CouplingRydbergAtomstoSuperconductingQubits ViaASuperconductingCoplanar
WaveguideResonator
MatthewBeckPreliminaryExamination
December9,2015
Outline
1. Motivation
2. Rydberg Atom β Superconductor Interface Design and Characterization
3. Proposed Initial Experiments
4. Cryostat Design and Characterization
5. Future Work
6. Conclusions
Rydberg Atoms / Superconductors For Quantum Computing
Ze-Liang Xiang, et al., Rev. Mod. Phys. 85, 623
Bridge computational speed of SC with long livedstates of atomic systems
Market For A Hybrid Quantum Interface
Market For A Hybrid Quantum Interface
Critical Element
Current Efforts - Tubingen
Fortagh GroupTubingen β’ Rb MOT in 6 K stage
β’ Magnetic Transport tomilliKelvin stage
β’ Hyperfine transitioncoupling, f = 6.835 GHz
β’ Superconducting Element?
Current Efforts β JQI, Maryland
Wellstood Group, JQI
β’ Rb atoms trapped inevanescent wave ofoptical nanofiber
β’ SC β lumped elementResonator
Atom β SC Coupling
β’ Utilize magnetic moment of hyperfine splitting in Rb ground state- Rely on ensemble coupling of many
atoms to compensate small mag. moment
β’ Road to bridging atom trapping with mKenvironment still unclear
β’ Utilize large electric dipole moment of Cs Rydberg atom- Strong coupling with 1 atom
β’ Initial experiments to demonstrate strong couplingto be conducted at 4 K
Our Approach
Current Approaches
Rydberg Atom-SC CPW Interface - In Theory
Cs Ground Hyperfine Ensemble Coupling[ Vienna, TΓΌbingen, NIST ]
Rydberg Level Electric Dipole Transition
nπ = 0
π = 15-10 GHz
5-10 GHz
CPW Electric Field Loss Rate @ 4K
Strong Atom - CPW Coupling At LHe Temperatures
Rydberg Atom-SC CPW Interface - In Practice
Resonant Dispersive
Rydberg Atom-SC Interface - In Practice
Strong Atom - CPW Coupling At LHe Temperatures
β’Quality factor, Q, is dominated by non-equilibrium thermal quasiparticle loss
- Max Q = CPW Theory + Mattis β Bardeenβ’Coupling strength,
- Maximize Electric Field Spatial Extent
MB + CPW Theory
π 'πΏ) + CπΏ+
πΏ)πΏ+π ' C
MB Surface Z CPW Geometry 4K CPW Resonator
MB + CPW Theory β Anomalous Skin Effect
π 'πΏ) + CπΏ+
πΏ)πΏ+π '
MB Surface Z CPW Geometry 4K CPW Resonator
C
πAnomalous Skin
Effect In SCπ-./ β π
MB + CPW Theory β CPW Geometry
π 'πΏ) + CπΏ+
πΏ)πΏ+π ' C
MB Surfce Z CPW Geometry 4K CPW ResonatorMB Surface Z
MB + CPW Theory β Quality Factor = dependent on geometry
π 'πΏ) + CπΏ+
πΏ)πΏ+π ' C
MB Surfae Z CPW Geometry 4K CPW ResonatorMB Surface Z
MattisβBardeen Conductivity: Anomalous Skin Effect in SC
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 110β20
10β15
10β10
10β5
100
T /Tc
Ο1(T
) / Ο
n
ππΈ
π 4(π)/π 9
MattisβBardeen Conductivity: Anomalous Skin Effect in SC
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1β0.2
0
0.2
0.4
0.6
0.8
1
1.2
T/Tc
Ο2(T)/Ο2(0)
π :(π)/π :(0)
CPW Theory β Inductance Vs. Geometry
4πΏ+π=>
π (π’π)
CPW Theory β Kinetic Inductance
π
~ Thick. Correction
~ Geom. Correction
Numerical Closed Form
Clem, JR J. Appl. Phys. 113, 013910 (2013)
CPW Theory β Kinetic Inductance: Numerical Results
0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 250.5
1
1.5
2
2.5
3
3.5
4x 10β8
Gap Width, S (um)
Lk (H
enry
/Met
er)
w = 5, Numericalw = 5, ClemW = 10, NumericalW = 10, ClemW = 15, NumericalW = 15, ClemW = 20, NumericalW = 20, Clem
Quality Factor Vs. CPW Geometry
Mattis β Bardeen Limited CPW: Measurement
Sputtered NbSapphire Subst.
100 nm thickTc ~ 8.5 KRIE Etch
Cc ~ 5 fF
Mattis β Bardeen Limited CPW: Measurement
4.67 4.672 4.674 4.676 4.678 4.68x 109
β15
β10
β5
Frequency (Hz)
S 21 d
B
Data Fit
0 0.5 1 1.5β0.4
β0.2
0
0.2
0.4
0.6
Re[S21]
Im[S21]
DataFit
Mattis β Bardeen Limited CPW: Quality Factor Data
0 5 10 15 20 25 30 350
2000
4000
6000
8000
10000
12000
14000
16000
CPW Gap Width (um)
Inte
rnal
Q
W = 5 um, DataW = 5 um ThyW = 10 um, DataW = 10 um, ThyW = 20 um, DataW = 20 um, ThyW = 30 um, DataW = 30 um, ThyW = 50 um DataW = 50 um Thy
Mattis β Bardeen Limited CPW: Quality Factor Data
0 5 10 15 20 25 30 350
2000
4000
6000
8000
10000
12000
14000
16000
CPW Gap Width (um)
Inte
rnal
Q
W = 5 um, DataW = 5 um ThyW = 10 um, DataW = 10 um, ThyW = 20 um, DataW = 20 um, ThyW = 30 um, DataW = 30 um, ThyW = 50 um DataW = 50 um Thy
Can maximize Q with wider center traces and wider CPW gaps
CPW Electric Field
x (Β΅m)
z(Β΅
m)
(a) (b)
β40 β20 0 20 400
20
40
60
80
|E0|(V
/m)
0
0.02
0.04
0.06
0.08
0.1
0 10 20 30 40 500
0.02
0.04
0.06
0.08
0.1
z (Β΅m)
0
1
2
3
4
5
g/2Ο(M
Hz)
x=0x= (s+w)/2
-100 -50 0 50 100
CPW Electric Field
x (Β΅m)
z(Β΅
m)
(a) (b)
β40 β20 0 20 400
20
40
60
80
|E0|(V
/m)
0
0.02
0.04
0.06
0.08
0.1
0 10 20 30 40 500
0.02
0.04
0.06
0.08
0.1
z (Β΅m)
0
1
2
3
4
5
g/2Ο(M
Hz)
x=0x= (s+w)/2
For achievable atom-CPW distances,coupling is low
Must extend electric field off chip to achieve strong coupling
-100 -50 0 50 100
CPW Electric Field Extension β Chip Design
17.5 mm
Niobium Sapphire
π/π
CPW Electric Field Extension β Chip Design
17.5 mm
CPW Electric Field Extension β Layer Stack-Up
17.5 mm
Nb
Ti/Pd
Cu
Sub - 500 um
- 200 nm
- 3/30 nm
- 50 um
CPW Electric Field Extension - Realization
125 um75 um
150 um
100 um
200 um
Re[S21]0.4 0.6 0.8 1 1.2
Im[S21]
-0.3
-0.2
-0.1
0
0.1
0.2
0.3
CPW Electric Field Extension - Realization
πF.FG = 3Γ10J β π-KNo added loss from Cu structures
DataFit
Rabi Oscillations
90
70
50
30
10
πF
π/2π (MHz)
πPQRF
Proposed Coupling Measurement - Log Magnitude
πΈ = 6Γ10T:V/mπ = 3.2ππ»π§ Γ2π
Proposed Coupling Measurement - Phasor
Proposed Coupling Measurement β IQ Plane
π« = πΆ[ β πΆT
Measurement β SNR
Measurement β SNR
Increasing cavity photon number will increaseSeparation and SNR
Experimental Apparatus β Custom 4K Cryostat, Design
β’ UHV Compatible- Conflat seals - Low outgassing Materials
β’ Long Cryogen Hold Times- Low Thermal Conductivity to 300 K- Minimization of stray light from optical access
ports
β’ Low Vibration- Rigid frame for mounting to an optical table
Experimental Apparatus β Custom 4K Cryostat, Design
LN Vessel(12 L)
LHe Vessel(27 L)
Outer VacuumJacket
77K Shield4K Cold Finger
πR < 2Γ10T_Torr
MOT
CPW
Experimental Apparatus β Custom 4K Cryostat, Design
LN Vessel(12 L)
LHe Vessel(27 L)
Outer VacuumJacket
77K Shield4K Cold Finger
MOT
CPW
Experimental Apparatus β Custom 4K Cryostat, Design
LN Vessel(12 L)
LHe Vessel(27 L)
Outer VacuumJacket
77K Shield4K Cold Finger
MOT
CPW
Experimental Apparatus β Custom 4K Cryostat, Design
LN Vessel(12 L)
LHe Vessel(27 L)
Outer VacuumJacket
77K Shield4K Cold Finger
MOT
CPW
Experimental Apparatus β Optical Access
Experimental Apparatus β Optical Access
Cryostat Design β Cold Lens
πab' = 100 K Reduced heat load on 4K stage by ~ 80 mW
Custom 4K Cryostat, Heat Load
Liquid Nitrogen
- Heat Load ~ 23 Watts
- Dominated by 300K radiation over large surface area
- 40 hour hold time for 11 L tank
Liquid Helium
- Heat Load ~ 270 mW
- 170 mW load originating from 300K optical access to cold finger
- 60 hour hold time for 27 L tank
Experimental Apparatus β Custom 4K Cryostat, Sample Mount
Cold Finger
SampleDC E Field Compensation
Pins
Custom 4K Cryostat, Vibration Characterization
852 nm
πcaQ'
πPad
Custom 4K Cryostat, Vibration Characterization
οΏ½Μ οΏ½ = 1.2ππ
οΏ½Μ οΏ½ = β« πππ·ππ
@ 3 KHz BW
Future Plans β Cz gates in DR
Rotation
πPulse
πPulse
Cavity photon number dependent phase
Conclusions
β’ Resonator quality factors > 1e4
β’ CPW E Field β Cu EPβd structures
β’ Strong coupling achievable at 4K
β’ Custom UHV cryostat has P < 2e-9 T
β’ Sample vibration ~ 1 um
β’ Final preparations in progress for experimental realization
MattisβBardeen Conductivity: Anomalous Skin Effect in SC
ππ» = π»=πTl/mAnomalousskin effect
In SCπ-./ β π
Two-Fluid Model
π4- Resistive Channel
π:- Reactive Channel
MattisβBardeen Conductivity: Anomalous Skin Effect in SC
π ' πΏ)
MB + CPW Theory
π 'πΏ) + CπΏ+
πΏ)πΏ+π '
Mattis Bardeen CPW Geometry 4K CPW Resonator
π π π
C
CPW Theory - Basics
πo
CPW Theory β Capacitance Vs. Geometry
πΆ`4πoπ=
S (um)
CPW Theory β Kinetic Inductance: Numerical Results
0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 250.5
1
1.5
2
2.5
3
3.5
4x 10β8
CPW Gap Width, S (um)
Lk (H
enry
/met
er)
w = 5 umw = 10 umw = 15 umw = 20 um
Strong Coupling
Strong Coupling
Experimental Apparatus β Custom 4K Cryostat, Design
Proposed Measurement - Phase
Coupling Regimes
Ξ = max π , πΎ = π = 250KHz
πΞ ~20
CPW-Rydberg
Ξ = πQ β π|
Schuster, Ph.D Thesis, (2007)
Measurement β SNR
Can increase photon number in cavity to increase seperation
Mattis β Bardeen Limited CPW: Quality Factor Data
0 5 10 15 20 25 30 350
2000
4000
6000
8000
10000
12000
14000
16000
CPW Gap Width (um)
Inte
rnal
Q
W = 5 um, DataW = 10 um, DataW = 20 um, DataW = 30 um, DataW = 50 um Data