Fragmenting ions in mass spectrometry

• US 7,541,575 B2
• Filed: 01/11/2007
• Issued: 06/02/2009
• Est. Priority Date: 01/11/2006
• Status: Active Grant

• Current Assignee: DH Technologies Development Pte. Ltd. (Danaher Corporation)
• Original Assignee: MDS Incorporated (Molecular Devices), Applera Corporation (Thermo Fisher Scientific Incorporated)
• Inventors: Bloomfield, Nic, Lock, Christopher Mark
• Primary Examiner(s): Berman; Jack I
• Application Number:
  US11/622,064
• Publication Number:
  US 20070158546A1
• Time in Patent Office: 873 Days
• Field of Search: None
• US Class Current: 250/281
• CPC Class Codes: H01J 49/005 by collision with gas, e.g. by introducing gas or by accelerating ions with an electric field

Abstract

Systems, methods, and computer program products useful in controlling the fragmentation of ions. Control of fragmentation is achieved by varying the collision energy imparted to precursor ions.

Claims

1. A method of controlling the fragmentation of ions during mass spectral analysis, comprising:

(i) at a starting collision energy provided within a mass spectrometer, fragmenting at least one of a plurality of precursor ions generated from a sample to produce a plurality of daughter ion fragments;

(ii) determining an ion current associated with unfragmented precursor ions in the mass spectrometer;

(iii) determining an ion current associated with the daughter ion fragments in the mass spectrometer;

(iv) determining the ratio of the current associated with the unfragmented precursor ions to the current associated with the daughter ion fragments; and

(v) adjusting the collision energy provided in the mass spectrometer at (i) to move the ratio toward a predetermined range or value.

2. The method of claim 1, further comprising repeating (i)-(v), as necessary, to bring the ratio into the predetermined range.

3. The method according to claim 1, wherein the collision energy is adjusted by an amount determined using the relation:

Δ

CE=m*ln (ion current ratio)+B,

where Δ

CE is the change by which the collision energy is adjusted; and

m and B are constants derived through at least one of theoretical analysis and experimentation.

4. The method according to claim 3, wherein the collision energy is adjusted by an amount determined using the relation:

Δ

CE=4.5*ln (ion current ratio)+13.5 (eV).

5. A system useful for controlling the fragmentation of ions during mass spectral analysis, the system comprising a controller adapted to:

(i) at a starting collision energy provided within a mass spectrometer, fragment at least one of a plurality of precursor ions generated from a sample to produce a plurality of daughter ion fragments;

(ii) determine an ion current associated with unfragmented precursor ions in the mass spectrometer;

(iii) determine an ion current associated with the daughter ion fragments in the mass spectrometer;

(iv) determine the ratio of the current associated with the unfragmented precursor ions to the current associated with the daughter ion fragments; and

(v) adjust the collision energy provided in the mass spectrometer at (i) to move the ratio toward a predetermined range or value.

6. The system of claim 5, wherein the controller is adapted to repeat (i)-(v), as necessary, to bring the ratio into the predetermined range.

7. The system of claim 5, wherein the collision energy is adjusted by an amount determined using the relation:

Δ

CE=m*ln (ion current ratio)+B,

where Δ

CE is the change by which the collision energy is adjusted; and

m and B are constants derived through at least one of theoretical analysis and experimentation.

8. The system of claim 7, wherein the collision energy is adjusted by an amount determined using the relation:

Δ

CE=4.5*ln (ion current ratio)+13.5 (eV).

9. A computer usable medium having computer readable code embodied therein for causing a mass spectrometer to:

(i) at a starting collision energy provided within a mass spectrometer, fragment at least one of a plurality of precursor ions generated from a sample to produce a plurality of daughter ion fragments;

(ii) determine an ion current associated with unfragmented precursor ions in the mass spectrometer;

(iii) determine an ion current associated with the daughter ion fragments in the mass spectrometer;

(iv) determine the ratio of the current associated with the unfragmented precursor ions to the current associated with the daughter ion fragments; and

(v) adjust the collision energy provided in the mass spectrometer at (i) to move the ratio toward a predetermined range or value.

10. The medium of claim 9, comprising code adapted for causing the mass spectrometer to repeat (i)-(v), as necessary, to bring the ratio into the predetermined range.

11. The medium of claim 9, wherein the collision energy is adjusted by an amount determined using the relation:

Δ

CE=m*ln (ion current ratio)+B,

where Δ

CE is the change by which the collision energy is adjusted; and

m and B are constants derived through at least one of theoretical analysis and experimentation.

12. The medium of claim 11, wherein the collision energy is adjusted by an amount determined using the relation:

Δ

CE=4.5*ln (ion current ratio)+13.5 (eV).