Time-of-flight mass spectrometer combining fields non-linear in time and space
A time-of-flight mass spectrometer which has an iron source, an evacuated tube proximate the ion source and adapted to receive ions from the ion source, and a detector disposed at an end of the evacuated tube opposite an end proximate the ion source. The ion source is constructed to generate an electric field that changes non-linearly as a function of position along a path from the ion source to the detector. The ion source is constructed to generate an electric field that changes as a function of time, the electric field being provided to accelerate ions from the ion source to the detector.
1. A time-of-flight mass spectrometer, comprising:
an ion source;
an evacuated tube proximate said ion source and adapted to receive ions from said ion source;
a detector disposed at an end of said evacuated tube opposite an end proximate said ion source;
an electrode having a substantially cylindrical shape and orthogonally positioned between said ion source and said detector;
wherein said mass spectrometer is constructed to generate an electric field that changes non-linearly as a function of position along substantially an entire path from said ion source to said detector, and
wherein said mass spectrometer is constructed to generate an electric field that changes as a function of time, said electric field being provided to continuously accelerate the ions from said ion source to said detector.
2. A time-of-flight mass spectrometer according to claim 1 , wherein a magnitude of a spatial distribution of said electric field changes as a function of time.
3. A time-of-flight mass spectrometer according to claim 1 , wherein a shape of a spatial distribution of said electric field changes as a function of time.
4. A time-of-flight mass spectrometer according to claim 1 , further comprising an ion mirror arranged in an ion path from said ion source and in an ion path to said detector,
wherein said ion mirror is constructed to generate an electric field that changes as a function of position along said path from the entrance of said ion mirror to said detector, and
wherein said ion mirror is constructed to generate an electric field that changes as a function of time, said electric field generated by said ion mirror being provided to focus ions from said ion source on said detector.
5. A time-of-flight mass spectrometer according to claim 4 , wherein a magnitude of a spatial distribution of said electric field generated by said ion mirror changes as a function of time.
6. A time-of-flight mass spectrometer according to claim 4 , wherein a shape of a spatial distribution of said electric field generated by said ion mirror changes as a function of time.
7. A time-of-flight mass spectrometer according to claim 4 , wherein said electric field generated by said ion mirror changes linearly as a function of position along said path from said ion source to said detector.
8. A time-of-flight mass spectrometer according to claim 4 , wherein said electric field generated by said ion mirror changes non-linearly as a function of position along said path from said ion source to said detector.
9. A time-of-flight mass spectrometer according to claim 1 , wherein said ion source further provides a delay pulse to allow for the dissipation of neutral molecules and free-radical chemical species.
10. A time-of-flight mass spectrometer according to claim 1 , wherein said ion source further provides a short-duration, high-amplitude voltage pulse prior to ion ejection from the source in order to bias an initial energy distribution of an ion population.
11. A time-of-flight mass spectrometer, comprising:
an ion source;
an evacuated tube proximate said ion source and adapted to receive ions from said ion source;
a detector disposed at an end of said evacuated tube opposite an end proximate said ion source;
an electrode having a substantially cylindrical shape and orthogonally positioned between said ion source and said detector; and
an ion mirror arranged in an ion path from said ion source and in an ion path to said detector,
wherein said ion mirror is constructed to generate an electric field that changes nonlinearly as a function of position along said path from the entrance of said ion source to said detector, and
wherein said ion mirror is constructed to generate an electric field that changes as a function of time, said electric field being provided to focus ions from said ion source on said detector.
12. A time-of-flight mass spectrometer according to claim 11 , wherein a magnitude of a spatial distribution of said electric field generated by said ion mirror changes as a function of time.
13. A time-of-flight mass spectrometer according to claim 11 , wherein a shape of a spatial distribution of said electric field generated by said ion mirror changes as a function of time.
14. A time-of-flight mass spectrometer according to claim 11 , wherein said electric field generated by said ion mirror changes linearly as a function of position along said path from said ion source to said detector.
15. A time-of-flight mass spectrometer according to claim 11 , wherein said electric field generated by said ion mirror changes non-linearly as a function of position along said path from said ion source to said detector.
16. A time-of-flight mass spectrometer according to claim 11 , wherein said ion source further provides a delay pulse to allow for the dissipation of neutral molecules and free-radical chemical species.
17. A time-of-flight mass spectrometer according to claim 11 , wherein said ion source further provides a short-duration, high-amplitude voltage pulse prior to ion ejection from the source in order to bias an initial energy distribution of an ion population.
18. A method of measuring the mass-to-charge ratio of an ion, comprising:
arranging an ion source;
arranging an evacuated tube proximate said ion source and adapted to receive ions from said ion source;
arranging a detector disposed at an end of said evacuated tube opposite an end proximate said ion source;
arranging an electrode having a substantially cylindrical shape and orthogonally positioned between said ion source and said detector;
generating an electric field between the ion source and the detector that changes non-linearly as a function of position along substantially an entire path from said ion source to said detector and that changes as a function of time;
accelerating an ion continuously from a source to a detector;
detecting said ion; and
determining a time-of-flight of said ion.
19. A method of measuring the mass-to-charge ratio of an ion according to claim 18 , further comprising focusing said ion on a detector using an ion mirror that produces an electric field that is both spatially and temporally non-constant.