1 ms = 0ms = 0
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High fidelity spin preparation: Optical pumping
f1f0
1
Long spin‐flip time >99% preparation fidelity under f0excitation
An order of magnitude reduction in error rate
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Resonant readout of the NV center spin
f0
f1f0
Enhanced collection efficiency
Spin‐selective transitions
Many photons
No photons
yMicrofabricated SILs
f0only excited from ms= 0 ground statef1only excited from ms = ± 1 ground state
Readout mechanism
Mostly spin‐conserving transitionsSome spin‐mixing within the excited state
2‐3% collection efficiency = 10x improvement
Challenge: Can we collect enough photons to measure the spin before it flips? Yes!
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Resonant readout of the NV center spin
f0f1
Optical pumping Spin readout
NV Af0
Many photons
No photons
Single shot d i
F 93%
detection fidelity(lower bound)
Favg = 93%
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Resonant readout of the NV center spin
f0f1
Optical pumping Spin readout
NV ADo the fluorescence levels indicate spin?
Single shot d i
F 93%
detection fidelity(lower bound)
Favg = 93%
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How ideal is our quantum measurement?
Partially destructive: readout also optically pumps the spin
But:But: The shorter the readout duration, the less likely a spin flip is to occur
Short duration readout:
to occur
iPreparation by optical pumping
Very short readout pulse (400 ns)spin
super-position
0 photons=> Virtually no information about
1+ photons=> Only if initially ms=0information about
the spin state Probably still in ms=0
Allows measurement‐based quantum state preparation
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Measurement-based initialization of a multi-spin register
The simplest system:NV + h t 14N l i (I 1)
14N hyperfine lines
NV + host 14N nuclear spin (I = 1)
1 0 1ms= -1 Optical
esce
nce
-1 0 1
Nuclear spin projections
pumpingShort readout
2 86 2 87
Fluo
re
ms=0p j
2.86 2.87Microwave frequency (GHz)
Rotates electronic spin conditional on the nuclear spin state – a CNOT gatep g
Probabilistic state preparation for the nuclear spin
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Measurement-based initialization of a multi-spin register
ce
The simplest system:NV + h t 14N l i (I 1)
fluorescenc
e
NV + host 14N nuclear spin (I = 1) No preparation
ms=0 ou
tcom
prob
ability With
preparation into
Straightforward extension to NV B: N i l 13C larger numbers of nuclear spinsNo proximal 13C
isotopic impurities
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Measurement-based initialization of a multi-spin register
No preparationThree nuclear spins: enc No preparation
12 partially overlapping lines
p
fluoresce
e
With preparation into
NV A: T i l 13CTwo proximal 13C isotopic impurities
Initialization by measurement into 1 of 36 electron‐nuclear spin configurations
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Nuclear spin readout
m 1‐1 0 1
ms= ‐1
ms=0
No proximal 13C isotopic impurities
Pioneering work with
92% average fidelity
conventional detection: single‐shot nuclear spin detection at room temperatureat room temperatureNeumann et al. 2010See also Jiang et al. 2009
Compatible with sequential readout of electronic and nuclear spin
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Preparation, manipulation, and single-shot readout of a two-spin quantum registerof a two-spin quantum register
Measurement based state preparation Driven spin
rotationsrotations Single shot electron spin qubit readout
Repetitive single shot readout of the nuclear spin qubit
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Preparation, manipulation, and single-shot readout of a two-spin quantum registerof a two-spin quantum register
Electron spin Nuclear spin
Single‐shot detection of two spin qubits
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Outline
1. Single shot readout
2 Two photon Quantum interference between photons 2. Two photon quantum
interference
Q pemitted by different NVs can be used to establish long‐distance entanglement
Photons cannot emerge from different ports
Indistinguishablephotons => destructive interference
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Resonant emission: Towards two photon quantum interference532nm Towards two photon quantum interference532nm
Wanted: indistinguishable photons
Recipe:1. Spectral filters to isolate ZPL2. Spin pumping into ms=0
same polarization, same timing,
But…Inhomogeneity between NVs
s3. Polarization filteringsame spatial mode, same frequency
Inhomogeneity between NVsSpectral diffusion in time
ms = 0
EyRobledo et al. 2010
These two lines are orthogonally polarized
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Resonant emission: Towards two photon quantum interferenceTowards two photon quantum interference
Wanted: indistinguishable photonsSolution # 1: TuneRecipe:1. Spectral filters to isolate ZPL2. Spin pumping into ms=0
But…Inhomogeneity between NVs
s3. Polarization filtering
Inhomogeneity between NVsSpectral diffusion in time
bl lTunable optical transitions:
Strong DC Stark shiftsStrong DC Stark shifts
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Resonant emission: Towards two photon quantum interferenceTowards two photon quantum interference
Wanted: indistinguishable photonsSolution # 2: Get luckyRecipe:1. Spectral filters to isolate ZPL2. Spin pumping into ms=0
But…Inhomogeneity between NVs
s3. Polarization filtering
Inhomogeneity between NVsSpectral diffusion in time
Natural linewidth = 15 MHz
S l diff i b d dSpectral diffusion broadened linewidth ~ 500 MHz
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Legero et al. 2003Coping with spectral diffusion
Wanted: indistinguishable photonsSolution #3:
Time resolution
g
Key idea: they only have to be indistinguishable to the detector
Click!Time = t + τ
NV 2 Record coincidence clicks as a function of τ
+filters
532nm picosecond
Bin size dτ << 1/frequency differenceIndistinguishable photons> d t ti i t f
paths
Click!
pulseTime = 0
=> destructive interference
Click!Time = tNV 1
τ 0+filters
τ=0 within the τ=0 bin the photons are indistinguishable!
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Coping with spectral diffusion
Wanted: indistinguishable photonsSolution #3:
Time resolution
ˆ a 3 ˆ a 1 ˆ a 2 Two photon quantum interference
ˆ a 4 ˆ a 1 ˆ a 2Initial state:
Probability to detect a photon at time = t + τ
1 3ˆ a 1 ˆ a 2
0 1112
2 4
Click!Time = t
Remaining photon state (immediately afterwards):
τ=0Time = tafterwards):
ˆ a 4 1112 0112 11 02 ˆ a 4 0 Probability = 0 to detect in 3 at τ=0
Probability oscillates as (ω1‐ω2)τ
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Time resolved two‐photon quantum interference
Record time‐resolved coincidence countscounts
Two NVs
532nm ps‐pulsed excitation(10 MH )
Perpendicular polarization:
(10 MHz)
Parallel l i i
66% visibility
polarization:
polarization:y
Zero‐free‐parameter simulationsimulation
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Outlook: Eliminating luck
Both experiments “got lucky”Electronic tuning is tricky in the presence of photoexcited carriers
Barrett et al 2011
Simulation using measured f d if
coun
ts
tage (V
) frequency drifts
nciden
ce
Gate volt
Coi
NV ANV B
Detection time difference (ns)Excitation detuning (GHz)
Avenues for improvement: better understanding of tuning dynamics, optimized excitation frequencies
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Outlook: Integrated optics
Cavity quantum electrodynamics
Diamond ring Photonic crystal cavity
Critical technology:Collection efficiency typically << 1%ZPL only 3% of total emission resonatorZPL only 3% of total emission
Directed emissionHP labs 2011
HP labs 2012
Also Loncar, Fu, Becher, Barclay, A
h l E l d
Loncargroup2010 200 nm
Emission on cavity resonance enhanced by
F 3
3 Q
wschalom, Englund
Only increases overall collection efficiency
FP 4 2 n
V Quality factor
M d lMode volume
Diamond nanophotonics
Promising avenue to enhance ZPL emission fraction andimprove collection efficiency
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Summary
The vision: • A few‐spin‐qubit register with
preparation, coherent control, and readout• Scalability via interactions between NV registers
control strain, phonon Integration in processes, spectral diffusion
goptical cavities
Materials
Efficient protocols
Materials science
Heading towards entanglement distribution for quantum communication and quantum networksfor quantum communication and quantum networks
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Thanks to
LucioRobledoHannesBernien
Gijs de LangeWolfgang Pfaff
$$ FOM, SOLID, Research Corporation
Bas HensenToenov.d. Sar
Anna KashkanovaD h L
Ronald Hanson
Brian YangMi h ll U d d
$$ , , pDonghunLeeJack SankeyAndrew Jayich
Mitchell UnderwoodJack Harris
St ti J 2013Starting January 2013 …positions available!