Apparatus and methods for continuous beam fourier transform mass spectrometry

• US 6,452,168 B1
• Filed: 09/15/1999
• Issued: 09/17/2002
• Est. Priority Date: 09/15/1999
• Status: Expired due to Fees

• Current Assignee: Lockheed Martin Energy Research Corporation (Martin Marietta Corporation)
• Original Assignee: UT-Battelle LLC
• Inventors: McLuckey, Scott A., Goeringer, Douglas E.
• Primary Examiner(s): Anderson, Bruce
• Assistant Examiner(s): Hashmi, Zia R.
• Application Number:
  US09/396,839
• Time in Patent Office: 1,098 Days
• Field of Search: 250/292, 250/282, 250/290-294
• US Class Current: 250/292
• CPC Class Codes: H01J 49/38 Omegatrons ; using ion cyclotron resonance

Abstract

A continuous beam Fourier transform mass spectrometer in which a sample of ions to be analyzed is trapped in a trapping field, and the ions in the range of the mass-to-charge ratios to be analyzed are excited at their characteristic frequencies of motion by a continuous excitation signal. The excited ions in resonant motions generate real or image currents continuously which can be detected and processed to provide a mass spectrum.

Claims

1. A continuous beam Fourier transform mass spectrometer comprising:

a. a confinement structure having a cavity, a first opening and a second opening;

b. means for applying an RF voltage to the structure to form a trapping field in the cavity;

c. means for supplying a continuous beam of ions through the first opening to the cavity to form a sample of ions with a range of masses, wherein the sample ions are trapped in the trapping field and each ion is characterized by a mass-to-charge dependent frequency of motion;

d. means for continuously applying an excitation signal having a frequency spectrum and an amplitude to the trapped sample ions, wherein the frequency spectrum of the excitation signal includes characteristic frequencies corresponding to at least one of the mass-to-charge dependent frequencies of motion of the sample ions, and the amplitude of the excitation signal is sufficiently high to cause resonant motions of the ions with at least one of the characteristic frequencies of the excitation signal; and

e. means for detecting signals responsive to the resonant motions of the ions, wherein the second opening allows at least some of the sample ions to exit the cavity.

2. The mass spectrometer of claim 1, further comprising means for converting the signals responsive to the resonant motions of the ions into a frequency spectrum.

3. The mass spectrometer of claim 2, further comprising means for converting the frequency spectrum into a mass spectrum.

4. The mass spectrometer of claim 1, wherein the confinement structure comprises a structure defining a three-dimensional trapping field.

5. The mass spectrometer of claim 4, wherein the three-dimensional trapping field comprises an electric field.

6. The mass spectrometer of claim 1, wherein the confinement structure comprises a structure defining a two-dimensional trapping field.

7. The mass spectrometer of claim 6, wherein the two-dimensional trapping field comprises an electric field.

8. The mass spectrometer of claim 6, wherein the two-dimensional trapping field comprises a uniform magnetic field.

9. A continuous beam Fourier transform mass spectrometer comprising:

a. a quadrupole structure having end caps and a ring electrode, the end caps and the ring electrode spaced apart from each other thereby defining a cavity, the cavity communicating with outside through a first opening and a second opening;

b. RF voltage means for applying an RF voltage to the ring electrode to form a three-dimensional trapping field in the cavity;

c. ion beam means for supplying a continuous beam of ions through the first opening to the cavity to form a sample of ions with a range of masses, wherein the sample ions are trapped in the trapping field and each ion is characterized by a mass-to-charge dependent frequency of motion;

d. excitation means for continuously applying an excitation signal having a frequency spectrum, the frequency spectrum including characteristic frequencies corresponding to at least one of the mass to charge dependent frequencies of motion, to at least one of the end caps to cause resonant motions of the trapped sample ions with at least one of the characteristic frequencies of the excitation signal, wherein the ions in resonant motions are ejected away from the cavity through the second opening continuously thereby to form a current; and

e. means for detecting the current.

10. The mass spectrometer of claim 9, further comprising means for converting the current into a frequency spectrum.

11. The mass spectrometer of claim 10, further comprising means for converting the frequency spectrum into a mass spectrum.

12. The mass spectrometer of claim 9, wherein the excitation means includes means for applying the excitation signal across the end caps in dipolar fashion.

13. The mass spectrometer of claim 12, wherein the excitation means comprises a transformer.

14. The mass spectrometer of claim 9, wherein the excitation means includes means for applying the excitation signal to one of the end caps in monopolar fashion.

15. The mass spectrometer of claim 9, wherein the detecting means is electrically detached from the end caps and the current includes a DC component and an AC component.

16. The mass spectrometer of claim 15, wherein the detecting means comprises means for selectively detecting the AC component of the current.

17. The mass spectrometer of claim 9, wherein the detecting means is electrically connected to at least one of the end caps and comprises means for detecting the image current induced by the ions in resonant motions.

18. A continuous beam Fourier transform mass spectrometer comprising:

a. a quadrupole structure having a plurality of linear quadrupole rods, the linear quadrupole rods spaced parallel and apart from each other thereby defining a bore extending axially between the ends of the structure, the bore having a longitudinal axis;

b. RF voltage means for applying RF voltage signals selectively to the rods so that voltage signals applied to adjacent rods are 180°

out-of-phase and voltage signals applied to opposing rods are in-phase thereby to form a two-dimensional trapping field radially in the bore;

c. ion beam means for supplying a continuous beam of ions through one end of the structure to the bore along the longitudinal axis to form a sample of ions with a range of masses, wherein the sample ions are trapped in the trapping field and each ion is characterized by a mass-to-charge dependent frequency of motion;

d. excitation means for continuously applying an excitation signal having a frequency spectrum, the frequency spectrum including characteristic frequencies corresponding to at least one of the mass to charge dependent frequencies of motion, to a pair of opposing rods to cause resonant motions of the trapped sample ions with at least one of the characteristic frequencies of the excitation signal, wherein the ions in resonant motions move in expanded radii of motion; and

e. means for detecting the ions in resonant motions.

19. The mass spectrometer of claim 18, wherein the excitation means includes means for applying the excitation signal across the opposing rods in dipolar fashion.

20. The mass spectrometer of claim 19, wherein the excitation means comprises a transformer.

21. The mass spectrometer of claim 18, wherein the detecting means comprises a ring-shaped plate closing one end of the bore, the plate having a first radius and a second radius defining an opening, wherein the first radius is selected to fit the bore and the second radius is selected to allow ions not in resonant motions to pass through the opening undetected and to allow the ions in resonant motions to be received by the plate thereby to yield a current.

22. The mass spectrometer of claim 21, further comprising means for converting the signals corresponding to the current into a frequency spectrum.

23. The mass spectrometer of claim 22, further comprising means for converting the frequency spectrum into a mass spectrum.

24. A continuous beam Fourier transform mass spectrometer comprising:

a. a cell structure having a first pair and second pair of opposing plates and a bore extending between the ends of the structure, the bore having a longitudinal axis;

b. means for applying a uniform magnetic field in the bore, the magnetic field having a direction parallel to the longitudinal axis thereby to form a two-dimensional trapping field radially in the bore;

c. ion beam means for supplying a continuous beam of ions through one end of the structure to the bore along the longitudinal axis to form a sample of ions with a range of masses, wherein the sample ions are trapped radially in the bore and each ion is characterized by a mass-to-charge dependent frequency of motion;

d. excitation means for continuously applying an excitation signal having a frequency spectrum and an amplitude to the first pair of opposing plates to cause resonant motions of the trapped sample ions with at least one of the characteristic frequencies of the excitation signal, wherein the ions in resonant motions move in expanded radii of motion thereby to approach the second pair of the opposing plates and induce an image current therein; and

e. means for detecting the image current.

25. The mass spectrometer of claim 24, further comprising means for converting the image current into a frequency spectrum.

26. The mass spectrometer of claim 25, further comprising means for converting the frequency spectrum into a mass spectrum.

27. The mass spectrometer of claim 24, wherein the excitation means comprises a transformer.

28. The mass spectrometer of claim 24, wherein the detecting means comprises an amplifier.

29. A method of mass analyzing ions trapped in a confinement structure, wherein the confinement structure has a cavity, comprising:

a. forming a trapping field in the cavity;

b. supplying a continuous beam of ions to form a sample of ions with a range of masses in the cavity, wherein the sample ions are trapped in the trapping field and each ion is characterized by a mass-to-charge dependent frequency of motion;

c. continuously applying an excitation signal having a frequency spectrum and an amplitude to the trapped sample ions, wherein the frequency spectrum of the excitation signal includes characteristic frequencies corresponding to at least one of the mass-to-charge dependent frequencies of motion of the sample ions, and the amplitude of the excitation signal is sufficiently high to cause resonant motions of the ions with at least one of the characteristic frequencies of the excitation signal; and

d. detecting signals responsive to the resonant motions of the ions.

30. The method of claim 29, further comprising the step of converting the signals responsive to the resonant motions of the ions into a frequency spectrum.

31. The method of claim 30, further comprising the step of converting the frequency spectrum into a mass spectrum.

32. The method of claim 29, wherein the trapping field is a three-dimensional electric field.

33. The method of claim 29, wherein the trapping field is a two-dimensional electric field.

34. The method of claim 29, wherein the trapping field is a uniform magnetic field.

35. A method of mass analyzing ions trapped in a quadrupole structure, wherein the structure has a cavity, a first opening and a second opening, comprising:

a. applying an RF voltage to the quadrupole structure to form a trapping field in the cavity;

b. supplying a continuous beam of ions through the first opening to the cavity to form a sample of ions with a range of masses, wherein the sample ions are trapped in the trapping field and each ion is characterized by a mass-to-charge dependent frequency of motion;

c. continuously applying an excitation signal having a frequency spectrum and an amplitude to the trapped sample ions, wherein the frequency spectrum of the excitation signal includes characteristic frequencies corresponding to at least one of the mass-to-charge dependent frequencies of motion of the sample ions, and the amplitude of the excitation signal is sufficiently high to cause resonant motions of the ions with at least one of the characteristic frequencies of the excitation signal; and

d. detecting signals responsive to the resonant motions of the ions.

36. The method of claim 35, further comprising the step of converting the signals responsive to the resonant motions of the ions into a frequency spectrum.

37. The method of claim 36, further comprising the step of converting the frequency spectrum into a mass spectrum.

38. The method of claim 35, wherein the trapping field is a three-dimensional electric field.

39. The method of claim 38, wherein the signals responsive to the resonant motions of the ions comprise a current, the current being formed by a flux of the ions in resonant motions which are ejected away from the cavity through the second opening.

40. The method of claim 35, wherein the trapping field is a two-dimensional electric field.

41. The method of claim 40, wherein the signals response to the resonant motions of the ions comprise a current, the current being formed in response to the ions in resonant motions which move in expanded radii of motion.

42. A method of mass analyzing ions trapped in a cell structure, wherein the cell structure has a bore, the bore having a longitudinal axis and extending axially between a first and a second openings, comprising:

a. applying a magnetic field to the cell structure to form a trapping field in the bore, the magnetic field having a direction along the longitudinal axis;

b. supplying a continuous beam of ions through the first opening to the bore to form a sample of ions with a range of masses, wherein the sample ions are constrained radially in the trapping field and each ion is characterized by a mass-to-charge dependent frequency of motion;

c. continuously applying an excitation signal having a frequency spectrum and an amplitude to the trapped sample ions, wherein the frequency spectrum of the excitation signal includes characteristic frequencies corresponding to at least one of the mass-to-charge dependent frequencies of motion of the sample ions, and the amplitude of the excitation signal is sufficiently high to cause resonant motions of the ions with at least one of the characteristic frequencies of the excitation signal; and

d. detecting the signals responsive to the resonant motions of the ions.

43. The method of claim 42, further comprising the step of converting the signals responsive to the resonant motions of the ions into a frequency spectrum.

44. The method of claim 43, further comprising the step of converting the frequency spectrum into a mass spectrum.

45. The method of claim 42, wherein the magnetic field is uniform.

46. A method of analyzing ions trapped in a confinement structure by a trapping field, comprising:

a. applying an excitation signal continuously to the confinement structure to cause resonant motions of the ions; and

b. detecting signals responsive to the resonant motions of the ions.

47. The method of claim 46, further comprising the step of converting the signals responsive to the resonant motions of the ions into a frequency spectrum.

48. The method of claim 47, further comprising the step of converting the frequency spectrum into a mass spectrum.