# US 5,347,127 A · Method and device for in-phase excitation of ion ejection from ion trap mass spectrometers

> Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt

- Number: US 5,347,127 A
- Document ID: US5347127A
- Status: Granted
- Kind: A
- Application number: 07/996,058
- Filed: 1992-12-23
- Granted: 1994-09-13
- Earliest claimed: 1991-12-23
- Assignees: Bruker-Franzen Analytik GmbH
- Inventors: Jochen Franzen
- Web page: https://patentgrep.com/patent/US5347127A

## CPC

- H01J 49/424: {Three-dimensional ion traps, i.e. comprising end-cap and ring electrodes}
- H01J 49/429: {Scanning an electric parameter, e.g. voltage amplitude or frequency}
- H01J: ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS (spark-gaps H01T; electric arc lamps H05B31/00; particle accelerators H05H)

## Abstract

An improvement of a fast scanning method in an ion trap mass spectrometer comprises setting the frequency and phase relationships between the ion trap storage frequency and the ion trap excitation frequency in such a way that the ions of consecutive masses each gain precisely the same "phase rhythm" or "phase sequence". The phase rhythm, or the historical succession of phase positions up to ion ejection, is optimally set in accordance with nonlinear resonance conditions used to cause ion ejection. The excitation voltage frequency is set to a value somewhat smaller that an integral fraction of the storage voltage frequency and the scan profile is set based on the excitation frequency so that the same time is required for ions of each mass to be ejected and so that precisely an integer number of cycles of the excitation frequency is used per mass.

## Claims

### Claim 1

A method for generating a mass spectrum of ions utilizing apparatus including a storage ion trap, a mechanism for introducing ions into the ion trap and a detector for detecting ions ejected from the trap and generating an output signal, the ions being ejected from the trap in groups of ion pulses, each of the ions in an ion pulse group having substantially equal mass and being ejected during an ejection cycle corresponding to that group, each ejection cycle being of a finite time duration, the method comprising:
applying to the storage ion trap with a storage signal generator an oscillating storage signal having an amplitude, a frequency and a phase;
applying to the storage ion trap with an excitation signal generator, an oscillating excitation signal having a frequency and a phase relative to the frequency and phase of the storage signal;
setting the frequency and phase of the excitation signal relative to the frequency and phase of the storage signal such that the phase of the excitation signal coincides with the phase of the storage signal periodically and the time period between said phase coincidences is t; and
varying the amplitude of the storage signal to consecutively eject ion pulse groups from the trap such that the time between the start of successive ejection cycles is constant and equal to t.

### Claim 2 (depends on 1)

A method according to claim 1 wherein setting the frequency and phase of the excitation signal relative to the frequency and phase of the storage signal comprises setting a frequency for the excitation signal which is slightly lower than a simple fraction of the storage frequency.

### Claim 3 (depends on 2)

A method according to claim 2 wherein, for an ion trap using a quadrupole field with a superposed hexapole field, setting the frequency and phase of the excitation signal relative to the frequency and phase of the storage signal comprises setting the excitation frequency (f.sub.e) relative to the storage frequency (f.sub.s) according to the equation f.sub.e =(r)(f.sub.s) where r=n/(3n+1) and n is an integer.

### Claim 4 (depends on 2)

A method according to claim 2 wherein, for an ion trap using a quadrupole field with a superposed octopole field, setting the frequency and phase of the excitation signal relative to the frequency and phase of the storage signal comprises setting the excitation frequency (f.sub.e) relative to the storage frequency (f.sub.s) according to the equation f.sub.e =(r)(f.sub.s) where r=n/(4n+1) and n is an integer.

### Claim 5 (depends on 1)

A method according to claim 1 wherein, for an ion trap using a quadrupole storage field, setting the frequency and phase of the excitation signal relative to the frequency and phase of the storage signal comprises setting the excitation frequency (f.sub.e) relative to the storage frequency (f.sub.s) according to the equation f.sub.e =(r) (f.sub.s) where r=n/(2n+1) and n is an integer.

### Claim 6 (depends on 3, 4, 5)

A method according to one of claims 5, 3 or 4 wherein n is greater than one and less than twenty-one.

### Claim 7 (depends on 1)

A method according to claim 1 wherein varying the amplitude of the storage signal further comprises varying the amplitude of the storage signal relative to the phases of the excitation signal and the storage signal such that the phase coincidences occur at the midpoint in time of each ejection cycle.

### Claim 8 (depends on 1)

A method according to claim 1 wherein varying the amplitude of the storage signal further comprises varying the amplitude of the storage signal relative to the phases of the excitation signal and the storage signal such that the phase coincidences occur at a time during each ejection cycle at which a maximum ion output is expected.

### Claim 9 (depends on 1)

A method according to claim 1 further comprising sampling the output signal of the detector with a phase sensitive amplifier.

### Claim 10

A method for generating a mass spectrum of ions utilizing apparatus including a storage ion trap, a mechanism for introducing ions into the ion trap and a detector for detecting ions ejected from the trap, the ions being ejected from the trap in groups of ion pulses, all of the ion pulses in an ion pulse group comprising ions of substantially equal masses and being ejected during an ejection cycle corresponding to that group, each ejection cycle being of a finite time duration, the method comprising:
applying to the storage ion trap with a storage signal generator an oscillating storage signal having an amplitude, a frequency and a phase;
applying to the storage ion trap with an excitation signal generator an oscillating excitation signal having a frequency and a phase relative to the frequency and phase of the storage signal;
setting the frequency and phase of the excitation signal relative to the frequency and phase of the storage signal to make the frequency of the excitation signal slightly smaller than a simple fraction of the frequency of the storage signal so that the phase of the excitation signal coincides with the phase of the storage signal periodically and the time period between successive phase coincidences is t; and
varying the amplitude of the storage signal to consecutively eject ion pulse groups from the trap such that the time between the start of successive ejection cycles is constant and equal to t and the phase coincidences occur at a time during each ejection cycle at which a maximum ion output is expected.

### Claim 11 (depends on 10)

A method according to claim 10 wherein the ion trap uses a quadrupole storage field and setting the excitation signal frequency and phase relative to the storage signal frequency and phase comprises setting the excitation frequency (f.sub.e) relative to the storage signal frequency (f.sub.s) according to the equation f.sub.e =(r)(f.sub.s) where r=n/(2n+1) and n is an integer.

### Claim 12 (depends on 10)

A method according to claim 10 wherein the ion trap uses a quadrupole storage field superposed by a hexapole field and setting the excitation signal frequency and phase relative to the storage signal frequency and phase comprises setting the excitation signal frequency (f.sub.e) relative to the storage signal frequency (f.sub.s) according to the equation f.sub.e =(r)(f.sub.s) where r=n/(3n+1) and n is an integer.

### Claim 13 (depends on 10)

A method according to claim 10 wherein the ion trap uses a quadrupole field superposed by an octopole field and setting the excitation signal frequency and phase relative to the storage signal frequency and phase comprises setting the excitation signal frequency (f.sub.e) relative to the storage signal frequency (f.sub.s) according to the equation f.sub.e =(r)(f.sub.s) where r=n/(4n+1) and n is an integer.

### Claim 14 (depends on 11, 12, 13)

A method according to claims 11, 12 or 13 wherein n is greater than one and less than twenty-one.

### Claim 15

Apparatus for recording a mass spectrum, the apparatus comprising:
a quadrupole storage ion trap;
a storage signal generator for applying to the storage ion trap an oscillating storage signal having an amplitude, a frequency and a phase;
an excitation signal generator for applying to the storage ion trap an oscillating excitation signal having a frequency and a phase relative to the frequency and phase of the storage signal;
an ion detection circuit for detecting ions ejected from the trap and generating an output signal, the ions being ejected from the trap in groups of ion pulses, all of the ion pulses in an ion pulse group comprising ions of substantially equal masses and being ejected during an ejection cycle corresponding to that group, each ejection cycle being of a finite time duration;
a frequency control circuit which sets the frequency of the excitation signal relative to the frequency of the storage signal such that the phase of the excitation signal coincides with the phase of the storage signal periodically and the time period between said phase coincidences is t; and
a scanning control circuit which varies the amplitude of the storage signal to consecutively eject ion pulse groups from the trap such that the time between the start of successive ejection cycles is constant and equal to t.

### Claim 16 (depends on 15)

Apparatus according to claim 15 wherein the frequency control circuit sets the frequency of the excitation signal frequency such that it is slightly lower than a simple fraction of the storage frequency.

### Claim 17 (depends on 16)

Apparatus according to claim 16 wherein the ion trap uses a quadrupole storage field and the excitation frequency (f.sub.e) is related to the storage frequency (f.sub.s) by the equation f.sub.e =(r)(f.sub.s) where r=n/(2n+1) and n is an integer.

### Claim 18 (depends on 16)

Apparatus according to claim 16 wherein the ion trap uses a quadrupole field with a superposed hexapole field and the excitation frequency (f.sub.e) is related to the storage frequency (f.sub.s) by the equation f.sub.e =(r)(f.sub.s) where r=n/(3n+1) and n is an integer.

### Claim 19 (depends on 16)

Apparatus according to claim 16 wherein the ion trap uses a quadrupole field with a superposed octopole field and the excitation frequency (f.sub.e) is related to the storage frequency (f.sub.s) by the equation f.sub.e =(r) (f.sub.s) where r=n/(4n+1) and n is an integer.

### Claim 20 (depends on 15)

Apparatus according to claim 15 wherein the scanning control circuit varies the amplitude of the storage frequency storage signal so that the midpoint of each ejection cycle occurs substantially at a time of one of said phase coincidences between the storage signal and the excitation signal.

### Claim 21 (depends on 20)

Apparatus according to claim 20 wherein the scanning control circuit varies the amplitude of the storage signal such that for each ejection cycle a time at which a maximum ion output is expected coincides with one of said phase coincidences between the storage signal and the excitation signal.

### Claim 22 (depends on 15)

Apparatus according to claim 15 further comprising a phase-sensitive amplifier which samples the output signal of the ion detector.

### Claim 23

Apparatus for recording a mass spectrum, the apparatus comprising:
a quadrupole ion trap;
a storage signal generator for applying to the ion trap an oscillating storage signal having an amplitude, a frequency and a phase;
an excitation signal generator for applying to the ion trap an oscillating excitation signal having a frequency and a phase relative to the frequency and phase of the storage signal;
an ion detection circuit for detecting ions ejected from the trap and for generating an output signal, the ions being ejected from the trap in groups of ion pulses, all of the ion pulses in an ion pulse group comprising ions of substantially equal masses and being ejected during an ejection cycle corresponding to that group, each ejection cycle being of a finite time duration;
a frequency control circuit for controlling the frequency and phase of the excitation signal relative to the frequency and phase of the storage signal such that the frequency of the excitation signal is slightly lower than a simple fraction of the storage frequency so that the phase of the excitation frequency coincides with the phase of the storage frequency periodically and the time period between successive phase coincidences is t; and
a scanning control circuit for varying the amplitude of the storage signal to consecutively eject ion pulse groups from the trap such that the time between the start of successive ejection cycles is constant and equal to t and said phase coincidences occur at a time during each ejection cycle at which a maximum ion output is expected.

### Claim 24 (depends on 23)

Apparatus according to claim 23 wherein the frequency control circuit comprises a microprocessor.

### Claim 25 (depends on 23)

Apparatus according to claim 23 wherein the frequency control circuit comprises a programmable logic array.

### Claim 26 (depends on 23)

Apparatus according to claim 23 wherein the frequency control circuit comprises a logic cell array.