Power supply for multipolar mass filter

• US 5,354,988 A
• Filed: 06/02/1993
• Issued: 10/11/1994
• Est. Priority Date: 10/24/1991
• Status: Expired due to Fees

• Current Assignee: Fisons PLC (Sanofi )
• Original Assignee: Fisons PLC (Sanofi )
• Inventors: Jullien, Paul
• Primary Examiner(s): Anderson, Bruce C.
• Application Number:
  US08/070,372
• Time in Patent Office: 496 Days
• Field of Search: 250/292, 250/281, 250/282
• US Class Current: 250/292
• CPC Class Codes: H01J 49/022 Circuit arrangements, e.g. for generating deviation currents or voltages regulating electric or magnetic variables in general, e.g. current, magnetic field G05F; Components associated with high voltage supply high voltage supply per se H02M
• CPC Class Codes: H01J 49/4215 Quadrupole mass filters H01J49/4225 takes precedence

Abstract

A quadrupole mass filter (1) includes a controllable RF oscillator (7) which follows any drift in the resonant frequency of a resonant circuit means (8), this circuit means (8) amplifying an alternating RF potential from the oscillator (7) and supplying it to the filter electrodes (2, 3, 4, 5). To ensure that the charge to mass ratio of the particles transmitted by the filter remains constant, a signal for controlling the amplitude of the oscillator (7) is corrected in response to any resonant frequency shift. This signal is also fed to DC supply means (12, 13, 15), to ensure that the amplitude of the DC potential applied to the electrodes (2, 3, 4, 5) remains in the correct ratio to the RF potential amplitude so that the filter resolution remains constant.

Claims

1. A multipolar mass filter (1) through which charged particles of a selected mass-to-charge ratio may be transmitted in response to the application to its electrodes of an alternating potential of selected amplitude and frequency, said filter comprising resonant circuit means (8) connected to the electrodes (2-5) of said filter, controllable radio-frequency oscillator means (7) for generating said alternating potential at a frequency determined by said resonant circuit means (8) and at an amplitude determined by an amplitude control signal, said mass filter being characterized by means (26-33, 18, 19) for adjusting the amplitude of said alternating potential in response to changes in the actual frequency of oscillation of said oscillator means (7) in order to maintain the transmission through said filter of charged particles of said selected mass-to-charge ratio.

2. A multipolar mass filter as claimed in claim 1 further comprising means (27-33) for correcting said amplitude control signal by a signal dependent on the actual frequency of said controllable radio-frequency oscillator means (7) before said amplitude control signal is applied to said oscillator means (7) to set the amplitude of said alternating potential.

3. A multipolar mass filter as claimed in claim 2 wherein a means for correcting comprises a timing oscillator (29-30) for controlling a gate (27) through which a signal representative of the frequency of said alternating potential passes to a counter (28), means (32) for squaring the digital count accumulated in said counter during a time determined by said timing oscillator (29, 20) and a digital-to-analogue convertor (33) for generating said amplitude control signal, said digital-to-analogue convertor receiving an analogue signal for setting the mass-to-charge ratio of charged particles to be transmitted by the filter and arranged to multiply it by the output of said means for squaring (32).

4. A multipolar mass filter as claimed in claim 3 wherein said controllable RF oscillator means (7) comprises a low-power oscillator (40) whose frequency is determined by a control signal, a radio-frequency power amplifier (37) driven by the output of said low-power oscillator (40) and a phase detector (53, 54) for comparing the phase of the input and output of said radio-frequency power amplifier connected in a control loop to set the frequency of said low-power oscillator so that the phase difference between said input and said output is minimized.

5. A multipolar mass filter as claimed in claim 3 wherein said controllable RF oscillator means (7) comprises a low-power oscillator (40) whose frequency is determined by a control signal, a radio-frequency power amplifier (37) driven by said low-power oscillator (40), means (51-39) for monitoring the current drawn by said amplifier (37), means for repeatedly changing the frequency of said low-power oscillator (40) over a limited range centered on a nominal frequency, which changes are small enough to have no significant effect on the performance of said mass filter, and means (38, 39), responsive to changes in the current drawn by said power amplifier (37) consequent upon said repeated frequency changes, for adjusting said nominal frequency of said low-power oscillator (40) until said changes in the current drawn substantially correspond to the changes expected when the frequency of said low-power oscillator is equal to the resonant frequency of said resonant circuit means (8).

6. A multipolar mass filter as claimed in claim 2 further comprising means (20-24, 18) for stabilizing the output amplitude of said controllable radio-frequency oscillator means (7) relative to said amplitude control signal.

7. A multipolar mass filter as claimed in claim 6 further comprising means (12, 13, 15) for applying direct potentials to the filter electrodes, and means for stabilizing said direct potentials relative to said amplitude control signal so that the ratio of said direct potentials and said alternating potentials is maintained substantially at a predetermined value.

8. A multipolar mass filter as claimed in claim 7 wherein said means for correcting comprises a timing oscillator (29-30) for controlling a gate (27) through which a signal representative of the frequency of said alternating potential passes to a counter (28), means (32) for squaring the digital count accumulated in said counter during a time determined by said timing oscillator (29, 20) and a digital-to-analogue convertor (33) for generating said amplitude control signal, said digital-to-analogue convertor receiving an analogue signal for setting the mass-to-charge ratio of charged particles to be transmitted by the filter and arranged to multiply it by the output of said means for squaring (32).

9. A multipolar mass filter as claimed in claim 1 further comprising means (20-24, 18) for stabilizing the output amplitude of said controllable radio-frequency oscillator means (7) relative to said amplitude control signal.

10. A multipolar mass filter as claimed in claim 1 further comprising means (12, 13, 15) for applying direct potentials to the filter electrodes, and means for stabilizing said direct potentials relative to said amplitude control signal so that the ratio of said direct potentials and said alternating potentials is maintained substantially at a predetermined value.

11. A multipolar mass filter as claimed in claim 1 wherein said controllable RF oscillator means (7) comprises a low-power oscillator (40) whose frequency is determined by a control signal, a radio-frequency power amplifier (37) driven by the output of said low-power oscillator (40) and a phase detector (53, 54) for comparing the phase of the input and output of said radio-frequency power amplifier connected in a control loop to set the frequency of said low-power oscillator so that the phase difference between said input and said output is minimized.

12. A multipolar mass filter as claimed in claim 1 wherein said controllable RF oscillator means (7) comprises a low-power oscillator (40) whose frequency is determined by a control signal, a radio-frequency power amplifier (37) driven by said low-power oscillator (40), means (51-39) for monitoring the current drawn by said amplifier (37), means for repeatedly changing the frequency of said low-power oscillator (40) over a limited range centered on a nominal frequency, which changes are small enough to have no significant effect on the performance of said mass filter, and means (38, 39), responsive to changes in the current drawn by said power amplifier (37) consequent upon said repeated frequency changes, for adjusting said nominal frequency of said low-power oscillator (40) until said changes in the current drawn substantially correspond to the changes expected when the frequency of said low-power oscillator is equal to the resonant frequency of said resonant circuit means (8).

13. A multipolar mass filter as claimed in claim 12 wherein said means (38, 39) responsive to changes in the current drawn by said power amplifier (37) is further responsive to said amplitude control signal, means (38) are provided for comparing at two or more measurement times during any one of said repeated frequency changes the actual current drawn by said amplifier with the current expected to be drawn when the frequency of said oscillator is equal to the resonant frequency of said resonant circuit means according to the value at said measurement time of said amplitude control signal, and means (38) are provided for adjusting the nominal frequency of said low-power oscillator (40) until said actual and expected currents at each said measurement time are substantially equal.

14. A method of operating a multipolar mass filter (1) through which charged particles of a selected mass-to-charge ratio may be transmitted and to which is applied through resonant circuit means (8) an alternating potential whose frequency is determined by said resonant circuit means and whose amplitude is determined by an amplitude control signal, said method being characterized by adjusting the amplitude of said alternating potential in response to changes in the actual frequency of said alternating potential to maintain the transmission through said mass filter of said charged particles of selected mass-to-charge ratio.

15. A method of operating a multipolar mass filter as claimed in claim 14 further comprising stabilizing the amplitude of said alternating potential with respect to said amplitude control signal and applying to the electrodes of said filter direct potentials which are also stabilized with respect to said amplitude control signal to maintain the ratio of said direct potentials to said alternating potential at a predetermined value.

16. A method as claimed in claim 15 further comprising the steps of:

a) passing a signal representative of the frequency of said alternating potential through a gate for a period of time determined by a timing oscillator;

b) counting said signal representative of said frequency for as long as said gate is open;

c) squaring the count accumulated during step b) and converting the result to a correction signal;

d) correcting said amplitude control signal by said correction signal to adjust the amplitude of said alternating potential to maintain the transmission of said charged-particles of selected mass through said filter, irrespective of the frequency of said alternating potential.

17. A method as claimed in claim 16 further comprising the steps of:

a) generating said alternating potential by means of a low-power variable-frequency oscillator;

b) amplifying said alternating potential by an amplifier whose gain is determined by an amplitude control signal;

c) repeatedly changing the frequency of said alternating potential over a limited range about a nominal frequency, said limited range being small enough to have no significant effect on the performance of said mass filter;

d) monitoring the current drawn by the amplifier used in step b) during said repeated frequency changes;

e) adjusting said nominal frequency until said repeated current changes substantially correspond with those expected when said nominal frequency is coincident with the resonant frequency of said resonant circuit means.

18. A method as claimed in claim 14 further comprising the steps of:

a) passing a signal representative of the frequency of said alternating potential through a gate for a period of time determined by a timing oscillator;

b) counting said signal representative of said frequency for as long as said gate is open;

c) squaring the count accumulated during step b) and converting the result to a correction signal;

d) correcting said amplitude control signal by said correction signal to adjust the amplitude of said alternating potential to maintain the transmission of said charged-particles of selected mass through said filter, irrespective of the frequency of said alternating potential.

19. A method as claimed in claim 14 further comprising the steps of:

a) generating said alternating potential by means of a low-power variable-frequency oscillator;

b) amplifying said alternating potential by an amplifier whose gain is determined by an amplitude control signal;

c) repeatedly changing the frequency of said alternating potential over a limited range about a nominal frequency, said limited range being small enough to have no significant effect on the performance of said mass filter;

d) monitoring the current drawn by the amplifier used in step b) during said repeated frequency changes;

e) adjusting said nominal frequency until said repeated current changes substantially correspond with those expected when said nominal frequency is coincident with the resonant frequency of said resonant circuit means.

20. A method as claimed in claim 19 further comprising the step of comparing at two or more measurement times during any one of said repeated frequency changes the actual current drawn by said amplifier with the current expected to be drawn when said frequency is equal to the resonant frequency of said resonant circuit means according to the value at said measurement time of said amplitude control signal, and adjusting said nominal frequency until said measured and said expected currents at each said measurement time are substantially equal.