A Portable Ultrasensitive SERF Atomic Magnetometer for Biomagnetic Measurements - PowerPoint PPT Presentation

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A Portable Ultrasensitive SERF Atomic Magnetometer for Biomagnetic Measurements

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... 1 Z Li,2 R Wakai,3 N Proite,1 P Cook,1 T Walker1. 1 Department of Physics, UW-Madison. 2 Center for Clinical Neurosciences, UT-Houston Health Science Center ... – PowerPoint PPT presentation

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Title: A Portable Ultrasensitive SERF Atomic Magnetometer for Biomagnetic Measurements


1
A Portable Ultrasensitive SERF Atomic
Magnetometer for Biomagnetic Measurements
  • R Wyllie,1 Z Li,2 R Wakai,3 N Proite,1 P Cook,1 T
    Walker1

1 Department of Physics, UW-Madison 2 Center
for Clinical Neurosciences, UT-Houston Health
Science Center 3 Department of Medical
Physics, UW-Madison
2
Requirements for Biomagnetic Measurements
  • Sensitivity
  • Bandwidth100Hz
  • Portability

3
Atomic SERF Magnetometer
Note Spin-exchange collisions do not affect G
Romalis et. al., Nature, 422, 596, 2003
4
Experimental Concerns
  • For full SERF sensitivity, precession rateltltspin
    relaxation rate
  • Magnetic shielding, careful nulling using
    Helmholtz coils
  • Noise Sources
  • Nonmagnetic, technical noise (e.g. vibrations,
    thermal fluctuations, etc.)
  • Johnson noise (thermal electron motion)

5
Technical Noise from an hot air heated cell scheme
6
Z-Mode
  • Goal use lock-in technique to extract signal
    from nonmagnetic noise
  • Apply a large, oscillating kHz magnetic field in
    z-direction (along pump)
  • For best sensitivity, Larmor frequencyparametric
    frequency, sets Bz430nT
  • Use lock-in detection of signal
  • Two detection directions
  • Z1, Sy signal oscillates at wz
  • Z2, Sx signal oscillates at 2wz
  • Zero transverse fields produce no
    signalbackground free

7
Z-Mode Results
  • Significantly reduces nonmagnetic noise
  • Retains sensitivity and bandwidth of normal SERF
    magnetometer operation

8
Current Setup
  • Rb 87 with N2 (100T) buffer gases
  • Circularly polarized pump at 795nm
  • Linearly polarized probe at 780nm
  • Cell heated to 180 C

9
Technical Improvements
  • Plastic, ceramic, and Teflon parts reduce Johnson
    noise, improve portability
  • Matched resistive film heaters create little
    magnetic field, allow smaller apparatus, less
    noise (similar to Kitching et al heating scheme)
  • RF heating, atoms not affected by high frequency
    (MHz) fields
  • Insulation allows subject to be 1cm away from
    cell
  • Easy conversion to gradiometer with pump tube

10
Adult MCG
11
Acknowledgments
  • This work funded by a grant from the NIH
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