IP Library Granted Patent US 10,056,244
Granted Patent B1
US 10,056,244 · App. 15/662,811 · Granted Aug 21, 2018

Tuning multipole RF amplitude for ions not present in calibrant

Inventors: Scott T. Quarmby (Round Rock, TX); Joshua T. Maze (Round Rock, TX); Nathaniel L. Sanders (Austin, TX)
Assignee: Thermo Finnigan LLC
H01J49/429H01J49/025H01J49/04H01J49/10H01J49/36H01J49/426H01J49/4225
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Quick Facts
Patent No.
US 10,056,244
App. No.
15/662,811
Granted
Aug 21, 2018
Kind
B1
Abstract

A mass spectrometry apparatus includes an ion source configured to generate ions; an ion guide configured to guide ions from the ion source towards a detector; the ion detector configured to detect ions; and a mass spectrometry controller. The mass spectrometry controller is configured to generate a tune curve for the ion guide; determine an observed low mass cutoff for the ion guide from the tune curve; calculate an effective r0 for the ion guide based on the observed low mass cutoff; determine an RF voltage based on the effective r0 and the RF frequency; apply the RF voltage to the ion guide; and perform a mass analysis of ions in a sample.

Claims (161)

1. A mass spectrometry apparatus comprising:

an ion source configured to generate ions;

an ion guide configured to guide ions from the ion source towards a detector;

the ion detector configured to detect ions; and

a mass spectrometry controller configured to:

generate a tune curve for the ion guide;

determine an observed low mass cutoff for the ion guide from the tune curve;

calculate an effective r0 for the ion guide based on the observed low mass cutoff;

determine an RF voltage based on the effective r0 and the RF frequency;

apply the RF voltage to the ion guide; and

perform a mass analysis of ions in a sample.

2. The mass spectrometry system of claim 1 wherein the ion guide is a quadrupole, a square quadrupole, a hexapole, an octopole, a stacked ring ion guide, an ion funnel, an ion carpet, or any combination thereof.

3. The mass spectrometry system of claim 1 wherein the processor is configured to calculate the effective r0 based on the observed low mass cutoff, a nominal r0, and an expected low mass cutoff.

4. The mass spectrometry system of claim 3 wherein the processor is configured to calculate the effective r0 according to

r

0

effective

=

K

observed

*

r

0

nominal

2

/

K

expected

where K expected is the expected value for a parameter and K observed is the observed value for the parameter, the parameter selected from q, q*(m/z), q*(m/z)*ω 2 , q*(m/z)*f 2 , V, V/ω 2 , V/f 2 , or a combination thereof.

5. The mass spectrometry system of claim 3 wherein the processor is configured to calculate the effective r0 according to

r

0

effective

=

cutoff

observed

*

r

0

nominal

2

/

cutoff

expected

.

6. The mass spectrometry system of claim 1 wherein the observed low mass cutoff is an average across at least two calibrant ion species.

7. The mass spectrometry system of claim 1 wherein the RF voltage is determined based on the effective r0, the frequency of the RF voltage, and a tune table.

8. The mass spectrometry system of claim 7 wherein the tune table includes optimum q values for mass-to-charge ratios.

9. A method of analyzing ion fragments, comprising:

generating a tune curve for an ion guide;

determining an observed low mass cutoff for the ion guide from the tune curve;

calculating an effective r0 for the ion guide based on the observed low mass cutoff;

determining an RF voltage based on the effective r0 and the RF frequency;

applying the RF voltage to the ion guide; and

performing a mass analysis of ions in a sample.

10. The method of claim 9 wherein the ion guide is a quadrupole, a square quadrupole, a hexapole, an octopole, a stacked ring ion guide, an ion funnel, an ion carpet, or any combination thereof.

11. The method of claim 9 wherein calculating an effective r0 is based on the observed low mass cutoff, a nominal r0, and an expected low mass cutoff.

12. The method of claim 11 wherein calculating the effective r0 is in accordance with

r

0

effective

=

K

observed

*

r

0

nominal

2

/

K

expected

the expected value for a parameter and K observed is the observed value for the parameter, the parameter selected from q, q*(m/z), q*(m/z)*ω 2 , q*(m/z)*f 2 , V, V/ω 2 , V/f 2 , or a combination thereof.

13. The method of claim 11 wherein calculating the effective r0 is in accordance with

r

0

effective

=

cutoff

observed

*

r

0

nominal

2

/

cutoff

expected

.

14. The method of claim 9 wherein the observed low mass cutoff is an average across at least two calibrant ion species.

15. The method of claim 9 wherein the RF voltage is determined based on the effective r0, the RF frequency, and a tune table.

16. The method of claim 15 wherein the tune table includes optimum q values for mass-to-charge ratios.

17. A non-transitory computer readable medium containing instructions that when implemented by a processor perform the steps of:

generating a tune curve for an ion guide;

determining a low mass cutoff for the ion guide from the tune curve;

calculating an effective r0 for the ion guide based on the observed low mass cutoff;

determining an RF voltage based on the effective r0 and the RF frequency;

applying the RF voltage to the ion guide; and

performing a mass analysis of ions in a sample.

18. The non-transitory computer readable medium of claim 17 wherein the ion guide is a quadrupole, a square quadrupole, a hexapole, an octopole, a stacked ring ion guide, an ion funnel, an ion carpet, or any combination thereof.

19. The non-transitory computer readable medium of claim 17 wherein the instructions to calculate the effective r0 are based on the observed low mass cutoff, a nominal r0, and an expected low mass cutoff.

20. The non-transitory computer readable medium of claim 19 wherein the instructions to calculate the effective r0 are in accordance with

r

0

effective

=

K

observed

*

r

0

nominal

2

/

K

expected

where K expected is the expected value for a parameter and K observed is the observed value for the parameter, the parameter selected from q, q*(m/z), q*(m/z)*ω 2 , q*(m/z)*f 2 , V, V/ω 2 , V/f 2 , or a combination thereof.

21. The non-transitory computer readable medium of claim 19 wherein the instructions to calculate the effective r0 are in accordance with

r

0

effective

=

cutoff

observed

*

r

0

nominal

2

/

cutoff

expected

.

22. The non-transitory computer readable medium of claim 17 wherein the observed low mass cutoff is an average across at least two calibrant ion species.

23. The non-transitory computer readable medium of claim 17 wherein the RF voltage is determined based on the effective r0, the RF frequency, and a tune table.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Aug 14, 2017
From: QUARMBY, SCOTT T.; MAZE, JOSHUA T.; SANDERS, NATHANIEL L.
To: THERMO FINNIGAN LLC
Reel/Frame 043283/0916 →
Cited By (8)
US 12,237,161 US 12,255,060 US 12,283,475 US 12,293,908 US 12,390,765 US 12,394,615 US 12,712,171 US 12,731,775