Mass spectrometer ion trap having asymmetric end cap apertures
An ion trap for a mass spectrometer is disclosed. The ion trap includes a ring electrode and first and second electrodes which are arranged on opposite sides of the ring electrode. The ring electrode and the first and second electrodes are configured to generate an electric field based on the received RF signal. The first electrode defines a first aperture and the second electrode defines a second aperture, the first aperture and the second aperture being asymmetric relative to each other and configured to generate a hexapole field.
1. An ion trap for a mass spectrometer configured to analyze a sample, the ion trap comprising:
a center electrode configured to receive a radio frequency (RF) signal;
first and second end electrodes which are arranged on opposite sides of the center electrode,
wherein the center electrode and the first and second end electrodes are configured to generate, based on the received RF signal, an electric field in an interior space defined by the center electrode, the first end electrode, and the second end electrode, and
wherein the first electrode defines a first aperture to the interior space and the second electrode defines a second aperture to the interior space through which ions are preferentially ejected, wherein a diameter of the first aperture and a diameter of the second aperture are substantially asymmetric, and wherein the first electrode and the second electrode are configured to generate a hexapole field caused by the asymmetry between the first aperture and the second aperture.
2. The ion trap of claim 1 , wherein the diameter of the second aperture is about twice the diameter of the first aperture.
3. The ion trap of claim 1 , wherein the diameter of the second aperture is about four times the diameter of the first aperture.
4. The ion trap of claim 1 , wherein the diameter of the first aperture is about 0.0126″.
5. The ion trap of claim 4 , wherein the diameter of the second aperture is about 0.025″.
6. The ion trap of claim 4 , wherein the diameter of the second aperture is about 0.050″.
7. The ion trap of claim 1 , wherein the dimensions of the first and second apertures are determined based on a desired electric field.
8. The ion trap of claim 7 , wherein a maximum diameter of the second aperture is determined based on a maximum desired hexapole field.
9. The ion trap of claim 7 , wherein a minimum diameter of the second aperture is determined based on a minimum desired hexapole field.
10. A mass spectrometer, comprising:
an ion trap configured to capture ions generated when a sample is ionized by an ion source, the ion trap comprising:
a ring electrode;
first and second end cap electrodes which are arranged on opposite sides of the ring electrode, wherein the first end cap electrode includes a first aperture, and the second end cap electrode includes a second aperture through which ions are discharged from the ion trap, wherein the second aperture has a diameter that is substantially greater than a diameter of the first aperture and sized to induce a hexapole field component of an electric field inside the ion trap; and
an ion detector which detects an amount of the ions discharged from the ion trap.
11. The mass spectrometer of claim 10 , wherein the diameter of the first aperture is about 0.0126 inches.
12. The mass spectrometer of claim 11 , wherein the diameter of the second aperture is about 0.025 inches.
13. The mass spectrometer of claim 11 , wherein the diameter of the second aperture is about 0.050 inches.
14. The mass spectrometer of claim 10 , wherein the diameter of the second aperture is sized so as to substantially reduce the number of electrons from the ion source that impinge an area of the second end cap electrode surrounding the second aperture.
15. The mass spectrometer of claim 10 , wherein RF energy is applied to the ring electrode to generate the electric field in the ion trap, and wherein the dimensions of the first and second apertures are determined based on a desired electric field.
16. The mass spectrometer of claim 15 , wherein a maximum diameter of the second aperture is determined based on a desired contribution of a hexapole field to the electric field.
17. A method of analyzing a sample, the method comprising:
capturing ions in an ion trap of a mass spectrometer, the ion trap comprising:
a ring electrode; and
first and second end cap electrodes which are arranged on opposite sides of the ring electrode, wherein the first end cap electrode includes a first aperture, and the second end cap electrode includes a second aperture through which ions are preferentially discharged from the ion trap, wherein the second aperture has a diameter that is substantially greater than a diameter of the first aperture and sized to induce a hexapole field component of an electric field inside the ion trap;
discharging ions from the ion trap through the second aperture; and
detecting an amount of ions discharged from the ion trap through the second aperture.
18. The method of claim 17 , applying RF energy to the ring electrode to generate an electric field in the ion trap.
19. The method of claim 18 , wherein the electric field inside the ion trap is a quadrupole electric field.
20. The method of claim 17 , wherein the hexapole field component causes ions to eject through the second aperture instead of the first aperture.