IP Library Granted Patent US 7,847,246
Granted Patent B2
US 7,847,246 · App. 11/946,164 · Granted Dec 7, 2010

Collision-induced decomposition of ions in RF ion traps

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Quick Facts
Patent No.
US 7,847,246
App. No.
11/946,164
Granted
Dec 7, 2010
Kind
B2
Abstract

In an RF ion trap, analyte ions are fragmented by applying a moderately high RF storage voltage to the trap. The ions are then excited via dipolar excitation, and after a short time, the ions are forced into a resting state, again using dipolar excitation. The RF storage voltage is then rapidly reduced to a low value thereby making it possible to store small fragment ions produced by ergodic decompositions that occur subsequent to the reduction of the RF storage voltage.

Claims (13)

1. A method for collision-induced decomposition of analyte ions in an RF ion trap having an RF storage voltage applied thereto and being filled with a collision gas, comprising:

(a) setting the RF storage voltage to a value such that a lower mass threshold of the ion trap is greater than one eighth and less than one half of the mass-to-charge ratio of the analyte ions;

(b) exciting oscillations of the analyte ions by means of an electric field, in order to produce hard collisions with the collision gas; and

(c) decelerating the oscillations to a halt by means of an electric field in order to assemble collisionally excited analyte ions in a center location of the ion trap.

2. The method of claim 1 , wherein after step (c), the RF storage voltage is reduced so that light fragment ions produced by ergodic decompositions of the collisionally excited analyte ions occurring after step (c) can also be stored in the ion trap.

3. The method of claim 1 , wherein the oscillations are excited in step (b) and decelerated to a halt in step (c) by resonant or non-resonant alternating excitation fields.

4. The method of claim 3 , wherein the alternating excitation fields are switched off for a predetermined exposure time between step (b) and step (c).

5. The method of claim 1 , wherein the oscillations are excited in step (b) by the field of a first DC voltage pulse and decelerated to a halt at step (c) by the field of a second DC voltage pulse, and wherein there is a predetermined exposure time between the first and the second DC voltage pulses.

6. The method of claim 1 , wherein step (b) comprises switching on an electric DC field with sufficient strength to force the analyte ions into an ion trap region with a strong RF storage field and to keep the analyte ions in that region, and wherein step (c) comprises switching off the electric DC field.

7. The method of claim 1 , further comprising, before step (a), partially deprotonating the analyte ions when the analyte ions are highly charged.

8. The method of claim 7 , wherein the partial deprotonation is halted when the analyte ions reach a predetermined charge level.

9. The method of claim 1 , wherein step (b) comprises increasing a pressure of the collision gas to enhance collision-induced decomposition.

10. The method of claim 1 , wherein the method further comprises after step (c), at least partially removing remaining undecomposed analyte ions from the ion trap by resonant excitation.

Assignments (2)
NUNC PRO TUNC ASSIGNMENT Recorded Jun 18, 2021
From: BRUKER DALTONIK GMBH
To: BRUKER DALTONICS GMBH & CO. KG
Reel/Frame 057209/0070 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jul 10, 2008
From: BREKENFELD, ANDREAS
To: BRUKER DALTONIK, GMBH
Reel/Frame 021220/0006 →