Field-frequency lock system for magnetic resonance system

• US 6,242,915 B1
• Filed: 08/27/1999
• Issued: 06/05/2001
• Est. Priority Date: 08/27/1999
• Status: Expired due to Fees

• Current Assignee: General Electric Company
• Original Assignee: General Electric Company
• Inventors: Hurd, Ralph E.
• Primary Examiner(s): Oda, Christine
• Assistant Examiner(s): Vargas, Dixomara
• Application Number:
  US09/384,945
• Time in Patent Office: 648 Days
• Field of Search: 324/309, 324/307, 324/314
• US Class Current: 324/309
• CPC Class Codes: G01R 33/24 for measuring direction or magnitude of magnetic fields or magnetic flux
• CPC Class Codes: G01R 33/3607 RF waveform generators, e.g. frequency generators, amplitude-, frequency- or phase modulators or shifters, pulse programmers, digital to analog converters for the RF signal, means for filtering or attenuating of the RF signal
• CPC Class Codes: G01R 33/389 Field stabilisation , e.g. by field measurements and control means or indirectly by current stabilisation

Abstract

A field-frequency lock system for an MRI system includes a microcoil and resonant sample located to sense changes in the polarizing magnetic field. Changes are detected as a shift in frequency of the NMR signal produced by the resonant sample, and the frequency shift is used to compensate the MRI system. Compensation is achieved by adjusting the RF reference signal employed in the MRI system transceiver.

Claims

1. In an MRI system having a magnet for producing a polarizing magnetic field B₀ in a region, and a gradient coil assembly for producing magnetic field gradients in a subject to be imaged located in the region, a field-frequency lock system which comprises:

a microcoil located outside the gradient coil assembly and in the region in which the polarizing magnetic field B₀ is produced;

a resonant sample disposed adjacent the microcoil and containing a material that produces a signal when the microcoil is energized with an rf pulse;

transmit means for producing an rf pulse that is applied to the microcoil;

receive means for acquiring a signal from the microcoil that is produced by the resonant sample material;

a frequency comparator for measuring the difference frequency (Δ

ω

) between the frequency of the acquired signal and a reference frequency which corresponds to a frequency produced by the resonant sample material when the polarizing magnetic field B₀ is at a nominal value; and

means responsive to the difference frequency Δ

ω

for compensating the operation of the MRI system as it performs a scan on the subject for variations in the magnitude of the polarizing magnetic field B₀.

2. The system as recited in claim 1 in which the MRI system includes a transceiver which produces rf excitation pulses and acquires NMR signals during the scan of the subject, and the means for compensating the operation of the MRI system adjusts the frequency of a reference signal employed by the transceiver.

3. The system as recited in claim 1 in which the resonant sample contains fluoride spins (¹⁹F).

4. The system as recited in claim 2 in which the microcoil is wound around the resonant sample.

5. The system as recited in claim 1 in which the resonant sample material produces a nuclear magnetic resonance signal.

6. The system as recited in claim 1 in which the gradient coil assembly is actively shielded and the microcoil is located outside the active shield.

7. A method for compensating an MRI system for changes in the polarizing magnetic field of the MRI system, the steps comprising:

monitoring a microcoil positioned in the polarizing magnetic field at a location in which magnetic field gradients are minimal;

acquiring an NMR signal from a resonant sample disposed adjacent the microcoil;

producing a difference signal by comparing the frequency of the acquired NMR signal with the frequency of a reference signal that is indicative of the NMR signal produced by the resonant sample when the polarizing magnetic field has a nominal value; and

producing a compensating signal for the MRI system from the difference signal which offsets changes in the polarizing magnetic field.

8. The method as recited in claim 7 in which the resonant sample produces an NMR signal having a substantially different frequency than the NMR signals produced by a subject being scanned with the MRI system.

9. The system as recited in claim 8 in which the resonant sample includes fluorine spins (¹⁹F) and the method includes controlling the temperature of the resonant sample to maintain it at a constant temperature.

10. The system as recited in claim 7 which includes:

adjusting the frequency of a reference signal in the MRI system with the compensating signal.

11. The system as recited in claim 10 in which the adjusted reference signal is employed during a scan to demodulate NMR signals produced when performing a scan.

12. The system as recited in claim 10 in which the adjusted reference signal is employed to produce rf excitation pulses when performing a scan.