Method and apparatus for high-order differential mobility separations

• US 20070069120A1
• Filed: 09/28/2005
• Published: 03/29/2007
• Est. Priority Date: 09/28/2005
• Status: Active Grant

• Current Assignee: Battelle Memorial Institute
• Original Assignee: Battelle Memorial Institute
• Inventors: Smith, Richard, Shvartsburg, Alexandre, Anderson, Gordon
• Granted Patent: US 7,449,683 B2
• Time in Patent Office: Days
• US Class Current: 250/287
• CPC Class Codes: G01N 27/624 Differential mobility spectrometry [DMS]; Field asymmetric-waveform ion mobility spectrometry [FAIMS]

Abstract

The present invention relates generally to separation of ions based on their transport properties. More particularly, the invention relates to separation of ionic mixtures and characterization of ions in gases using higher-order differential ion mobility spectrometry (HODIMS) enabled by asymmetric waveforms of fundamentally new types. The invention discloses a method and apparatus for separation of ionic mixtures and characterization, identification, or quantification of ions in a gas based substantially on the terms of third or higher order in a series expansion of ion mobility as a function of electric field intensity. This is achieved using a periodic, time-dependent electric field with novel waveform profiles that cancel or substantially reduce the contributions to time-averaged ion motion of the leading n (where n≧2) terms of that expansion, thereby achieving ion separations based substantially on the (n+1)th term. Separations using HODIMS with different n are expected to be highly orthogonal, enabling multidimensional separations employing HODIMS analyzers of different orders. The expected high orthogonality between HODIMS and mass spectrometry or ion mobility spectrometry would make HODIMS/MS and HODIMS/IMS combinations powerful analytical tools of broad utility.

Claims

1. A method for separation, characterization, or identification of ions in a gas, the method comprising establishing a periodic, time-dependent electric field over an analytical gap, wherein the electric field substantially cancels the contributions to time-averaged ion motion of a number, n (where n≧

2), of leading terms in a series expansion for ion mobility, K, as a function of the electric field intensity, E, via a polynomial of powers of E/N, where N is the gas number density;

thereby achieving separation of ions based substantially on coefficients with the (n+1)^th and subsequent terms of said series expansion.

2. The method of claim 1, wherein said analytical gap is contained between at least two electrodes, and said electric field is produced by at least one voltage waveform applied to at least one of the electrodes.

3. The method of claim 2, wherein said electric field is a superposition of electric fields produced by voltage waveforms applied to at least two electrodes.

4. The method of claim 2, wherein said electrodes have a planar geometry.

5. The method of claim 4, where said electrodes are parallel, thereby establishing a spatially homogeneous electric field.

6. The method of claim 2, wherein at least one of said electrodes has a curved geometry, thereby establishing a spatially inhomogeneous electric field.

7. The method of claim 6, wherein said geometry is selected from the group of cylindrical, conical, spherical, hemispherical, ellipsoidal, ovoid, and combinations thereof.

8. The method of claim 6, wherein said electrodes have the geometry selected from the group of two coaxial cylinders, two concentric spheres or hemispheres, and combinations thereof.

9. The method of claim 6, further comprising selecting a field polarity such that said inhomogeneous electric field creates a pseudopotential well inside said analytical gap, thereby focusing or confining a plurality of ions within said gap.

10. The method of claim 9, wherein said confining is employed to guide said plurality of ions through said analytical gap to a desired volume in space, trapping said plurality of ions by containment in said well, temporarily storing said plurality of ions by containment in said well, or combinations thereof.

11. The method of claim 2, further comprising controlling the temperature of at least one of said electrodes.

12. The method of claim 11, wherein the temperatures of at least two of the electrodes differ, thereby providing a temperature gradient across the analytical gap that renders the value of E/N across said analytical gap spatially inhomogeneous, thereby creating a pseudopotential well inside said gap that focuses or confines a plurality of ions within said gap.

13. The method of claim 12, wherein said confining is employed to guide said plurality of ions through said analytical gap to a desired volume in space, trapping said plurality of ions by containment in said well, temporarily storing said plurality of ions by containment in said well, or combinations thereof.

14. The method of claim 1, wherein ions are moved through said analytical gap by a gas flow, a secondary electric field component perpendicular to said periodic time-dependent electric field, or combinations thereof.

15. The method of claim 14, wherein said secondary electric field is produced using at least one segmented electrode carrying a voltage gradient.

16. The method of claim 14, wherein said gas flow is heated or cooled before entering said analytical gap.

17. The method of claim 1, wherein said electric field is a superposition of elements selected from the group consisting of different discrete field settings applied over finite time intervals, different harmonic waveforms, and combinations thereof.

18. The method of claim 17, comprising (n+1) elements.

19. The method of claim 1, wherein said gas comprises a mixture of at least two homomolecular gases or vapors.

20. The method of claim 19, wherein said mixture has a composition resulting in a measurable deviation from Blanc'"'"'s law for ion mobilities.

21. The method of claim 1, wherein said gas comprises a gas-phase insulator with high electrical breakdown threshold.

22. The method of claim 1, wherein said ions are introduced into said analytical gap continuously.

23. The method of claim 1, wherein said ions are injected into said analytical gap in discrete pulses.

24. The method of claim 1, wherein said ions are received directly or through others stages from a source selected from the group consisting of electrospray ionization, desorption electrospray ionization, thermospray, sonic spray, matrix-assisted laser desorption ionization, atmospheric pressure matrix-assisted laser desorption ionization, surface-enhanced laser desorption ionization, laser vaporization, laser desorption, secondary ion ionization, photoionization, atmospheric pressure photo-ionization, arc discharge, coronary or cathode discharge, electron impact, chemical ionization, atmospheric pressure chemical ionization, liquid evaporation, liquid clustering, “

pick-up”

, and combinations thereof.

25. The method of claim 1, wherein the pressure of said gas in said analytical gap exceeds the pressure in an adjacent region from which said ions enter said analytical gap, such that said gas flows out of said analytical gap in the direction opposite to that of ion ingress.

26. The method of claim 1, wherein at least a portion of said ions is dissociated during, at the end of, or after said separation or characterization, by a technique selected from the group consisting of collisional dissociation, thermal dissociation, field dissociation, photodissociation, electron capture dissociation, and combinations thereof.

27. The method of claim 1 sequentially coupled to one or more iterations of said method having different values for said parameter n.

28. The method of claim 1, sequentially coupled on-line or off-line to at least one additional analytical method selected from the group consisting of ion mobility spectrometry, field asymmetric waveform ion mobility spectrometry, mass spectrometry, gas chromatography, photoelectron spectroscopy, photodissociation spectroscopy, liquid chromatography, strong cation exchange, supercritical fluid chromatography, capillary electrophoresis, capillary isoelectric focusing, gel separations in one or more dimensions, and combinations thereof.

29. An apparatus for separation, characterization, or identification of ions in a gas, comprising a plurality of electrodes operably connected to a waveform-generating device, said electrodes and said device configured to establish a periodic, time-dependent electric field over an analytical gap, wherein said electric field substantially cancels the contributions to ion motion of a number, n (where n≧

2), of leading terms in a series expansion for ion mobility, K, as a function of the electric field intensity, E, via a polynomial of powers of E/N, where N is the gas number density;

thereby achieving separation of ions based substantially on coefficients with the (n+1)^th and subsequent terms of said series expansion.

30. The apparatus of claim 29, wherein said analytical gap is contained between at least two electrodes, and said electric field is produced by at least one voltage waveform applied to at least one of the electrodes.

31. The apparatus of claim 29, wherein said electric field is a superposition of electric fields produced by voltage waveforms applied to at least two of the electrodes.

32. The apparatus of claim 29, wherein said electrodes have a planar geometry.

33. The apparatus of claim 32, where said electrodes are parallel, thereby establishing a spatially homogeneous electric field.

34. The apparatus of claim 29, wherein at least one of said electrodes has a curved geometry, thereby establishing a spatially inhomogeneous electric field.

35. The apparatus of claim 34, wherein said geometry is selected from the group of cylindrical, conical, spherical, hemispherical, ellipsoidal, ovoid, and combinations thereof.

36. The apparatus of claim 34, wherein said electrodes have the geometry selected from the group of two coaxial cylinders, two concentric spheres or hemispheres, and combinations thereof.

37. The apparatus of claim 29, further comprising at least one temperature-control device in thermal contact with at least one of said electrodes.

38. The apparatus of claim 29, wherein at least one of the electrodes is segmented with a voltage gradient thereon, thereby establishing a longitudinal electric field component perpendicular to said periodic, time-dependent electric field.

39. The apparatus of claim 29, further comprising a temperature-control device in thermal contact with said gas heating or cooling said gas prior to inflow into said analytical gap.

40. The apparatus of claim 29, operably connected, directly or through other stages, to an ion source selected from the group consisting of electrospray ionization, desorption electrospray ionization, thermospray, sonic spray, matrix-assisted laser desorption ionization, atmospheric pressure matrix-assisted laser desorption ionization, surface-enhanced laser desorption ionization, laser vaporization, laser desorption, secondary ion ionization, photoionization, atmospheric pressure photo-ionization, arc discharge, coronary or cathode discharge, electron impact, chemical ionization, atmospheric pressure chemical ionization, liquid evaporation, liquid clustering, “

pick-up”

, and combinations thereof.

41. The apparatus of claim 29, sequentially coupled on-line or off-line to at least one additional analytical device selected from the group consisting of ion mobility spectrometers, field asymmetric waveform ion mobility spectrometers, mass spectrometers, gas chromatographs, photoelectron spectrometers, photodissociation spectrometers, liquid chromatographs, strong cation exchange units, supercritical fluid chromatographs, capillary electrophoresis units, capillary isoelectric focusing units, gel separation units, and combinations thereof.

42. The apparatus of claim 29, further comprising means for dissociating at least a portion of said ions during, at the end of, or after said separation.

43. The apparatus of claim 29, further comprising means for pulsing or gating ions at the entrance to said analytical gap, thereby allowing discrete ion packets inside said gap.

44. The apparatus of claim 29, wherein said waveform-generating device comprises a plurality of operably-connected oscillating circuits, each outputting a periodic waveform, wherein said waveforms are superposed to provide said periodic, time-dependent electric field.

45. The apparatus of claim 29, wherein said waveform-generating device comprises at least one switched power source.

46. The apparatus of claim 45, wherein said at least one switched power source comprises at least one solid state switch in a series configuration operably connected to a power supply.

47. The apparatus of claim 46, wherein said at least one switched power source comprises a computer-controlled power supply.

48. The apparatus of claim 47, wherein said computer-controlled power supply is operably connected to a sequence generator.

49. The apparatus of claim 45, wherein said at least one switched power source provides at least one of the distinct voltages composing a period of the time-dependent electric field.

50. The apparatus of claim 29, further comprising a transformer operably connected to the waveform-generating device, wherein the waveform-generating device generates a sub-scaled form of a periodic time-dependent voltage waveform and the transformer amplifies said sub-scaled form to a desired amplitude.