Method and apparatus for injection of ions into an electrostatic ion trap

Patent metadata

Field	Value
Publication number	US-9831079-B2
Application number	US-201615145638-A
Country	US
Kind code	B2
Filing date	May 3, 2016
Priority date	May 5, 2015
Publication date	Nov 28, 2017
Grant date	Nov 28, 2017

Abstract

A method of injecting ions into an electrostatic trap, comprising: generating ions in an ion source; transporting the ions from the ion source to an ion store downstream of the ion source; releasing the ions from the ion store to an ion guide downstream of the ion store; and accelerating the ions from the ion guide as a pulse into an orbital electrostatic trap for mass analysis, wherein the average velocity of the ions as the ions exit from the ion guide is substantially higher than the average velocity of the ions as they exit from the ion store, wherein there is a delay between releasing the ions from the ion store and accelerating the ions from the ion guide. Also an apparatus suitable for the method.

First claim

The invention claimed is:

1. A method of injecting ions into an electrostatic trap, comprising:
generating ions in an ion source;
transporting the ions from the ion source to an ion store downstream of the ion source;
releasing the ions from the ion store to a non-trapping ion guide downstream of the ion store; and
accelerating the ions from the ion guide as a pulse into an orbital electrostatic trap for mass analysis, wherein the average velocity of the ions as the ions exit from the ion guide is substantially higher than the average velocity of the ions as they exit from the ion store, wherein there is a delay between releasing the ions from the ion store and accelerating the ions from the ion guide such that for ions of the same m/z forming an ion packet, the duration of the ion packet as it enters the electrostatic trap is substantially shorter than when the ion packet enters the ion guide from the ion store.

2. The method as claimed in claim 1 wherein the electrostatic trap separates the ions along a direction z according to their mass-to-charge ratio; and the initial velocity of the ions in the ion guide in the direction z prior to acceleration is substantially smaller than the velocity of the ions in the direction z during ion detection in the electrostatic trap.

3. The method as claimed in claim 2 wherein the ions are accelerated from the ion guide to the electrostatic trap either:
a. substantially in the same direction as the ions were released from the ion store, which is a direction substantially orthogonal to direction z; or
b. along a direction that is substantially orthogonally to the direction in which the ions were released from the ion store and is substantially parallel to direction z.

4. The method as claimed in claim 1 wherein the ions are transported from the ion source to the ion store via at least one ion optical device.

5. The method as claimed in claim 1 further comprising separating the ions according to mass-to-charge ratio or ion mobility upstream of the ion store.

6. The method as claimed in claim 1 wherein the ion store is a linear or 3D RF ion trap.

7. The method as claimed in claim 1 wherein the ion store is gas-filled, optionally to a pressure 1 ×10 −3 mbar to 5 ×10 −3 mbar.

8. The method as claimed in claim 1 wherein the ions are slowly released from the ion store to the ion guide with energies less than 1V.

9. The method as claimed in claim 1 wherein the ions are released from the ion store over a period of 10 to 100 microseconds.

10. The method as claimed in claim 1 wherein the ions are released from the ion store by applying a DC voltage pulse to generate an axial field gradient in the ion store.

11. The method as claimed in claim 1 wherein the ion guide is gas-free, optionally wherein the pressure is less than or equal to 10 −3 mbar.

12. The method as claimed in claim 1 wherein the ions are accelerated from the ion guide by applying a DC voltage pulse to generate an axial field gradient in the ion guide, whereby an energy increase of the ions depends on their initial position within the guide.

13. The method as claimed in claim 12 wherein the energy range of the accelerated ions is 1% to 30% of the final energy of the ions in the electrostatic trap.

14. The method as claimed in claim 1 wherein at the same time as applying the axial field gradient, any RF field in the ion guide is switched off.

15. The method as claimed in claim 1 wherein the energy spread of the ions accelerated by the ion guide is significantly smaller than the final energy of the ions within the electrostatic trap, optionally wherein the energy spread of the ions is not more than 30% or not more than 20% or not than 10%, of the final energy of the ions within the electrostatic trap.

16. The method as claimed in claim 1 wherein the ion guide focuses the ions at a focal point within the electrostatic trap and wherein the ions are focused into ion packets that are sufficiently narrow in the z-direction of the electrostatic trap when they pass near one or more detection electrodes of the electrostatic trap so as to maintain coherence of the ion packets during detection.

17. The method as claimed in claim 16 further comprising adjusting the position of the focal point using an ion lens located downstream of the ion guide.

18. The method as claimed in claim 1 wherein the ion guide is a linear RF multipole ion guide, optionally wherein the ion guide axis is substantially orthogonally to the direction z of mass separation in the electrostatic trap.

19. The method as claimed in claim 1 wherein the ion guide is a helical trajectory ion guide wherein the ions move with both axial and rotational motion, optionally wherein the ion guide axis is substantially parallel to the direction z of mass separation in the electrostatic trap.

20. The method as claimed in claim 19 , further comprising providing a potential step within the ion guide that reduces the velocity of the ions in the direction z.

21. The method as claimed in claim 19 wherein the ions are accelerated out of the ion guide at a fixed radius to the ion guide axis, which lies parallel to the direction z.

22. The method as claimed in claim 19 wherein after accelerating the ions out of the ion guide by means of applying a DC axial field gradient in the ion guide, a further DC axial field gradient is applied in the ion guide that stays on whilst ions are being detected in the electrostatic trap, wherein the further DC axial field gradient is chosen such that perturbations of an ideal electric field within the electrostatic trap are minimized.

23. The method as claimed in claim 22 wherein the further DC axial field gradient is chosen such that ion oscillations in the EST in the direction z remain as close to harmonic as possible.

Assignees

• Thermo Fisher Scient (Bremen) Gmbh

Inventors

• Makarov Alexander A

Classifications

• H01J49/4245 Primary

  Electrostatic ion traps (H01J49/422 takes precedence) · CPC title

• H01J49/4295

  Storage methods · CPC title

• H01J49/062

  Ion guides (linear ion traps performing mass selection H01J49/4225, mass filters H01J49/421) · CPC title

• H01J49/426

  Methods for controlling ions · CPC title

• H01J49/425 Primary

  with a logarithmic radial electric potential, e.g. orbitraps · CPC title