cavity bifurcation amplifier as …qulab.eng.yale.edu/documents/talks/cbaq_d.pdfmeasuring...
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![Page 1: CAVITY BIFURCATION AMPLIFIER AS …qulab.eng.yale.edu/documents/talks/CBAQ_D.pdfMEASURING QUANTRONIUM QUBIT WITH CAVITY BIFURCATION AMPLIFIER Michael Metcalfe E. Boaknin, V. Manucharyan,](https://reader031.vdocuments.us/reader031/viewer/2022022604/5b68634f7f8b9acc608ce124/html5/thumbnails/1.jpg)
MEASURING QUANTRONIUM QUBIT WITH CAVITY BIFURCATION
AMPLIFIER
Michael Metcalfe
E. Boaknin, V. Manucharyan, R. Vijay, C. Rigetti, I. Siddiqi, L. Frunzio and M. H. Devoret
(Qlab, Department of Applied Physics, Yale University)
Acknowledgements: D. Prober, R.J. Schoelkopf, S. Girvin
Monday evening seminarSeptember 11th 2006
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CONTENTS1. Introduction: - Quantum computing
- Implementations- Quantum circuits- Quantronium
2. Cavity bifurcation amplifier (CBA) :- Non-linear readout - Implementations- Bistability
3. Quantronium with CBA:- Spectroscopy/Gate modulations- Rabi/Ramsey oscillations
4. Outlook: - Coupled qubits (See Chad’s talk)- Multiplexed C.B.A’s
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QUANTUM COMPUTATIONQuantum computation:
Unitary evolution of initially prepared n-qubit state and its subsequent measurement
Qubit:Just a 2-state system (effective spin – ½)
0 1ϕ α β= +
0
1
ener
gy 2
01
3
Isolate two energy levels
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QUANTUM PARALLELISM
N-qubit state:2 1
0
N
kk
kCψ−
=
= ∑
Unitary operation,U:
2 1
0
N
kk
U C kUψ−
=
= ∑
2N operations in parallel!!
0 0 00 0 00 0 0 0 0 0
0 0 00 0 00 0 0 0 0 1
0 0 00 0 00 0 0 0 1 0
k
1 1 11 1 11 1 1 1 1 0
1 1 11 1 11 1 1 1 1 1
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QUBIT REALIZATIONSTrapped ions NMR
chloroform molecule
Long qubit coherenceLow environmental couplingScalability difficult
semiconductor dots superconducting circuits
Shorter qubit coherenceLarge environmental
couplingScalability easierElectrical access
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QUANTUM CIRCUITS
L
φ 2 2
2 2LH q
Cφ= ++q
-qC
[ ], iqφ = h
BE k Tω∆ = h
Ene
rgy
1GHzω
10mKT
Microfabricationand cryogenics
Equal level spacing Need non-linear element
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NON-LINEAR ELEMENT: JOSEPHSON JUNCTION
Model:
SCInsulator
SC
Josephson current: Circuit symbol:
( ) ( )02sin Jei t I t⎡ ⎤= − Φ⎢ ⎥⎣ ⎦h
ϕ∆SEM:Inductance:
( )0
12 cos
L i eI ϕ= =∂ ∆∂Φ
h
3.5µmNon-Linear Inductor!
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COOPER PAIR BOX
0
1
2
E/E
CP
1 2 3
LJ,EJ
Vg
Cg
~ ( )( )
222CP
g JC Ce
E =+
Island( ) ( ) ( )2
cosg CP g JH N E N N E θ= − −)) )
2g g
g
C VN
e= , N iθ⎡ ⎤ =⎣ ⎦
) )
0Ng
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SPLIT COOPER PAIR BOX0
1
CgVgδ
SEM image of Quantronium
Gate
Readout
SET4µm
( ) ( ) ( )21 cosg CP g JH N E N E
iδ θ δ
θ∂⎛ ⎞ ⎡ ⎤= − −⎜ ⎟ ⎣ ⎦∂⎝ ⎠
))
( ) ( )CPB z z x g xH h h Nδ σ σ= +CPJ EE <<
Artificial 2-level atom
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ENERGY LEVELSEigenstates, Ek: Mathieu Functions
( )δ
δϕ
δ∂
∂=
,1),(i0
kgk
g
NEN
Average loop current:
( )
Ecp = 17GHz, EJ0 = 15GHz
With inductance:
( ) 1
2
2
20
1
0
,11,−−
⎥⎥⎦
⎤
⎢⎢⎣
⎡⎟⎟⎠
⎞⎜⎜⎝
⎛
∂∂
=⎥⎦
⎤⎢⎣
⎡⎟⎠⎞
⎜⎝⎛
∂∂=
δδ
ϕδϕδ gk
g
NEINL
Sweet spot
Sweet spot:
0=∂∂=
∂∂
g
kk
NEE
δ
Ng=1/2
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NON-LINEAR READOUT
Vd
Vdrive
R
C
L
Non-linear LC oscillator
w
linear LC oscillator
|Vou
t| V
LJ
Vd
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NON-LINEAR READOUTNon-linear LC oscillator
Vd
R
C
L
|Vou
t|
Vd
stable
unstable
stable
LJ
Mapping
0
1
Quantronium Qubit0
1
E/E
c
Energy levels
Cg
Vg
g gC V e
0
1
2
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IMPLEMENTATIONSQuantronium qubit with Josephson bifurcation amplifier (JBA)
∼
2µm
(I. Siddiqi et. al, PRB 2006)
Quantronium qubit with cavity bifurcation amplifier (CBA)
Qubitin
out
Resonator
0 1
Qubit
NEW
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SAMPLEresonator
1) Precisely control non-linearity2) Engineer freq, Q3) No dissipation on-chipcapacitors
3mm
10mm
100µm
Nb
10µm
Al
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MICROWAVE RESPONSEBistable states
1.8 GHz 9.8 GHz
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OBSERVATION OF BISTABILITY
Re[Vout]
Im[V
out]
τm-2µs
2µs 3µs 10ns
countscounts
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WHY: MULTIPLEXED QUBITS
Coupling line Qubit in resonator
Multiplexed readout and gate lines
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C.B.A. WITH QUANTRONIUMSEM image of Quantronium in CBA
10µm
CPW ground
Island + 2 junctions
Readout junction
CPW ground
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GATE MODULATIONS
Readout in linear regime
Move to bistable regime:
More gainFlux (rads)
Fit is with Ecp = 17.0GHz and EJ0 = 15.1GHz
Gat
e ch
arge
(Coo
per p
airs
)
Flux (rads)
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SPECTROSCOPY
Fit: Ecp = 17.0GHzEJ0 = 15.1GHz
ReadoutSpectroscopy pulse
Varying frequency
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RABI OSCILLATIONSReadout Y-rotation
0
1qubit pulse
τA
,τ
A, (Volts)
A,
A2 (dBm)
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BEST RABI OSCILLATIONS
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RELAXATION TIME, T1
π pulse Readout
0
1τω
T1=1.4µs↔1.8µs
τω (µs)
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RAMSEY FRINGESπ/2 pulse τ Readoutπ/2 pulse
0
1
200ns ≤ T2 ≤ 800ns4 4
01 22 2.10 7.10Q Tϕ πν= = ↔
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MEASURED CONTRASTπ pulse Readout
V
0
1
Readout relaxation Reduced contrast
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TOMOGRAPHYPreparation
pulseReadout
Tom. pulse
h
h φ
φ
0 0 12
+ 0 12− 01
Initial states
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NOW: SLOTLINE NON-LINEAR RESONATOR
Optical image of device
200µm
Gate
Slotline
SEM image of qubit
4µm
Advantages: 1. Completely fabricated using e-beam lithography2. Gate and readout lines separated3. Excite ± mode in slotline for readout
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NEAR FUTURE: COUPLED QUBITS
QUBIT 2
Optical image of coupled qubit with slotline readoutSee Chad’s MES upcoming…..
Ug1
Ug2
QUBIT 1
Cc
QUBIT 2
QUBIT 1
Ug2
Ug1
Cc
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LONGER TERM: MANY COUPLED MULTIPLEXED QUIBTS
3mm10mm
Nb
Multiplexed resonators
preliminary data:
amplitude response
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CONCLUSION
• Developed fast, non-dissipative RF readout• Single shot qubit readout feasible• Scalable architecture• Coupled qubit experiments in progress…
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PREDICTED CONTRAST
0 0.4nAI∆ =0 0.3µAI =
2GHz12mK
Freq ∆ω
2GHz 1.4MHz 0.4nA 0.5nA
10GHz 20MHz 6.4nA 5nA
0measI∆ 0
theoryI∆
V
Sw
itchi
ng p
roba
bilit
y
68%
V (volts)
Single shot possible
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RAMSEY TOMOGRAPHYMap of state during Ramsey experiment (c.f. Martinis, PRL)
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Slides after this are additional
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RANDOM EQUATIONSJosephson Junction:
( ) ( )
( )
( )
spotSweet 0field transverseE
fieldZeeman
22E
where
1
cos1
CP
21
z
2
⇒=↔
↔
−==
+−=<<
∂∂=
−⎟⎠⎞
⎜⎝⎛ −
∂∂=
cont
J
gJCPcont
J
xcontzzCPB
CPJ
Jgcg
X
E
NEEXE
XEHEE
iN
ENi
ENH
σσ
θ
θθ
))
Cooper Pair box: Loop current/Inductances:
( )
( ) [ ]
( )
( ) ( )2
2
20
1
0
0k
00
21
,11,L
:inductancewith
,1),(i
:iscurrent loop average theHence
ˆ1ˆ,ˆ1,
2
ˆˆ K
island onto tunnelling pairscooper ofnumber where
2,
−−
⎥⎥⎦
⎤
⎢⎢⎣
⎡⎟⎟⎠
⎞⎜⎜⎝
⎛
∂∂
=⎥⎦
⎤⎢⎣
⎡⎟⎠⎞
⎜⎝⎛
∂∂=
∂∂=
∂∂=−=
⎟⎠⎞⎜
⎝⎛ +
=
−=
δδ
ϕδϕδ
δδ
ϕδ
δϕϕδ
δ
gk
kg
NEINg
NgEN
HHKi
NgI
NN
dtKdeNgI
)
))
))
[ ]
( )J
Jr
Ce
EeQN
iN
eNQ
22E
where
cos2E H
:JJ ofHamilton ,
:JJ across diff phase SC
with associatedFlux 2
:JJ through tunnelingCharge
2
CJ
2
CJ
0
=
−⎟⎠⎞⎜
⎝⎛ −=
==Φ
=
θ
θθϕ
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NON-LINEAR OSCILLATOR
LJ.I0V
R C L
R cost d NqL q q V t VC
ω+ + = +&& &
Linear resonance
( )20
1R 1 cos1 /
t J d NqL q q L q V t VC q I
ω⎛ ⎞⎜ ⎟+ + + − = +⎜ ⎟−⎝ ⎠
&& & &&&
V
w
Non-Linear resonance
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Readout scheme
0
B-Field
Biaspoint
I0’’
I0’
I0’’ < I0’
Vdrive
|Vou
t|
V
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Previous workCQEDQuantronium qubit with JBA
I. Siddiqi et. al, PRB 2006 A. Wallraff et. al, Nature 2004
Flux qubit with linear resonator and JBA
A. Lupascu et. al cond-mat/0601634
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Experimental observation of two oscillator states
-60
-40
-20
0
20
40
2.22.01.81.61.41.21.0
Voltage (V)
Pha
se (d
egre
es)
V
time
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Microwave responseBistable states
1.8 GHz 9.8 GHz
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Bistability
-1
0
1
-1 0 1
counts
-1
0
1
-1 0 1
counts
-1
0
1
-1 0 1
counts
-1
0
1
-1 0 1
counts
|Vou
t|
Vdrive
AB
C D
A
DRe[Vout]
Im[V
out]
B
C
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Readout scheme
0 1
Biaspoint
STATE 0
STATE 1
0
OS
CIL
LATI
ON
A
MP
LITU
DE
Power in
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JBA
Ti
Al capacitor pads
Bonding pads
SiCrCuCr
• Complicated fabrication• Same physics
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4.2K
260mK
300KIN OUT
2w2w
Arb
Source Source
Cold RussianAmplifier
MitiqAmplifier
Mini-CircuitAmplifier
Stepattenuator
Ecosorbfilter
Chocolatefilter
TIME RESOLVEDMEASURMENT
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ESCAPE RATES
For : aω Γ
exp2
a
B esc
Uk T
ωγπ
⎛ ⎞∆= −⎜ ⎟⎝ ⎠
Thermally activated escape:
Where:
1/ 222 1 /3 3a bω β β= ΓΩ − 3
2/ 264 1 /
9 3 Jt
Jb
LL
UQ
E β β⎛ ⎞⎜
Ω −⎟⎠
∆⎝
=
( )2/3ln( / 2 ) /a bvsω πγ β βPlot: Tesc
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ESCAPE RATESMETHOD
400
300
200
100
0
coun
ts
1.431.421.411.401.39
V ( Volts )
V
time
time
phase not switched
switched
( )1( )
( )v V
v V V
P vdVV Ln
V dt P vγ ≥
≥ +∆
⎡ ⎤⎢ ⎥= ⎢ ⎥∆⎢ ⎥⎣ ⎦
∑∑
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ESCAPE RATES
6
5
4
3
2
1
0
[ Ln
( ωa /
2 π
γ )
]2/3
2.22.12.01.91.8
V 2 ( Volts2
)
Intercept: Vb
Slope: Tesc
U0/KBT = 420
U0 = 220K
Tesc = 520mK
Tphysical= 260mK
Useful tool
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2D-HISTOGRAMS
τm-2µsReal (arb)
Imag
inar
y (a
rb)
Real (arb)
Imag
inar
y (a
rb)
-50
0
50
-50 0 50
latching
-50
0
50
-50 0 50
No latching
2µs 3µs 10ns 2µs 2µs 11µs 10ns
τm-10µs
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CAVITY BIFURCATION AMPLIFIER
( )20
1R 1 cos1 /
t eff J d Neff
qL q q L q V t VC q I
ω⎛ ⎞⎜ ⎟+ + + − = +⎜ ⎟−⎝ ⎠
&& & &&&
Veff
Reff
Ceff
Leff
LJ.I0
Parameters: Z0 = 50Ω;
ω0 ~ (1.8Ghz)2π;
COUT ~ 50fF;
Leff ~ 7nH;
Ceff ~ 1.5pF;
Reff ~ 0.03Ω;
Q ~ 2000
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THE JOSEPHSON TUNNEL JUNCTION:AN ATOM-LIKE CIRCUIT ELEMENT
TO WHICH YOU CAN ATTACHWIRES ...
S I STUNNEL
JUNCTIONEJ-N(2e) +N(2e)
Cj
[ , ] iNθ =))θ
NON-LINEAR INDUCTOR
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)sin( ϕ∆= cs IIZero voltage supercurrent:
Model:SC
Insulator
SC
JOSEPHSON JUNCTION
C R
tdtvt
J ′′=Φ ∫∞−
)(e2
0h=Φ
0
)(Φ
Φ=∆ tJϕ
h
eVdt
d 2)( =∆ϕApplied voltage: → alternating current
Free energy stored in junction: dtVIW s∫=
eIE C
J2h=constEF J +∆−= )cos( ϕ
02eILJ
h=
Non-Linear Inductor!
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ENERGY LEVELS OF AN ISOLATED JUNCTION
( )2/ 2 cos( )JCPH E N q e E θ= − −
))HAMILTONIAN: Z >> RQ = h/4e2
CHARGINGENERGY
COUPLING ENERGY, UJE/ECP
0
1
2
3
qe 2e
UJ
0
BLOCH WAVEFUNCTIONS
-π πθ
E
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E-BEAM
WRITE PATTERN WITH SEM
3.5µmOPTICAL IMAGE
OF RESIST
SHADOW-MASK EVAPORATION
PLEXIGLAS (PMMA)
COPOLYMER(MMA 8.5)
SILICON
2” SI WAFER
SPIN ON RESIST
2” SI WAFER
SPIN ON RESIST
DICE WAFER INTO SMALL CHIPS
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SHADOW-MASK EVAPORATION
PMMA
MMA
Bridge
Si
Undercut
Develop in MIBK:IPA, 1:3, for ~40s and rinse in IPA
2nd Al evaporation
CROSS SECTION:
Al
Lift off resist with unwanted
Al with Acetone (60-90ºC)
3.5µm
SEM IMAGE OF AL/AL2O3/AL JUNCTION
Oxidation: 15%O2, 85% Ar. 1-10T, 5-20mins
Al
First angle Al
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NON-LINEAR OSCILLATOR
LJ.I0V
R C L
R cost d NqL q q V t VC
ω+ + = +&& &
Linear resonance
( )20
1R 1 cos1 /
t J d NqL q q L q V t VC q I
ω⎛ ⎞⎜ ⎟+ + + − = +⎜ ⎟−⎝ ⎠
&& & &&&
V
w
Non-Linear resonance