Differentially pumped dual linear quadrupole ion trap mass spectrometer
The present disclosure provides a new tandem mass spectrometer and methods of using the same for analyzing charged particles. The differentially pumped dual linear quadrupole ion trap mass spectrometer of the present disclose includes a combination of two linear quadrupole (LQIT) mass spectrometers with differentially pumped vacuum chambers.
1. A mass spectrometry system comprising:
a first linear quadrupole ion trap mass spectrometer in a first vacuum chamber;
a second linear quadrupole ion trap mass spectrometer in a second vacuum chamber, the second linear quadrupole ion trap mass spectrometer configured to analyze the mass-to-charge ratio of a charged particle provided from the first linear quadrupole ion trap mass spectrometer; and
a vacuum manifold operably coupled between the first and second vacuum chambers and configured to allow the charged particle to travel from the first linear quadrupole ion trap mass spectrometer in the first vacuum chamber to the second linear quadrupole ion trap mass spectrometer in the second vacuum chamber.
2. The mass spectrometry system of claim 1 , further comprising an ionization source configured to supply the charged particle to the first linear quadrupole ion trap mass spectrometer.
3. The mass spectrometry system of claim 2 , wherein said ionization source is an atmospheric pressure ionization source.
4. The mass spectrometry system of claim 2 , further comprising:
a first multipole and a first lens configured to direct the charged particle to be received by the first linear quadrupole ion trap mass spectrometer; and
a second multipole and a second lens configured to direct the charged particle to be received by the second linear quadrupole ion trap mass spectrometer.
5. The mass spectrometry system of claim 4 , further comprising an ion introduction multipole positioned between said ionization source and said first multipole.
6. The mass spectrometry system of claim 5 , wherein said first lens is disposed linearly between said ion introduction multipole and said first multipole.
7. The mass spectrometry system of claim 4 , wherein said second lens is disposed linearly between said first linear quadrupole ion trap mass spectrometer and said second multipole.
8. The mass spectrometry system of claim 1 , wherein said first linear quadrupole ion trap mass spectrometer, said vacuum manifold, and said second linear quadrupole ion trap mass spectrometer are arranged linearly.
9. The mass spectrometry system of claim 1 , wherein said first linear quadrupole ion trap mass spectrometer is arranged at an angle to said second linear quadrupole ion trap mass spectrometer.
10. The mass spectrometry system of claim 1 , wherein said vacuum manifold further includes a third multipole, said third multiple being configured to allow ions to travel from the first linear quadrupole ion trap mass spectrometer to the second linear quadrupole ion trap mass spectrometer.
11. The mass spectrometry system of claim 1 , wherein said first linear quadrupole ion trap mass spectrometer is configured for performing a first gas phase ion reaction and said second linear quadrupole ion trap mass spectrometer is configured for performing a second gas phase ion reaction.
12. The mass spectrometry system of claim 11 , wherein said first gas phase ion reaction and said second gas phase ion reaction are selected from the group consisting of collision activated dissociation reactions, ion-molecular interaction, ion-ion reactions, and photon-induced dissociation reactions.
13. The mass spectrometry system of claim 1 , wherein said vacuum manifold contacts said first linear quadrupole ion trap mass spectrometer at a back portion of said first linear quadrupole ion trap mass spectrometer and contacts said second linear quadrupole ion trap mass spectrometer at a front portion of said second linear quadrupole ion trap mass spectrometer.
14. The mass spectrometry system of claim 1 , wherein said ionization source contacts said first linear quadrupole ion trap mass spectrometer at a front portion of said first linear quadrupole ion trap mass spectrometer.
15. The mass spectrometry system of claim 14 further comprising an RF power amplifier.
16. The mass spectrometry system of claim 1 , wherein said mass spectrometry system is configured to utilize a direct current power source.
17. A method of analyzing the mass-to-charge ratio of at least one charged particle including the steps of:
performing a first gas phase ion reaction on a first quantity of particles in a first linear quadrupole ion trap mass spectrometer in a first vacuum chamber;
transferring at least a portion of the first quantity of particles to a second linear quadrupole ion trap mass spectrometer in a second vacuum chamber via a vacuum manifold operably coupled between the first and second vacuum chambers;
performing a second gas phase ion reaction on at least a portion of the first quantity of particles in the second linear quadrupole ion trap mass spectrometer; and
determining with the second linear quadrupole ion trap mass spectrometer the mass-to-charge ratio of at least one of the first quantity of particles.
18. The method of claim 17 , wherein said first gas phase ion reaction and said second gas phase ion reaction are selected from the group consisting of collision activated dissociation reactions, ion-molecular interaction, ion-ion reactions, and photon-induced dissociation reactions.
19. The method of claim 18 , wherein said first linear quadrupole ion trap mass spectrometer includes a first ion trap, said first ion trap having a front section, a center section, a back section, and a back lens, and said transferring step further comprises the steps of:
applying at least one of an RF field and a direct current field to said front, center, and back sections and back lens of said first ion trap;
decreasing the at least one of an RF field and a direct current field in said back section while maintaining the at least one of a RF field and a direct current field to said center and front sections and said back lens higher than said back section; and
decreasing the at least one of an RF field and a direct current field in the back lens.
20. The method of claim 17 , wherein the vacuum manifold contacts the first linear quadrupole ion trap mass spectrometer at a back portion of the first linear quadrupole ion trap mass spectrometer and contacts the second linear quadrupole ion trap mass spectrometer at a front portion of the second linear quadrupole ion trap mass spectrometer.