Apparatus and method for increasing the sensitivity of a nuclear magnetic resonance probe

• US 4,633,181 A
• Filed: 08/11/1983
• Issued: 12/30/1986
• Est. Priority Date: 08/11/1983
• Status: Expired due to Term

• Current Assignee: Regents of the University of California (University of California)
• Original Assignee: Regents of the University of California (University of California)
• Inventors: Koretsky, Alan P., Murphy-Boesch, Joseph A.
• Primary Examiner(s): Levy, Stewart J.
• Assistant Examiner(s): NOT, DEFINED
• Application Number:
  US06/522,150
• Time in Patent Office: 1,237 Days
• Field of Search: 324/307, 324/311, 324/313, 324/314, 324/315, 324/316, 324/318, 324/322, 324/61 QS, 324/61 QL, 324/57 Q, 324/128
• US Class Current: 324/322
• CPC Class Codes: G01R 33/3628 Tuning/matching of the transmit/receive coil

Abstract

The discovery has been made that coil-to-ground parasitic losses substantially reduce the sensitivity of a nuclear magnetic resonance probe used in nuclear magnetic resonance analyses of lossy dielectic (i.e., relatively conductive) samples, such as biological tissue. A probe circuit is disclosed in which a balancing impedance is inserted for substantially reducing the influence of coil-to-ground parasitics. The probe circuit resulting from the insertion of the balancing impedance markedly increases sensitivity. Concomittantly, the quality factor of the probe circuit and the signal-to-noise ratio of nuclear magnetic resonance signals are substantially improved. The disclosed probe circuit can be incorporated in nuclear magnetic resonance analysis systems where the sample coil is either implanted or placed on the surface of a sample; where the sample coil forms a portion of a large-scale imaging system; or the sample coil is used in a traditional analytical mode with a sample contained in a glass tube.

Claims

1. A nuclear magnetic resonance probe circuit having an improved quality factor in the presence of coil-to-ground parasitics encountered in nuclear magnetic resonance analysis of a specimen, comprising:

a sample coil having a nominal inductance, the sample coil being positioned in close proximity to the specimen;

a tuning circuit element connected to the sample coil, the sample coil and tuning circuit element substantially forming a resonant circuit tuned to a selected Larmor frequency; and

a balanced impedance circuit means connected to the sample coil and tuning circuit element for controlling the voltage across the sample coil in the presence of leakage current from the sample coil through the specimen to ground in a manner to balance the leakage currents as seen from the ends of the sample coil, thereby reducing the influence of coil-to-ground parasitics additional to any coil-to-ground parasitic attributable solely to leakage current directly from the sample coil to ground.

2. The nuclear magnetic resonance probe circuit of claim 1 wherein the tuning circuit element comprises a tuning capacitor and the balanced impedance circuit means comprises a balanced impedance matching capacitance connected in series circuit with the sample coil for balancing the voltage across the sample coil.

3. The nuclear magnetic resonance probe circuit of claim 2 wherein the balanced impedance matching capacitance comprises a first impedance matching capacitor connected between the sample coil and an ungrounded output terminal and a second impedance matching capacitor connected between the sample coil and a grounded output terminal, the first impedance matching capacitor and the second impedance matching capacitor each having a capacitance which is approximately twice the capacitance of the tuning capacitor.

4. The nuclear magnetic resonance probe circuit of claim 1 wherein the selected Larmor frequency is approximately 100 MHz and the sample coil has a nominal inductance of approximately 100 nanohenries.

5. A nuclear magnetic resonance probe circuit having an improved quality factor in the presence of coil-to-ground parasitics encountered in nuclear magnetic resonance analysis of a specimen, comprising:

a sample coil having a nominal inductance, the sample coil being positioned in close proximity to the specimen;

a tuning capacitor connected to the sample coil, the sample coil and tuning capacitor substantially forming a resonant circuit tuned to a selected Larmor frequency;

a first impedance matching capacitor connected between the sample coil and an ungrounded output terminal; and

a second impedance matching capacitor connected between the sample coil and a grounded output terminal;

the sample coil being connected in series circuit between the first and second impedance matching capacitors across the ungrounded and grounded output terminals;

the first and second impedance matching capacitors controlling the voltage across the sample coil in the presence of leakage current from the sample coil through the specimen to ground in a manner to balance the leakage currents as seen from the ends of the sample coil, thereby reducing the influence of coil-to-ground parasitics additional to any coil-to-ground parasitic attributable solely to leakage current directly from the sample coil to ground.

6. The nuclear magnetic resonance probe circuit of claim 5 wherein the tuning capacitor is connected in parallel circuit with the sample coil.

7. The nuclear magnetic resonance probe circuit of claim 6 wherein the tuning capacitor is positioned in close proximity to the specimen.

8. The nuclear magnetic resonance probe circuit of claim 5 wherein the tuning capacitor is connected between the grounded output terminal and a first junction, where the first impedance matching capacitor is connected to the sample coil, and wherein the second impedance matching capacitor is connected between the sample coil and a second junction, where the tuning capacitor is connected to the grounded output terminal.

9. The nuclear magnetic resonance probe circuit of claim 8, further comprising an additional capacitor connected in parallel circuit with the sample coil, the parallel circuit formed by the sample coil and additional capacitor being connected in series circuit between the first and second impedance matching capacitors across the ungrounded and ground output terminals.

10. The nuclear magnetic resonance probe circuit of claim 9 wherein the second impedance matching capacitor and the additional capacitor are positioned in close proximity to the specimen.

11. The nuclear magnetic resonance probe circuit of claim 5 wherein the tuning capacitor is adjustable for tuning the resonant circuit formed substantially by the sample coil and tuning capacitor to a selected Larmor frequency.

12. The nuclear magnetic resonance probe circuit of claim 8 wherein the tuning capacitor is adjustable for tuning the resonant circuit formed substantially by the sample coil and tuning capacitor to a selected Larmor frequency.

13. The nuclear magnetic resonance probe circuit of claim 5 wherein at least one of the first and second impedance matching capacitors is adjustable for matching the impedance across the ungrounded and grounded output terminals to a predetermined impedance.

14. The nuclear magnetic resonance probe circuit of claim 13 wherein the predetermined impedance is approximately 50 ohms.

15. The nuclear magnetic resonance probe circuit of claim 5 wherein the first impedance matching capacitor and the second impedance matching capacitor each have a capacitance which is approximately twice the capacitance of the tuning capacitor.

16. The nuclear magnetic resonance probe circuit of claim 5 wherein the selected Larmor frequency is approximately 100 MHz and the sample coil has a nominal inductance of approximately 100 nanohenries.

17. A nuclear magnetic resonance probe circuit having an improved quality factor in the presence of coil-to-ground parasitics encountered in nuclear magnetic resonance analysis of a specimen, comprising:

a sample coil having a nominal inductance, the sample coil being positioned in close proximity to the specimen, the sample coil being connected between a first node and a second node;

a tuning capacitor connected between the first and second nodes, the sample coil and tuning capacitor substantially forming a parallel resonant circuit resonant at a selected Larmor frequency;

a first impedance matching capacitor connected between the first node and an underground output terminal; and

a second impedance matching capacitor connected between the second node and a grounded output terminal;

the parallel resonant circuit formed substantially by the sample coil and tuning capacitor being connected in series circuit between the first and second impedance matching capacitors across the ungrounded and grounded output terminals;

the first and second impedance matching capacitors controlling the voltage across the sample coil in the presence of leakage current from the sample coil through the specimen to ground in a manner to balance the leakage currents as seen from the ends of the sample coil, thereby reducing the influence of coil-to-ground parasitics additional to any coil-to-ground parasitic attributable solely to leakage current directly from the sample coil to ground.

18. The nuclear magnetic resonance probe circuit of claim 17 wherein the tuning capacitor is positioned in close proximity to the specimen.

19. The nuclear magnetic resonance probe circuit of claim 17 wherein the tuning capacitor is adjustable for tuning the parallel resonant circuit formed substantially by the sample coil and tuning capacitor to a selected Larmor frequency.

20. The nuclear magnetic resonance probe circuit of claim 17 wherein at least one of the first and second impedance matching capacitors is adjustable for matching the impedance across the grounded and ungrounded output terminals to a predetermined impedance.

21. The nuclear magnetic resonance probe circuit of claim 20 wherein the predetermined impedance is approximately 50 ohms.

22. The nuclear magnetic resonance probe circuit of claim 17 wherein the first impedance matching capacitor and the second impedance matching capacitor each have a capacitance which is approximately twice the capacitance of the tuning capacitor.

23. The nuclear magnetic resonance probe circuit of claim 17 wherein the selected larmor frequency is approximately 100 MHz and the sample coil has a nominal inductance of approximately 100 nanohenries.

24. A nuclear magnetic resonance probe circuit having an improved quality factor in the presence of coil-to-ground parasitics encountered in nuclear magnetic resonance analysis of a specimen, comprising:

a sample coil having a nominal inductance, the sample coil being positioned in close proximity to the specimen, the sample coil being connected between a first node and a second node;

a tuning capacitor connected between the first node and a grounded output terminal, the sample coil and tuning capacitor substantially forming a parallel resonant circuit resonant at a selected Larmor frequency;

a first impedance matching capacitor connected between the first node and an ungrounded output terminal; and

a second impedance matching capacitor connected between the second node and the grounded output terminal;

the sample coil being connected in series circuit between the first and second impedance matching capacitors across the ungrounded and grounded output terminals;

the first and second impedance matching capacitors controlling the voltage across the sample coil in the presence of leakage current from the sample coil through the specimen to ground in a manner to balance the leakage currents as seen from the ends of the sample coil, thereby reducing the influence of coil-to-ground parasitics additional to any coil-to-ground parasitic attributable solely to leakage current directly from the sample coil to ground.

25. The nuclear magnetic resonance probe circuit of claim 24, further comprising an additional capacitor connected in parallel circuit with the sample coil between the first and second nodes, the parallel circuit formed by the sample coil and additional capacitor being connected in series circuit between the first and second impedance matching capacitors across the ungrounded and grounded output terminals.

26. The nuclear magnetic resonance probe circuit of claim 25 wherein the second impedance matching capacitor and the additional capacitor are positioned in close proximity to the specimen.

27. The nuclear magnetic resonance probe circuit of claim 24 wherein the tuning capacitor is adjustable for tuning the parallel resonant circuit formed substantially by the sample coil and tuning capacitor to a selected Larmor frequency.

28. The nuclear magnetic resonance probe circuit of claim 24 wherein at least one of the first and second impedance matching capacitors is adjustable for matching the impedance across the grounded and ungrounded output terminals to a predetermined impedance.

29. The nuclear magnetic resonance probe circuit of claim 28 wherein the predetermined impedance is approximately 50 ohms.

30. The nuclear magnetic resonance probe circuit of claim 24 wherein the first impedance matching capacitor and the second impedance matching capacitor each have a capacitance which is approximately twice the capacitance of the tuning capacitor.

31. The nuclear magnetic resonance probe circuit of claim 24 wherein the selected Larmor frequency is approximately 100 MHz and the sample coil has a nominal inductance of approximately 100 nanohenries.

32. A method for improving the signal-to-noise ratio of nuclear magnetic resonance signals detected in the presence of coil-to-ground parasitics encountered in nuclear magnetic resonance analysis of a specimen by a probe circuit having a sample coil and a tuning circuit element, the sample coil and tuning circuit element substantially forming a resonant circuit across an ungrounded output terminal and a grounded output terminal, the resonant circuit being tuned to a selected Larmor frequency, comprising the steps of:

positioning the sample coil in close proximity to the specimen; and

inserting a balanced impedance circuit means connected to the sample coil and tuning circuit element for controlling the voltage across the sample coil in the presence of leakage current from the sample coil through the specimen to ground in a manner to balance the leakage currents as seen from the ends of the sample coil, whereby the influence of coil-to-ground parasitics additional to any coil-to-ground parasitic attributable solely to leakage current directly from the sample coil to ground is reduced.

33. The method of claim 32 wherein the tuning circuit element comprises a tuning capacitor and the balanced impedance circuit means comprises a balanced impedance matching capacitance for balancing the voltage across the sample coil.

34. The method of claim 33 wherein the balanced impedance matching capacitance comprises a first impedance matching capacitor connected between the sample coil and an ungrounded output terminal and a second impedance matching capacitor connected between the sample coil and a grounded output terminal, the sample being connected in series circuit between the first and second impedance matching capacitors across the ungrounded and grounded output terminals, the first impedance matching capacitor and the second impedance matching capacitor each having a capacitance which is approximately twice the capacitance of the tuning capacitor.

35. The method of claim 32 wherein the selected Larmor frequency is approximately 100 MHz and the sample coil has a nominal inductance of approximately 100 nanohenries.

36. A method for improving the signal-to-noise ratio of nuclear magnetic resonance signals detected in the presence of coil-to-ground parasitics encountered in nuclear magnetic resonance analysis of a specimen by a probe circuit having a sample coil and a tuning capacitor, the sample coil and the tuning capacitor substantially forming a resonant circuit across an ungrounded output terminal and a grounded output terminal, the resonant circuit being tuned to a selected Larmor frequency, and further having a first impedance matching capacitor between the sample coil and the ungrounded output terminal, comprising the steps of:

positioning the sample coil in close proximity to the specimen; and

inserting a second impedance matching capacitor between the sample coil and the grounded output terminal;

the sample coil being connected in series circuit between the first and second impedance matching capacitors across the ungrounded and grounded output terminals;

the first and second impedance matching capacitors controlling the voltage across the sample coil in the presence of leakage current from the sample coil through the specimen to ground in a manner to balance the leakage currents as seen from the ends of the sample coil, whereby the influence of coil-to-ground parasitics additional to any coil-to-ground parasitic attributable solely to leakage current directly from the sample coil to ground is reduced.

37. The method of claim 36 wherein the tuning capacitor is connected in parallel circuit with the sample coil.

38. The method of claim 37, further comprising the step of positioning the tuning capacitor in close proximity to the specimen.

39. The method of claim 36 wherein the first impedance matching capacitor is inserted between the ungrounded output terminal and a first junction, where the tuning capacitor is connected to the sample coil, and wherein the second impedance matching capacitor is inserted between the sample coil and a second junction, where the tuning capacitor is connected to the grounded output terminal.

40. The method of claim 36 wherein the tuning capacitor is adjustable for tuning the resonant circuit formed substantially by the sample coil and tuning capacitor to a selected Larmor frequency, further comprising the step of adjusting the tuning capacitor for tuning the resonant circuit formed substantially by the sample coil and tuning capacitor to the selected Larmor frequency.

41. The method of claim 39 wherein the tuning capacitor is adjustable for tuning the resonant circuit formed substantially by the sample coil and tuning capacitor to a selected Larmor frequency, further comprising the step of adjusting the tuning capacitor for tuning the resonant circuit formed substantially by the sample coil and tuning capacitor to the selected Larmor frequency.

42. The method of claim 36 wherein at least one of the first and second impedance matching capacitors is adjustable for matching the impedance across the ungrounded and grounded output terminals to a predetermined impedance, further comprising the step of adjusting the at least one of the first and second impedance matching capacitors for matching the impedance across the ungrounded and grounded output terminals to the predetermined impedance.

43. The method of claim 42 wherein the predetermined impedance is approximately 50 ohms.

44. The method of claim 36 wherein the first impedance matching capacitor and the second impedance matching capacitor each have a capacitance which is approximately twice the capacitance of the tuning capacitor.

45. The method of claim 36 wherein the selected Larmor frequency is approximately 100 MHz and the sample coil has a nominal inductance of approximately 100 nanohenries.