Electrostatic mass spectrometer with encoded frequent pulses

Patent metadata

Field	Value
Publication number	US-9406493-B2
Application number	US-201414506270-A
Country	US
Kind code	B2
Filing date	Oct 3, 2014
Priority date	Apr 30, 2010
Publication date	Aug 2, 2016
Grant date	Aug 2, 2016

Abstract

A method, apparatus and algorithms are disclosed for operating an open electrostatic trap (E-trap) or a multi-pass TOF mass spectrometer with an extended flight path. A string of start pulses with non equal time intervals is employed for triggering ion packet injection into the analyzer, a long spectrum is acquired to accept ions from the entire string and a true spectrum is reconstructed by eliminating or accounting overlapping signals at the data analysis stage while using logical analysis of peak groups. The method is particularly useful for tandem mass spectrometry wherein spectra are sparse. The method improves the duty cycle, the dynamic range and the space charge throughput of the analyzer and of the detector, so as the response time of the E-trap analyzer. It allows flight extension without degrading E-trap sensitivity.

First claim

What is claimed is:

1. An electrostatic mass spectrometer comprising:
(a) a pulsed ion source for ion packet formation;
(b) an ion detector;
(c) a multi-pass electrostatic mass analyzer providing an ion packet passage though said analyzer in a Z-direction and isochronous ion oscillations in the locally orthogonal direction X;
(d) a pulse string generator for triggering said pulsed ion source or pulsed converter with time intervals between any pair of start pulses being unique within the peak time width AT on the detector;
(e) a data acquisition system recording of detector signal at the duration of said pulse string and for summing spectra corresponding to multiple pulse strings;
(f) a main pulse generator for triggering both—said data acquisition system and said pulse string generator; and
(g) a spectral decoder for reconstructing mass spectra based on the detector signal and on the information on the preset time intervals of said start pulses.

2. An apparatus as set forth in claim 1 , wherein within the pulse string, for any non-equal numbers of start pulses i and j, the start times T i , and T j satisfy one condition of the group: (i) |(T i+1 −T i )−(T j+1 −T j )|>ΔT; (ii) T j =j*(T 1 +T 2 *j*(j−1)), wherein 1 us<T 1 <100 us and 5 ns<T 2 <1000 ns.

3. An apparatus as set forth in claim 1 , wherein the electrodes of said electrostatic analyzer are parallel and are linearly extended in Z-direction to thereby provide a two-dimensional electrostatic filed of planar symmetry.

4. An apparatus as set forth in claim 1 , wherein said electrostatic analyzer comprises parallel and coaxial ring electrodes to thereby provide a toroidal volume with a two-dimensional electrostatic filed of cylindrical symmetry.

5. An apparatus as in claim 4 , wherein the mean radius of said toroidal volume is larger than one sixth of ion path per single oscillation and wherein said analyzer has at least one ring electrode for radial ion deflection.

6. An apparatus as set forth in claim 1 , wherein said electrostatic analyzer comprises one set of electrodes selected from the group consisting of: (i) at least two electrostatic ion mirrors spaced by field-free region; (ii) at least two electrostatic sectors; and (iii) at least one ion mirror and at least one electrostatic sector.

7. An apparatus as set forth in claim 6 , wherein said electrostatic analyzer is an open ion trap with a non fixed ion path and wherein the number of ion oscillations M in said analyzer has one span ΔM of the group: (i) from 2 to 3; (ii) from 3 to 10; (iii) from 10 to 30; and (iv) from 30 to 100.

8. An apparatus as set forth in claim 7 , wherein said electrostatic analyzer comprises a multi-pass time-of-flight mass analyzer with a fixed flight path which and one means for limiting ion divergence in the Z-direction of the group: (i) a set of periodic lens; (ii) electrostatic mirrors modulated in the Z-direction; (iii) electrostatic sector modulated in the Z-direction; and (iv) at least two slits.

9. An apparatus as set forth in claim 8 , wherein said pulsed source comprises one orthogonal pulsed converter selected from the group consisting of: (i) an orthogonal pulsed accelerator; (i) a grid-free orthogonal pulsed accelerator; (iii) a radiofrequency ion guide with pulsed orthogonal extraction; (iv) an electrostatic ion guide with pulsed orthogonal extraction; and (v) any of the above accelerators preceded by an upstream accumulating radio-frequency ion guide.

10. An apparatus as in claim 9 , wherein said converter is tilted relative to Z axis and an additional deflector steers ion packets at the same angle after at least one ion reflection or turn within said electrostatic analyzer.

11. A method of mass spectral analysis comprising:
(a) frequent pulsing of a pulsed source with a pulse string generator;
(b) signal encoding with pulse strings having uneven intervals;
(c) generating a pulse with a main pulse generator to trigger (i) a data acquisition system and (ii) said pulse string generator;
(d) passing ion packets through an electrostatic analyzer in a Z-direction such that said packets isochronously oscillate in an orthogonal X-direction;
(e) acquiring long spectra corresponding to string duration; and
(f) subsequent spectra decoding using the information on predetermined uneven pulse intervals.

12. A method as set forth in claim 11 , further comprising one step of the group consisting of: (i) discarding peaks overlapping between series; and (ii) separating partially overlapping peaks based on the information deduced from the non-overlapping peaks in related series and assigning thus separated peaks to the related series.

13. A method as set forth in claim 12 , wherein within the pulse string, for any non-equal numbers of start pulses i and j, start times T i and T j satisfy one condition of the group: (i) ∥T i−1 −T i |−|T j+1 −T j ∥>ΔT; (ii) T j =j*T 12 +T 2 *j*(j−1), where T 1 >>T 2 ; and wherein T 1 is from 10 to 100 us and T 2 is from 5 to 100 ns.

14. A method as set forth in claim 13 , wherein number of start pulses S in said pulse string is selected from the group consisting of: (i) from 3 to 10; (ii) from 10 to 30; (iii) from 30 to 100; (iv) between 100 and 300; and (v) over 300.

15. A method as set forth in claim 14 , wherein the ion path between said pulsed ion source and said detector is equal to an integer number of oscillations M within a span ΔM and wherein said spread ΔM in number of reflections is one of the group: (i) from 2 to 3; (ii) from 3 to 10; (iii) from 10 to 30; and (iv) from 30 to 100.

16. A method as set forth in claim 15 , further comprising at least one step of the group consisting of: (i) adjusting source emittance under 20 mm2*eV; (ii) accelerating to provide angular-spatial divergence of less than 20 mm*mrad; (iii) adjusting the packet divergence by at least one lens to less than 1 mrad; and (iv) limiting angular divergence by at least two slits within said electrostatic analyzer.

17. A method as set forth in claim 16 , wherein said electrostatic analyzer field is formed by at least four electrodes with distinct potentials, and wherein said field comprises at least one spatial focusing field of an accelerating lens such that to provide a time-of-flight focusing relative to small deviations in spatial, angular, and energy spreads of ion packets to an nth order of the Tailor expansion, and further wherein said order of the aberration compensation is selected from the group consisting of: (i) at least first-order, (ii) at least second-order relative to all spreads and including cross terms, and (iii) at least third-order relative to energy spread of ion packets.

18. A method as set forth in claim 17 , further comprising a step of ion separation prior to said step of pulsed packets formation, and wherein said upstream separation step comprises one or more of the group consisting of: (i) an ion mobility separation; (ii) a differential mobility separation; (iii) a filter mass spectrometer for passing through one m/z component in a time; (iv) an ion trapping followed by mass dependent sequential release; (v) an ion trapping with a time-of-flight mass separation; and (vi) any of the above separations followed by ion fragmentation.

19. A method as set forth in claim 18 , wherein generating a pulse with a main pulse generator further comprises an additional second encoding string of start pulses for synchronizing said step of the upfront ion separation; said second string has non equal intervals between pulses; the duration of said second string is comparable to the

Assignees

• Leco Corp

Inventors

• Verenchikov Anatoly N

Classifications

• H01J49/406 Primary

  with multiple reflections · CPC title

• H01J49/0031

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

• H01J49/401 Primary

  characterised by orthogonal acceleration, e.g. focusing or selecting the ions, pusher electrode · CPC title

• H01J49/22

  Electrostatic deflection · CPC title

• H01J49/40 Primary

  Time-of-flight spectrometers (H01J49/36 takes precedence) · CPC title