Method for automatically shimming a high resolution NMR magnet

• US 5,343,151 A
• Filed: 03/11/1993
• Issued: 08/30/1994
• Est. Priority Date: 03/11/1993
• Status: Expired due to Term

• Current Assignee: Bruker Instruments Incoporated (Bruker Corporation)
• Original Assignee: Bruker Instruments Incoporated (Bruker Corporation)
• Inventors: Sprenger, Peter, Cory, David G.
• Primary Examiner(s): ARANA, LOUIS M
• Application Number:
  US08/029,906
• Time in Patent Office: 537 Days
• Field of Search: 324/320, 324/319, 324/318, 324/322, 324/307, 324/309, 128/653.5
• US Class Current: 324/320
• CPC Class Codes: G01R 33/3875 using correction coil assemblies, e.g. active shimming

Abstract

A plurality of measurements are made with a probe containing a material sample with a known frequency spectrum. The probe is positioned in one spot in the magnet bore in the presence of a field gradient along a predetermined axis. Prior to each measurement, the gradient strength is increased by a predetermined constant amount. The resulting measurement values are mathematically manipulated to yield a set of values which can be used to set the shim coil currents based on known equations for the field generated by each shim coil. The method can be used with a material sample with a simple NMR spectrum or a complex NMR spectrum. If a sample with a complex NMR spectrum is employed in the measurement, the spectral complexity can be removed by deconvolution during the manipulation of the measurement values.

Claims

1. In an NMR spectrometer having coils for generating a main magnetic field having a direction over a sample volume, means for passing field current through the coils, a gradient coil, means for passing a gradient current through the gradient coil to generate a magnetic field gradient along a predetermined direction within the sample volume, a method for correcting the main magnetic field to a spatially uniform field along the predetermined direction over the sample volume by selectively adjusting the magnitude of the field current, the method comprising the steps of:

A. inserting a material sample containing NMR-active nuclei into the sample volume;

B. setting the gradient current to a predetermined value;

C. performing an NMR experiment to acquire a frequency spectrum data set of the sample while the gradient current remains at the predetermined value set in step B;

D. adjusting the gradient current to a new value to change the gradient field;

E. repeating steps C and D a predetermined number of times to acquire multiple frequency spectrum data sets with different times and gradient field magnitudes;

F. manipulating the frequency spectrum data sets acquired in step E to produce a new data set relating field strength to spatial position; and

G. using the new data set produced in step F to adjust the magnitude of the field current.

2. In an NMR spectrometer, the method according to claim 1 wherein step D comprises the step of:

D1. incrementing the gradient coil current between NMR experiments.

3. In an NMR experiment, the method according to claim 1 wherein step F comprises the steps of:

F1. generating amplitude modulated data sets;

F2. Fourier transforming the amplitude modulated data sets generated in step F1 at constant time to produce first Fourier transform results;

F3. processing the first Fourier transform results in step F2 to obtain a pure absorption mode data set; and

F4. Fourier transforming the pure absorption mode data set generated in step F3 to generate the new data set relating field strength to spatial position.

4. In an NMR spectrometer, the method according to claim 3 wherein step F1 comprises the step of:

F1A. generating quadrature data by selectively combining the frequency spectrum data sets acquired in step E for each time and gradient field.

5. In an NMR spectrometer, the method according to claim 4 wherein step F2 comprises the step of:

F2A. calculating the real and imaginary parts of the Fourier transformation of the quadrature data generated in step F1A.

6. In an NMR spectrometer, the method according to claim 5 wherein step F3 comprises the steps of:

F3A. scaling the real and imaginary parts calculated in step F2A; and

F3B. combining the scaled real and imaginary parts to form the pure absorption mode data set.

7. In an NMR spectrometer having coils for generating a main magnetic field having a direction over a sample volume, a shim coil for generating a shim field within the sample volume, and means for passing a shim current with a selected magnitude through the shim coil, a method for correcting the main magnetic field to a spatially uniform field along a predetermined direction over the sample volume by selectively adjusting the magnitude of the shim current, the method comprising the steps of:

A. inserting a material sample containing NMR-active nuclei into the sample volume;

B. setting the shim current to a predetermined value;

C. performing an NMR experiment to acquire a frequency spectrum data set of the sample;

D. adjusting the shim current to a new value;

E. repeating steps C and D a predetermined number of times to acquire multiple frequency spectrum data sets;

F. manipulating the frequency spectrum data sets acquired in step E to produce a new data set relating field strength to spatial position;

G. using the new data set produced in step F to adjust the magnitude of the shim coil current.

8. In an NMR spectrometer, the method according to claim 7 wherein step D comprises the step of:

D1. adjusting the shim current so that the shim coil produces a shim field having a magnitude which varies linearly along the predetermined direction.

9. In an NMR spectrometer, the method according to claim 7 wherein step E comprises the step of:

E1. repeating the NMR experiment a sufficient number of times in order to acquire data sets in which the shim field increases in magnitude along the predetermined direction and data sets in which the shim field decreases in magnitude along the predetermined direction.

10. In an NMR spectrometer, the method according to claim 9 wherein step F comprises the steps of:

F1. selectively combining data sets in which the shim field is aligned with the main magnetic field with data sets in which the shim field is opposed to the main magnetic field to form a plurality of combined sets;

F2. Fourier transforming each of the plurality of combined sets formed in step F1 to form a first transformed result;

F3. rescaling the first transformed result generated in step F2;

F4. Fourier transforming the rescaled result formed in step F3 to generate a second transformed result; and

F5. using the second transformed result of step F4 to control the means for passing a shim current through the shim coil.

11. In an NMR spectrometer, the method according to claim 10 wherein step F1 comprises the steps of:

F1A. forming the sum of data sets in which the shim field is aligned with the main magnetic field with data sets in which the shim field is opposed to the main magnetic field; and

F1B. forming the difference between data sets in which the shim field is aligned with the main magnetic field and data sets in which the shim field is opposed to the main magnetic field.

12. In an NMR spectrometer, the method according to claim 11 wherein step F3 comprises the steps of:

F3A. using an interpolation function to rescale the Fourier transformed results of step F2 by the value [t^-1 ] t/1, where t represents time.

13. In an NMR spectrometer, the method according to claim 10 wherein step F5 comprises the steps of:

F5A. fitting a mathematical function to the second transformed result produced in step F4; and

F5B. using the function determined in step F5A to control the means for passing a shim current through the shim coil.

14. In an NMR spectrometer, the method according to claim 13 wherein step F5A comprises the steps of:

F5A1. fitting a mathematical function to the second transformed result by means of a least squares operation.

15. In an NMR spectrometer, the method according to claim 13 wherein step F5A comprises the step of:

F5A2. selecting data points in the second transformed result for each position which have the largest magnitude.

16. In an NMR spectrometer, the method according to claim 10 wherein step F3 comprises the steps of:

F3B. deconvolving the Fourier transformed results with a predetermined spectral response of the material sample.

17. In an NMR spectrometer, the method according to claim 10 further comprising the steps of:

H. increasing the resolution of the NMR spectrometer; and

I. repeating steps A through G.

18. In an NMR spectrometer, the method according to claim 7 wherein step C comprises the step of:

C1. spinning the sample during acquisition of an NMR signal.

19. In an NMR spectrometer, the method according to claim 7 wherein step C comprises the step of:

C2. acquiring the frequency spectrum data at an NMR resonant frequency.

20. In an NMR spectrometer having coils for generating a main magnetic field having a z-axis direction over a sample volume, a z-shim coil for generating an on-axis shim field within the sample volume, and means for passing a first shim current with a selected magnitude through the z-shim coil, a plurality of additional shim coils, means for passing a plurality of second shim currents through the plurality of additional shim coils, a method for correcting the main magnetic field to a spatially uniform field along the z-axis direction over the sample volume by selectively adjusting the magnitude of the first shim current and the plurality of second shim currents, the method comprising the steps of:

A. inserting a material sample containing NMR-active nuclei into the sample volume;

B. setting the first shim current to a predetermined value;

C. exciting the sample nuclei at an NMR resonant frequency and detecting a free induction decay signal to acquire a frequency spectrum data set of the sample;

D. incrementing the first shim current to a new value;

E. repeating steps C and D a predetermined number of times to acquire multiple frequency spectrum data sets;

F. Fast Fourier transform the multiple frequency data sets acquired in step E to generate first transformed data;

G. interpolating the first transformed data to generate field map data representing magnetic field strength versus position;

H. selecting data points in the field map data generated in step G for each position which have the largest field magnitude;

I. fitting a curve to the data points selected in step H to obtain coefficients describing the shim coil currents necessary to correct inhomogeneities in the main magnetic field; and

J. using the coefficients obtained in step I to adjust the magnitude of the first shim coil current and the magnitude of the plurality of second shim coil currents.

21. In an NMR spectrometer, the method according to claim 20 wherein step F comprises the steps of:

F1. generating quadrature data by selectively combining the frequency spectrum data sets acquired in step E for each time and gradient field.

F2. Fourier transforming the quadrature data generated in step F1 at constant time to produce first Fourier transformed results;

22. In an NMR spectrometer, the method according to claim 21 wherein step F further comprises the step of:

F3. calculating the real and imaginary parts of the Fourier transformation of the quadrature data generated in step F2.

23. In an NMR spectrometer, the method according to claim 22 wherein step G comprises the steps of:

G1. scaling the real and imaginary parts calculated in step F3;

G2. combining the scaled real and imaginary parts to form the pure absorption mode data set; and

G3. Fourier transforming the pure absorption mode data set to generate the field map data.

24. In an NMR spectrometer, the method according to claim 23 wherein step I comprises the step of:

I1. using a least squares curve fitting method.

25. In an NMR spectrometer, the method according to claim 24 wherein step C comprises the step of:

C1. spinning the sample.