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Stuart Ingleby Strathclyde University Glasgow Magnetometry Optimisation in Unshielded Environments

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Page 1: Magnetometry Optimisation in Unshielded Environments · Introduction Strathclyde University Quantum Sensors & Metrology Lab - Clocks, Magnetometry and Rota?on sensors March 2015 25/05/16

Stuart InglebyStrathclyde University

Glasgow

Magnetometry Optimisation in Unshielded Environments

Page 2: Magnetometry Optimisation in Unshielded Environments · Introduction Strathclyde University Quantum Sensors & Metrology Lab - Clocks, Magnetometry and Rota?on sensors March 2015 25/05/16

IntroductionStrathclydeUniversityQuantumSensors&MetrologyLab-Clocks,MagnetometryandRota?onsensorsMarch2015

25/05/16 Stuart Ingleby DAMOP 2016 2

Page 3: Magnetometry Optimisation in Unshielded Environments · Introduction Strathclyde University Quantum Sensors & Metrology Lab - Clocks, Magnetometry and Rota?on sensors March 2015 25/05/16

Introduction•  Unshielded

Magnetometry•  Surveying•  Seismology

•  Performance criteria•  Sensitivity•  Bandwidth•  Portable & scalable•  Arbitrary fields•  Noise rejection

25/05/16 Stuart Ingleby DAMOP 2016 3

Page 4: Magnetometry Optimisation in Unshielded Environments · Introduction Strathclyde University Quantum Sensors & Metrology Lab - Clocks, Magnetometry and Rota?on sensors March 2015 25/05/16

Introduction•  Unshielded

Magnetometry•  Surveying•  Seismology

•  Performance criteria•  Sensitivity•  Bandwidth•  Portable & scalable•  Arbitrary fields•  Noise rejection

25/05/16 Stuart Ingleby DAMOP 2016 4

•  Single-laser NMOR•  Software control & feedback•  Iterative optimisation

ADC16-bit

CurrentBuffers

Lock-in

Amp

FrequencyGenera=on

UserInterfaceFiAng

Page 5: Magnetometry Optimisation in Unshielded Environments · Introduction Strathclyde University Quantum Sensors & Metrology Lab - Clocks, Magnetometry and Rota?on sensors March 2015 25/05/16

Introduction•  Unshielded

Magnetometry•  Surveying•  Seismology

•  Performance criteria•  Sensitivity•  Bandwidth•  Portable & scalable•  Arbitrary fields•  Noise rejection

25/05/16 Stuart Ingleby DAMOP 2016 5

•  Single-laser NMOR•  Software control & feedback•  Iterative optimisation

ADC16-bit

CurrentBuffers

Lock-in

Amp

FrequencyGenera=on

UserInterfaceFiAng

Cs cell• 28 mm diameter• 2x10-6 torr Cs vapour• Paraffin anti-relaxation• 7 Hz intrinsic relaxation• Made in Fribourg [1]

[1] Castagna, Bison, Di Domenico, Hofer, Knowles, Macchione, Saudan, Weis, Appl. Phys. B 96, 763

Page 6: Magnetometry Optimisation in Unshielded Environments · Introduction Strathclyde University Quantum Sensors & Metrology Lab - Clocks, Magnetometry and Rota?on sensors March 2015 25/05/16

NMOR resonance

•  B0 // polarisation•  First-harmonic

response•  BRF modulation•  Software

•  Demodulation•  Phase

correction•  Regression

25/05/16 Stuart Ingleby DAMOP 2016 6

[2] T. Zigdon, A. D. Wilson-Gordon, S. Guttikonda, E. J. Bahr, O. Neitzke, S. M. Rochester, D. Budker, Opt. Express 18, 25494

Page 7: Magnetometry Optimisation in Unshielded Environments · Introduction Strathclyde University Quantum Sensors & Metrology Lab - Clocks, Magnetometry and Rota?on sensors March 2015 25/05/16

B0 Orientation & Gradient

•  B0 orientation•  B0 // polarisation

•  Relaxation [3]

25/05/16 Stuart Ingleby DAMOP 2016 7[3]S.Pustelny,D.F.JacksonKimball,S.M.Rochester,V.V.Yashchuk,D.Budker,Phys.Rev.A74,063406

Page 8: Magnetometry Optimisation in Unshielded Environments · Introduction Strathclyde University Quantum Sensors & Metrology Lab - Clocks, Magnetometry and Rota?on sensors March 2015 25/05/16

B0 optimisation•  Finite-field

optimisation1  Minimise Bx

By2  Set Bz3  Minimise

HWHM wrt ∇Bx ∇By ∇Bz

•  Convergence 2-3 iterations•  ΔB0 < 20 nT•  ∇Β < 2 nT/mm

25/05/16 Stuart Ingleby DAMOP 2016 8

Page 9: Magnetometry Optimisation in Unshielded Environments · Introduction Strathclyde University Quantum Sensors & Metrology Lab - Clocks, Magnetometry and Rota?on sensors March 2015 25/05/16

B0 optimisation•  Finite-field

optimisation1  Minimise Bx

By2  Set Bz3  Minimise

HWHM wrt ∇Bx ∇By ∇Bz

•  Convergence 2-3 iterations•  ΔB0 < 20 nT•  ∇Β < 2 nT/mm

25/05/16 Stuart Ingleby DAMOP 2016 9

Page 10: Magnetometry Optimisation in Unshielded Environments · Introduction Strathclyde University Quantum Sensors & Metrology Lab - Clocks, Magnetometry and Rota?on sensors March 2015 25/05/16

B0 optimisation•  Finite-field

optimisation1  Minimise Bx

By2  Set Bz3  Minimise

HWHM wrt ∇Bx ∇By ∇Bz

•  Convergence 2-3 iterations•  ΔB0 < 20 nT•  ∇Β < 2 nT/mm

25/05/16 Stuart Ingleby DAMOP 2016 10

Page 11: Magnetometry Optimisation in Unshielded Environments · Introduction Strathclyde University Quantum Sensors & Metrology Lab - Clocks, Magnetometry and Rota?on sensors March 2015 25/05/16

B0 optimisation•  Finite-field

optimisation1  Minimise Bx

By2  Set Bz3  Minimise

HWHM wrt ∇Bx ∇By ∇Bz

•  Convergence 2-3 iterations•  ΔB0 < 20 nT•  ∇Β < 2 nT/mm

25/05/16 Stuart Ingleby DAMOP 2016 11

Page 12: Magnetometry Optimisation in Unshielded Environments · Introduction Strathclyde University Quantum Sensors & Metrology Lab - Clocks, Magnetometry and Rota?on sensors March 2015 25/05/16

B0 optimisation•  Finite-field

optimisation1  Minimise Bx

By2  Set Bz3  Minimise

HWHM wrt ∇Bx ∇By ∇Bz

•  Convergence 2-3 iterations•  ΔB0 < 20 nT•  ∇Β < 2 nT/mm

25/05/16 Stuart Ingleby DAMOP 2016 12

Page 13: Magnetometry Optimisation in Unshielded Environments · Introduction Strathclyde University Quantum Sensors & Metrology Lab - Clocks, Magnetometry and Rota?on sensors March 2015 25/05/16

B0 optimisation•  Finite-field

optimisation1  Minimise Bx

By2  Set Bz3  Minimise

HWHM wrt ∇Bx ∇By ∇Bz

•  Convergence 2-3 iterations•  ΔB0 < 20 nT•  ∇Β < 2 nT/mm

25/05/16 Stuart Ingleby DAMOP 2016 13

Page 14: Magnetometry Optimisation in Unshielded Environments · Introduction Strathclyde University Quantum Sensors & Metrology Lab - Clocks, Magnetometry and Rota?on sensors March 2015 25/05/16

B0 optimisation•  Finite-field

optimisation1  Minimise Bx

By2  Set Bz3  Minimise

HWHM wrt ∇Bx ∇By ∇Bz

•  Convergence 2-3 iterations•  ΔB0 < 20 nT•  ∇Β < 10 nT/mm

25/05/16 Stuart Ingleby DAMOP 2016 14

Page 15: Magnetometry Optimisation in Unshielded Environments · Introduction Strathclyde University Quantum Sensors & Metrology Lab - Clocks, Magnetometry and Rota?on sensors March 2015 25/05/16

BRF optimisation•  Signal

•  Saturation

25/05/16 Stuart Ingleby DAMOP 2016 15

Page 16: Magnetometry Optimisation in Unshielded Environments · Introduction Strathclyde University Quantum Sensors & Metrology Lab - Clocks, Magnetometry and Rota?on sensors March 2015 25/05/16

Optimised resonance

•  HWHM 680 → 108 Hz (7 Hz intrinsic) • Sensitivity 228 → 20 pT.Hz-1/2

25/05/16 Stuart Ingleby DAMOP 2016 16

Page 17: Magnetometry Optimisation in Unshielded Environments · Introduction Strathclyde University Quantum Sensors & Metrology Lab - Clocks, Magnetometry and Rota?on sensors March 2015 25/05/16

Stability & Dynamic range

25/05/16 Stuart Ingleby DAMOP 2016 17

5 μT

50 μT

•  Dipole ~ 8 mA.m2

•  Location < 5 mm

Page 18: Magnetometry Optimisation in Unshielded Environments · Introduction Strathclyde University Quantum Sensors & Metrology Lab - Clocks, Magnetometry and Rota?on sensors March 2015 25/05/16

Response & Noise measurement•  Software PID

feedback•  Self-optimised

•  Phase•  Gain

•  1 Hz field tracking

25/05/16 Stuart Ingleby DAMOP 2016 18

Page 19: Magnetometry Optimisation in Unshielded Environments · Introduction Strathclyde University Quantum Sensors & Metrology Lab - Clocks, Magnetometry and Rota?on sensors March 2015 25/05/16

Summary•  QT Hub: application of QT to devices•  Unshielded vapour cell magnetometry•  Scalable, flexible ☞ Hardware < Software•  Arbitrary fields ☞ Studying B0 & ∇B•  Sensitivity ☞ Noise rejection

25/05/16 Stuart Ingleby DAMOP 2016 19

Strathclyde QT Sensors & Metrology HubAidan Arnold, Paul Griffin, Erling RiisYogeshwar Kale, Stuart InglebyVictoria Henderson, Rachel Elvin, James McGilligan