Amplifier amplitude control for a mass spectrometer

Patent metadata

Field	Value
Publication number	US-11456166-B2
Application number	US-202117194419-A
Country	US
Kind code	B2
Filing date	Mar 8, 2021
Priority date	Oct 25, 2019
Publication date	Sep 27, 2022
Grant date	Sep 27, 2022

Abstract

Control of an amplitude of a signal applied to a component of a mass spectrometer is described. In one aspect, a mass spectrometer includes a component and a resonant circuit to generate a radio frequency (RF) signal applied to the component. An amplitude control circuit can be inductively coupled with inductors of the resonant circuit to selectively discharge energy from the resonant circuit and, therefore, adjust the amplitude of the signal in particular situations.

First claim

I claim:

1. A mass spectrometer, comprising:
a component of the mass spectrometer;
a resonant circuit configured to generate a first radio frequency (RF) signal applied to the component, the resonant circuit having a first resonant inductor used to store energy for generating the first RF signal at a first amplitude;
an amplitude control circuit having a first amplitude control inductor that is inductively coupled with the first resonant inductor, and having a first diode that is coupled with the first amplitude control inductor; and
a controller circuit configured to transfer energy from the first resonant inductor to the first amplitude control inductor to adjust the first RF signal from the first amplitude to a second amplitude by changing an operational state of the first diode.

2. The mass spectrometer of claim 1 , wherein the first resonant inductor has a higher inductance than the first amplitude control inductor.

3. The mass spectrometer of claim 1 , wherein the operational state of the first diode is changed from being in a reverse bias mode of operation to a forward bias mode of operation.

4. The mass spectrometer of claim 1 , wherein the first RF signal is applied to a first pair of rods of the component, wherein the component includes a second pair of rods, the resonant circuit is configured to generate a second RF signal applied to the second pair of rods, the resonant circuit having a second resonant inductor used to store energy for generating the second RF signal at the first amplitude, wherein the amplitude control circuit includes a second amplitude control inductor that is inductively coupled with the second resonant inductor, and having a second diode that is coupled with the second amplitude control inductor, and wherein the controller circuit is configured to transfer energy from the second resonant inductor to the second amplitude control inductor to adjust the second RF signal from the first amplitude to the second amplitude by changing an operational state of the second diode.

5. The mass spectrometer of claim 4 , wherein a cathode of the first diode is coupled with a cathode of the second diode to define a cathode node, and wherein the controller circuit is configured to bias the cathode node to change the operational state of one or both of the first diode or the second diode.

6. The mass spectrometer of claim 1 , wherein the amplitude control circuit further includes a switch, and the controller circuit is further configured to operate the switch to bias a cathode of the first diode to change the operational state.

7. The mass spectrometer of claim 6 , wherein the controller is further configured to determine a bleed down time representative of a time for adjusting the first RF signal from the first amplitude to the second amplitude, and configured to operate the switch to bias the cathode of the first diode for the bleed down time.

8. The mass spectrometer of claim 1 , wherein the first resonant inductor and the first amplitude control inductor are air core coils.

9. The mass spectrometer of claim 1 , wherein the first amplitude control inductor includes one or more coils that are wound around coils of the first resonant inductor.

10. The mass spectrometer of claim 1 , wherein the resonant circuit is defined by an inductance of the first resonant inductor and a capacitance of a pair of rods of the component.

11. The mass spectrometer of claim 1 , wherein the first diode is a Schottky diode.

12. An apparatus, comprising:
a component for a mass spectrometer configured to manipulate ions by generating an oscillating electric field;
a resonant circuit configured to store energy using a first resonant inductor and use the energy to generate a signal applied to the component to generate the electric field; and
an amplitude control circuit configured to transfer energy from the first resonant inductor using a first amplitude control inductor to adjust an amplitude of the signal applied to the component.

13. The apparatus of claim 12 , wherein the amplitude control circuit includes a first diode having an anode coupled with the first amplitude control inductor.

14. The apparatus of claim 13 , further comprising:
a controller circuit configured to bias a cathode of the first diode to transfer the energy away from the first resonant inductor to reduce the amplitude of the signal.

15. The apparatus of claim 13 , wherein the diode is a Schottky diode.

16. The apparatus of claim 12 , wherein the first resonant inductor has a higher inductance than the first amplitude control inductor.

17. A method of operating a mass spectrometer, comprising:
applying a voltage at a cathode of a diode;
applying a radio frequency (RF) signal having a first amplitude to a component for a mass spectrometer via a resonant circuit having a resonant circuit inductor;
applying a voltage to an anode of the diode via inductive coupling of the resonant circuit and the anode of the diode; and
discharging energy from the resonant circuit to adjust the first amplitude of the RF signal applied to the component to a second amplitude based on the inductive coupling and the voltages applied at the cathode and the anode of the diode.

18. The method of claim 17 , further comprising:
determining a bleed down time indicative of a time for adjusting the first amplitude of the RF signal to the second amplitude; and
applying the voltage at the cathode of the diode in accordance with the bleed down time.

19. The method of claim 17 , wherein discharging the energy from the resonant circuit is based on changing an operational mode of the diode from a non-conductive state to a conductive-state based on the voltages applied to the cathode and the diode.

20. The method of claim 17 , wherein the diode is a Schottky diode.

Assignees

• Thermo Finnigan Llc

Inventors

• Smith Johnathan Wayne

Classifications

• H03F1/34 Primary

  Negative-feedback-circuit arrangements with or without positive feedback (H03F1/02 - H03F1/30, H03F1/38 - H03F1/50, H03F3/50 take precedence {; for rejection of common mode signals H03F3/45479}) · CPC title

• H01J49/427

  Ejection and selection methods · CPC title

• H01J49/022 Primary

  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 title

• H01J49/063

  Multipole ion guides, e.g. quadrupoles, hexapoles · CPC title

• H01J49/0031

  Step by step routines describing the use of the apparatus (H01J49/0081 takes precedence) · CPC title