Method and device for measuring a magnetic field by synchronised excitations

• US 9,797,966 B2
• Filed: 07/07/2014
• Issued: 10/24/2017
• Est. Priority Date: 07/08/2013
• Status: Expired due to Fees

• Current Assignee: Commissariat a L'Energie Atomique (French Alternative Energies and Atomic Energy Commission)
• Original Assignee: Commissariat a L'Energie Atomique (French Alternative Energies and Atomic Energy Commission)
• Inventors: Le Prado, Matthieu, Bertrand, Francois, Corsi, Marie-Constance, Delevoye, Elisabeth, Morales, Sophie
• Primary Examiner(s): Arana, Louis
• Application Number:
  US14/324,379
• Publication Number:
  US 20150008916A1
• Time in Patent Office: 1,205 Days
• Field of Search: 324304, 324302, 324318, 324322
• CPC Class Codes: G01R 33/04 using the flux-gate principle
• CPC Class Codes: G01R 33/26 using optical pumping

Abstract

The invention relates to a magnetic field measurement device, including a detector (4) configured to measure the amplitude of an output signal at a harmonic of an oscillation frequency of an excitation source, said amplitude being proportional to the magnetic field (B) to be measured, characterised in that it comprises an excitation circuit configured to associate with a principal excitation source (B₁cosωt) oscillating at a principal oscillation frequency at least one secondary excitation source (B₂cos(ω/3t+Φ₂)) oscillating at a secondary oscillation frequency that is a fraction of the principal oscillation frequency, said fraction being odd if said harmonic is odd, and even if said harmonic is even.

Claims

1. A magnetic field measurement device, comprising:

a cell filled with a gas;

a laser source configured to emit a polarized optical pumping beam towards the cell along a propagation direction;

a magnetic resonance excitation circuit comprising a principal excitation source configured to oscillate at a principal oscillation frequency and at least one secondary excitation source configured to oscillate at a secondary oscillation frequency that is a fraction 1/n of the principal oscillation frequency;

a detector configured to measure an amplitude of an output signal at a harmonic of the principal oscillation frequency, said amplitude being proportional to the magnetic field to be measured,

wherein the detector is a photodetector configured to output as said output signal a signal representative of the beam that passed through the cell, and

the magnetic resonance excitation circuit comprises a coil surrounding the cell and a frequency generator powering the coil, the magnetic resonance excitation circuit being configured to associate magnetic fields comprising a principal sinusoidal magnetic excitation field at the principal oscillation frequency and at least one secondary sinusoidal magnetic excitation field at the secondary oscillation frequency, n being odd.

2. The device according to claim 1, wherein said harmonic is the fundamental of the principal oscillation frequency.

3. The device according to claim 1, further comprising a slaving circuit configured to inject a current into the coil so as to generate a compensating magnetic field creating a zero sum with the magnetic field to be measured.

4. The device according to claim 1, wherein the detector is a synchronous detector tuned to said harmonic.

5. A magnetic field measurement device, comprising:

a magnetic resonance excitation circuit comprising a principal excitation source configured to oscillate at a principal oscillation frequency and at least one secondary excitation source configured to oscillate at a secondary oscillation frequency that is a fraction 1/n of the principal oscillation frequency;

a detector configured to measure an amplitude of an output signal at a harmonic of the principal oscillation frequency, said amplitude being proportional to the magnetic field to be measured,

wherein the magnetic resonance excitation circuit is configured to associate alternating excitation currents output to an excitation coil surrounding a magnetic core, wherein the alternating excitation currents comprise a principal excitation current at the principal oscillation frequency and at least one secondary excitation current at the secondary oscillation frequency, and wherein n is even.

6. The device according to claim 5, wherein said harmonic is the order 2 or order 4 harmonic of the principal oscillation frequency.

7. A method of measuring a magnetic field, said method comprising:

emitting, from a laser source, a polarized pumping beam towards a cell filled with gas along a propagation direction;

operating a magnetic resonance excitation circuit which comprises a coil surrounding the cell and a frequency generator that powers the coil to associate magnetic fields comprising a principal sinusoidal magnetic excitation field at a principal oscillation frequency and at least one secondary sinusoidal magnetic excitation field at a secondary oscillation frequency that is a fraction 1/n of the principal oscillation frequency, n being odd,

measuring an amplitude of a signal at a harmonic of said principal oscillation frequency, said amplitude being proportional to the magnetic field to be measured,

wherein the measurement of the amplitude of the signal is performed by a photodetector that outputs a signal representative of the beam that passed through the cell.

8. A method of measuring a magnetic field, said method comprising:

operating a magnetic resonance excitation circuit to supply an excitation coil surrounding a magnetic core with a principal excitation current at a principal oscillation frequency and at least one secondary excitation current at a secondary oscillation frequency that is a fraction 1/n of the principal oscillation frequency, n being even; and

measuring, using a detection coil surrounding the magnetic core, an amplitude of a signal at a harmonic of said principal oscillation frequency, said amplitude being proportional to the magnetic field to be measured.