Method and apparatus for providing tailored excitation as in Fourier transform mass spectrometry

• US 5,248,882 A
• Filed: 05/28/1992
• Issued: 09/28/1993
• Est. Priority Date: 05/28/1992
• Status: Expired due to Term

• Current Assignee: Extrel Ftms
• Original Assignee: Extrel FTMS, Inc. (Thermo Fisher Scientific Incorporated)
• Inventors: Liang, Zhenmin
• Primary Examiner(s): Anderson, Bruce C.
• Application Number:
  US07/890,623
• Time in Patent Office: 488 Days
• Field of Search: 250/282, 250/291, 250/286
• US Class Current: 250/291
• CPC Class Codes: B01D 59/44 Separation by mass spectrography particle spectrometers or separator tubes H01J49/00
• CPC Class Codes: H01J 49/38 Omegatrons ; using ion cyclotron resonance
• CPC Class Codes: H01J 49/424 Three-dimensional ion traps, i.e. comprising end-cap and ring electrodes
• CPC Class Codes: H01J 49/427 Ejection and selection methods

Abstract

Tailored excitation of ions in a mass spectrometer is obtained by using an excitation signal which comprises at least one signal having the form of a sinc function modulated sine wave. The sinc modulated sine wave has a magnitude function in the frequency domain in the form of a rectangular function centered at the frequency of the sine wave and having a width determined by the width of the sinc function. Plural sinc modulated sine wave signals can be applied to the ion trap of the spectrometer, with the various signals having different sine wave frequencies, to provide a tailored excitation spectrum without the need for extended computation.

Claims

1. Mass spectrometry apparatus comprising:

(a) an ion trap including a plurality of electrode plates;

(b) means for detecting motion of ions in the trap and providing a signal indicative thereof;

(c) excitation means connected to the ion trap for producing an electric field in the trap, wherein the excitation means generates a sine wave signal at a selected frequency and a sinc function signal of a selected width and center time and multiplies the two signals to provide an excitation signal which is applied to plates of the ion trap, whereby the magnitude spectrum of the excitation signal in the frequency domain is a substantially rectangular function centered on the frequency of the sine wave signal and having a width determined by the width of the sinc function signal.

2. The apparatus of claim 1 wherein the excitation signal E(t) is generated in accordance with the expression:

##EQU3## where t₀ is the desired center time at the maximum of the sinc function, W is the width of the sinc function, which corresponds to one-half the bandwidth of the rectangular excitation function in the frequency domain, t is time, and f is the frequency of the sine wave.

3. The apparatus of claim 2 wherein the excitation means provides a composite signal which is the sum of plural excitation signals, each excitation signal having a different sine wave frequency f and with the width W of each signal selected so that the bandwidth of the rectangular functions in the frequency domain of each of the individual sinc modulated sine wave signals do not overlap.

4. The apparatus of claim 2 wherein the time t₀ of the maximum of each sinc modulated sine wave component of the excitation signal differs from the time of the maximum of all the other components.

5. The apparatus of claim 1 wherein the excitation means generates an excitation signal comprised of the sum of a plurality of excitation signals each comprising a sinc modulated sine wave, each sinc modulated sine wave having a different sine wave frequency and the width of each sinc modulated sine wave being chosen so that the bandwidths of the rectangular functions of each sinc modulated sine wave in the frequency domain do not overlap.

6. The apparatus of claim 1 wherein the excitation means includes means for mixing a first higher frequency carrier signal with a time domain signal and wherein the excitation means produces an electric field in the trap which varies in accordance with the first higher frequency signal modulated by the time domain signal.

7. The apparatus of claim 1 wherein the excitation means includes:

(a) sinc function digital memory storing digital data in locations which can be sequentially read out to provide an output signal wherein the data when read out follows a sinc function;

(b) sine function digital memory storing digital data in locations which can be sequentially read out to provide an output signal wherein the data when read out follows a sine function;

(c) multiplying means for multiplying the output signal of the sinc function digital memory with the output signal of the sine function digital memory to provide a digital output signal;

(d) a digital-to-analog converter connected to receive digital data input from the multiplying means and connected to provide its analog output signal to the ion trap;

(e) means for selectively controlling the output of digital data stored in the sinc function and sine function digital memories to the multiplying means to apply a desired time domain excitation signal to the ion trap.

8. The apparatus of claim 1 wherein the excitation signal E(t) is a composite excitation signal, having a selected number n of signal components, which is generated in accordance with the expression:

##EQU4## where t is time and the widths W₁, . . . , W_n, the center times t₀₁, . . . , t_on, the sine wave frequencies f₁, . . . , f_n, and the component magnitudes M₁, . . . , M_n are excitation signal parameters selected by the user.

39. The method of claim 3 wherein the excitation signal E(t) is generated in accordance with the expression:

##EQU13## where t₀ is the desired center time at the maximum of the sinc function, W is the width of the sinc function, which corresponds to one-half the bandwidth of the rectangular excitation function in the frequency domain, t is time, and f is the frequency of the sine wave.

40. The method of claim 39 wherein the excitation signal is a composite signal which is the sum of the plural excitation signals, each excitation signal having a different sine wave frequency f and with the width W of each signal selected so that the bandwidth of the rectangular functions in the frequency domain of each of the individual sinc modulated sine wave signals do not overlap.

41. The method of claim 40 wherein the time t₀ of the maximum of each sinc modulated sine wave component of the excitation signal differs from the time of the maximum of all of the other components.

9. Mass spectrometry apparatus comprising:

(a) an ion trap including a plurality of electrode plates;

(b) means for detecting motion of ions in the trap and providing a signal indicative thereof;

(c) excitation means connected to the ion trap for producing an electric field in the trap, the excitation means including;

(1) sinc function digital memory storing digital data in locations which can be sequentially read out to provide an output signal wherein the data when read out follows a sinc function;

(2) sine function digital memory storing digital data in locations which can be sequentially read out to provide an output signal wherein the data when read out follows a sine function;

(3) multiplying means for multiplying the output signal of the sinc function digital memory with the output signal of the sine function digital memory to provide a digital output signal;

(4) a digital-to-analog converter connected to receive digital data input from the multiplying means and connected to provide its analog output signal to the ion trap;

(5) means for selectively controlling the output of digital data stored in the sinc function and sine function digital memories to the multiplying means to apply a desired time domain excitation signal to the ion trap.

10. The apparatus of claim 9 wherein the excitation signal E(t) is generated in accordance with the expression:

##EQU5## where t₀ is the desired center time at the maximum of the sinc function, W is the width of the sinc function, which corresponds to one-half the bandwidth of the rectangular excitation function in the frequency domain, t is time, and f is the frequency of the sine wave.

11. The apparatus of claim 10 wherein the excitation means provides a composite signal which is the sum of plural excitation signals, each excitation signal having a different sine wave frequency f and with the width W of each signal selected so that the bandwidth of the rectangular functions in the frequency domain of each of the individual sinc modulated sine wave signals do not overlap.

12. The apparatus of claim 11 wherein the time t₀ of the maximum of each sinc modulated sine wave component of the excitation signal differs from the time of the maximum of all the other components.

13. The apparatus of claim 9 wherein the excitation means generates an excitation signal comprised of the sum of a plurality of excitation signals each comprising a sinc modulated sine wave, each sinc modulated sine wave having a different sine wave frequency and the width of each sinc modulated sine wave being chosen so that the bandwidths of the rectangular functions of each sinc modulated sine wave in the frequency domain do not overlap.

14. The apparatus of claim 9 wherein the excitation means includes means for mixing a first higher frequency carrier signal with a time domain signal and wherein the excitation means produces an electric field in the cell which varies in accordance with the first higher frequency signal modulated by the time domain signal.

15. The apparatus of claim 9 wherein the excitation signal E(t) is a composite excitation signal, having a selected number n of signal components, which is generated in accordance with the expression:

##EQU6## where t is time and the widths W₁, . . . , W_n, the center times t₀₁, . . . , t₀, the sine wave frequencies f₁, . . . , f_n, and the component magnitudes M₁, . . . , M_n are excitation signal parameters selected by the user.

16. In an ion cyclotron resonance mass spectrometer apparatus of the type having an ion cyclotron resonance trap cell including excitation plates and detection plates, a magnet producing a substantially constant unidirectional magnetic field through the ion cyclotron resonance cell such that the electric field from potentials applied to the excitation plates is transverse to the applied magnetic field, means connected to the detector plates of the cell for detecting resonance motion of ions in the cell and providing a signal indicative thereof, and an excitation amplifier connected to the excitation plates for applying electrical potentials to the plates to form an electric field between the plates in accordance with the input signal to the excitation amplifier means, the improvement comprising:

excitation generator means connected to the excitation amplifier for providing an excitation signal to the amplifier, wherein the excitation generator generates a sine wave signal at a selected frequency and a sinc function signal of a selected width and center time and multiplies the two signals to provide the excitation signal, whereby the magnitude spectrum of the excitation signal in the frequency domain is a substantially rectangular function centered on the frequency of the sine wave signal and having a width determined by the width of the sinc function signal.

17. The apparatus of claim 16 wherein the excitation signal E(t) is generated in accordance with the expression:

##EQU7## where t₀ is the desired center time at the maximum of the sinc function, W is the width of the sinc function, which corresponds to one-half the bandwidth of the rectangular excitation function in the frequency domain, t is time, and f is the frequency of the sine wave.

18. The apparatus of claim 17 wherein the excitation means provides a composite signal which is the sum of plural excitation signals, each excitation signal having a different sine wave frequency f and with the width W of each signal selected so that the bandwidth of the rectangular functions in the frequency domain of each of the individual sinc modulated sine wave signals do not overlap.

19. The apparatus of claim 18 wherein the time t₀ of the maximum of each sinc modulated sine wave component of the excitation signal differs from the time of the maximum of all the other components.

20. The apparatus of claim 16 wherein the excitation means generates an excitation signal comprised of the sum of a plurality of excitation signals each comprising a sinc modulated sine wave, each sinc modulated sine wave having a different sine wave frequency and the width of each sinc modulated sine wave being chosen so that the bandwidths of the rectangular functions of each sinc modulated sine wave in the frequency domain do not overlap.

21. The apparatus of claim 16 wherein the excitation means includes means for mixing a first higher frequency carrier signal with a time domain signal and wherein the excitation means produces an electric field in the cell which varies in accordance with the first higher frequency signal modulated by the time domain signal.

22. The apparatus of claim 16 wherein the excitation means includes:

(a) sinc function digital memory storing digital data in locations which can be sequentially read out to provide an output signal wherein the data when read out follows a sinc function;

(b) sine function digital memory storing digital data in locations which can be sequentially read out to provide an output signal wherein the data when read out follows a sine function;

(c) multiplying means for multiplying the output signal of the sinc function digital memory with the output signal of the sine function digital memory to provide a digital output signal;

(d) a digital-to-analog converter connected to receive digital data input from the multiplying means and connected to provide its analog output signal to the ion cell;

(e) means for selectively controlling the output of digital data stored in the sinc function and sine function digital memories to the multiplying means to apply a desired time domain excitation signal to the ion cell.

23. The apparatus of claim 16 wherein the excitation signal E(t) is a composite excitation signal, having a selected number n of signal components, which is generated in accordance with the expression:

##EQU8## where t is time and the widths W₁, . . . , W_n, the center times t₀₁, . . . , t₀, the sine wave frequencies f₁, . . . , f_n, and the component magnitudes M₁, . . . , M_n are excitation signal parameters selected by the user.

24. A method of providing tailored excitation to a spectrometer having excitation electrodes, comprising the steps of:

(a) generating a sine wave signal of a selected frequency;

(b) generating a sinc function signal of a selected width and center time;

(c) multiplying the sinc function signal and the sine function signal to provide a time varying excitation signal; and

(d) applying the excitation signal to the excitation electrodes whereby a time varying excitation field is formed having one or more substantially rectangular components in the frequency domain.

25. The method of claim 24 wherein the excitation signal E(t) is generated in accordance with the expression:

##EQU9## where t₀ is the desired center time at the maximum of the sinc function, W is the width of the sinc function, which corresponds to one-half the bandwidth of the rectangular excitation function in the frequency domain, t is time, and f is the frequency of the sine wave.

26. The method of claim 25 wherein the excitation signal is a composite signal which is the sum of plural excitation signals, each excitation signal having a different sine wave frequency f and with the width W of each signal selected so that the bandwidth of the rectangular functions in the frequency domain of each of the individual sinc modulated sine wave signals do not overlap.

27. The method of claim 25 wherein the time t₀ of the maximum of each sinc modulated sine wave component of the excitation signal differs from the time of the maximum of all of the other components.

28. The method of claim 24 wherein the excitation signal is comprised of the sum of a plurality of excitation signals each comprising a sinc modulated sine wave, each sinc modulated sine wave having a different sine wave frequency and the width of each sinc modulated sine wave being chosen so that the bandwidths of each sinc modulated sine wave in the frequency domain do not overlap.

29. The method of claim 24 wherein the excitation signal E(t) is a composite excitation signal, having a selected number n of signal components, which is generated in accordance with the expression:

##EQU10## where t is time and the widths W₁, . . . , W_n, the center times t₀, . . . , t_on, the sine wave frequencies f₁, . . . , f_n, and the component magnitudes M₁, . . . , M_n are excitation signal parameters selected by the user.

30. In an ion trap apparatus of the type having a ring electrode and end electrodes, a source of ions, and means for detecting ions to produce a signal indicative thereof, the improvement comprising:

excitation means connected to the end electrodes of the trap for producing an electric field in the trap, wherein the excitation means generates a sine wave signal at a selected frequency and a sinc function signal of a selected width and center time and multiplies the two signals to provide an excitation signal which is applied to electrodes of the ion trap, whereby the magnitude spectrum of the excitation signal in the frequency domain is a substantially rectangular function centered on the frequency of the sine wave signal and having a width determined by the width of the sinc function signal.

31. The apparatus of claim 30 wherein the excitation signal E(t) is generated in accordance with the expression:

##EQU11## where t₀ is the desired center time at the maximum of the sinc function, W is the width of the sinc function, which corresponds to one-half the bandwidth of the rectangular excitation function in the frequency domain, t is time, and f is the frequency of the sine wave.

32. The apparatus of claim 31 wherein the excitation means provides a composite signal which is the sum of plural excitation signals, each excitation signal having a different sine wave frequency f and with the width W of each signal selected so that the bandwidth of the rectangular functions in the frequency domain of each of the individual sinc modulated sine wave signals do not overlap.

33. The apparatus of claim 32 wherein the time t₀ of the maximum of each sinc modulated sine wave component of the excitation signal differs from the time of the maximum of all the other components.

34. The apparatus of claim 30 wherein the excitation means generates an excitation signal comprised of the sum of a plurality of excitation signals each comprising a sinc modulated sine wave, each sinc modulated sine wave having a different sine wave frequency and the width of each sinc modulated sine wave being chosen so that the bandwidths of the rectangular functions of each sinc modulated sine wave in the frequency domain do not overlap.

35. The apparatus of claim 30 wherein the excitation means includes means for mixing a first higher frequency carrier signal with a time domain signal and wherein the excitation means produces an electric field in the trap which varies in accordance with the first higher frequency signal modulated by the time domain signal.

36. The apparatus of claim 30 wherein the excitation means includes:

(a) sinc function digital memory storing digital data in locations which can be sequentially read out to provide an output signal wherein the data when read out follows a sinc function;

(b) sine function digital memory storing digital data in locations which can be sequentially read out to provide an output signal wherein the data when read out follows a sine function;

(c) multiplying means for multiplying the output signal of the sinc function digital memory with the output signal of the sine function digital memory to provide a digital output signal;

(d) a digital-to-analog converter connected to receive digital data input from the multiplying means and connected to provide its analog output signal to the ion trap;

(e) means for selectively controlling the output of digital data stored in the sinc function and sine function digital memories to the multiplying means to apply a desired time domain excitation signal to the ion trap.

37. The apparatus of claim 36 wherein the excitation signal E(t) is a composite excitation signal, having a selected number n of signal components, which is generated in accordance with the expression:

##EQU12## where t is time and the widths W₁, . . . , W_n, the center times t₀₁, . . . , t_on, the sine wave frequencies f₁, . . . , f_n, and the component magnitudes M₁, . . . , M_n are excitation signal parameters selected by the user.

38. A method of ejecting selected mass-to-charge ratio ions from an ion trap of the type having a ring electrode and end electrodes, comprising the steps of:

(a) generating a sine wave signal at a selected frequency;

(b) generating a sinc function signal having a selected width and center time;

(c) multiplying the sine wave signal times the sinc function signal to provide an output excitation signal; and

(d) applying a voltage to the end electrodes of the ion trap to create an electric field in the ion trap which has a time domain waveform which corresponds to the excitation signal waveform to eject ions having mass-to-charge ratios which generally correspond to the frequency of the sine wave signal in the excitation signal.

42. The method of claim 38 wherein the excitation signal is comprised of the sum of a plurality of excitation signals each comprising a sinc modulated sine wave, each sinc modulated sine wave having a different sine wave frequency and the width of each sinc modulated sine wave being chosen so that the bandwidths of each sinc modulated sine wave in the frequency domain do not overlap.

43. The method of claim 38 wherein the excitation signal E(t) is a composite excitation signal, having a selected number N of signal components, which is generated in accordance with the expression:

##EQU14## where t is time and the widths W₁, . . . , W_n, the center times t₀₁, . . . , t_on, the sine wave frequencies f₁, . . . , f_n, and the component magnitudes M₁, . . . , M_n are excitation signal parameters selected by the user.

44. A method of obtaining mass spectra from a mass spectrometer having an ion trap, comprising the steps of:

(a) generating a sine wave signal at a selected frequency and a sinc function signal having a selected width and center time and multiplying the two signals to provide an excitation signal, whereby the magnitude spectrum of the excitation signal in the frequency domain is a substantially rectangular function centered on the frequency of the sine wave signal and having a width determined by the width of the sinc function signal;

(b) applying an electric field to the ion trap which has a time domain waveform which corresponds to the excitation signal at a power level to eject ions having mass to charge ratios near the frequency of the sine wave signal; and

(c) thereafter applying a broad band excitation to the ion trap to acquire a mass spectrum containing peaks corresponding to the ions remaining in the trap.