Orthogonal acceleration system for time-of-flight mass spectrometer

Patent metadata

Field	Value
Publication number	US-8975580-B2
Application number	US-201313828512-A
Country	US
Kind code	B2
Filing date	Mar 14, 2013
Priority date	Mar 14, 2013
Publication date	Mar 10, 2015
Grant date	Mar 10, 2015

Abstract

An orthogonal pulse accelerator for a Time-of-Flight mass analyzer includes an electrically-conductive first plate extending in a first plane, and a second plate spaced from the first plate. The second plate includes a grid that defines a plurality of apertures each having a first dimension extending in a first direction and a second dimension orthogonal to the first dimension, the first and second dimensions lying in the second plane and the second dimension begin larger than the first dimension. The first and second plates are positioned in the Time-of-Flight mass analyzer to receive, during operation of the mass analyzer, an ion beam propagating in the first direction in a region between the first and second plates, and the orthogonal pulse accelerator directs ions in the ion beam through the apertures.

First claim

What is claimed is:

1. An orthogonal pulse accelerator for a Time-of-Flight mass analyzer, comprising:
an electrically-conductive first plate extending in a first plane; and
a second plate spaced from the first plate, the second plate extending in a second plane parallel to the first plane, the second plate comprising a grid that defines a plurality of apertures each having a first dimension extending in a first direction and a second dimension orthogonal to the first dimension, the first and second dimensions lying in the second plane and the second dimension being larger than the first dimension;
wherein the first and second plates are positioned in the Time-of-Flight mass analyzer to receive, during operation of the mass analyzer, an ion beam propagating in the first direction in a region between the first and second plates while a first electric field between the first and second plates is essentially zero, and the orthogonal pulse accelerator directs at least a portion of ions in the ion beam through the apertures when a second electric field is applied between the first and second plates, such that an electric field strength in the region between the first and second plates is essentially identical to an electric field strength in a region on an opposite side of the second plate, away from the first plate.

2. The orthogonal pulse accelerator of claim 1 , wherein at least some of the apertures are rectangular apertures.

3. The orthogonal pulse accelerator of claim 2 , wherein for the rectangular apertures, the first dimension corresponds to a width of each rectangle and the second dimension corresponds to a length of the rectangle.

4. The orthogonal pulse accelerator of claim 1 , wherein each of the apertures has the same shape.

5. The orthogonal pulse accelerator of claim 1 , wherein the first dimension is between 0.05 mm-0.5 mm.

6. The orthogonal pulse accelerator of claim 1 , wherein the first dimension is 0.13 MM.

7. The orthogonal pulse accelerator of claim 6 , wherein the second dimension is between 0.3 mm to 2.0 mm.

8. The orthogonal pulse accelerator of claim 1 , wherein the second dimension is 0.85 mm.

9. The orthogonal pulse accelerator of claim 1 , wherein a grid density along the first direction is greater than in a direction orthogonal to the first direction.

10. The orthogonal pulse accelerator of claim 1 , wherein the grid comprises electrically-conductive wires.

11. The orthogonal pulse accelerator of claim 10 , wherein the wires have square, or rectangular, or circular, or arbitrary-shaped cross-sections and characteristic dimensions in any direction of between 5-100 micron.

12. The orthogonal pulse accelerator of claim 11 , wherein the wires are of square cross-section, having a side dimension of 30 microns.

13. The orthogonal pulse accelerator of claim 1 , wherein the grid has a circular shape in the second plane.

14. The orthogonal pulse accelerator of claim 1 , wherein second plate is electrically-conductive.

15. The orthogonal pulse accelerator of claim 1 , wherein the grid has a thickness sufficient to obstruct at least some of the ions incident on the grid at a grazing incidence angle with respect to the second plane.

16. The orthogonal pulse accelerator of claim 1 , further comprising a third electrically conductive-plate extending in a third plane downstream of the second plate and parallel to the second plane, the third plate comprising a second grid , the second grid defining a second plurality of apertures each having a third dimension extending in the first direction and a fourth dimension orthogonal to the third dimension, the third and fourth dimensions lying in the third plane, the third dimension being larger than the fourth dimension.

17. The Time-of-Flight mass analyzer comprising the orthogonal pulse accelerator of claim 1 further comprising a detector.

18. The Time-of-Flight mass analyzer comprising the orthogonal pulse accelerator of claim 1 further comprising a reflectron.

19. The Time-of-Flight mass analyzer comprising the orthogonal pulse accelerator of claim 1 further comprising a flight tube.

Assignees

• Perkinelmer Health Sci Inc

Inventors

• Welkie David G

Classifications

• H05H5/047

  Pulsed generators · CPC title

• H05H5/02

  Details (targets for producing nuclear reactions H05H6/00) · CPC title

• H01J49/0031

  Step by step routines describing the use of the apparatus (H01J49/0081 takes precedence) · CPC title

• H01J49/403

  characterised by the acceleration optics and/or the extraction fields · CPC title

• H01J49/40

  Time-of-flight spectrometers (H01J49/36 takes precedence) · CPC title