Dynamic range improvement for isotope ratio mass spectrometry

Patent metadata

Field	Value
Publication number	US-10312071-B2
Application number	US-201615227196-A
Country	US
Kind code	B2
Filing date	Aug 3, 2016
Priority date	Aug 14, 2015
Publication date	Jun 4, 2019
Grant date	Jun 4, 2019

Abstract

In a mass spectrometer, a mass-to-charge dispersive element separates received ions spatially according to their mass-to-charge ratios, to provide a dispersed ion beam thereby. An ion detection arrangement that detects the dispersed ion beam comprises: at least one primary ion detector, each detecting spatially separated ions having mass-to-charge ratios within a respective desired range and each providing a respective main beam signal based on its respective detected ions; and at least one secondary ion detector, each detecting ions having mass-to-charge ratios outside all of the desired ranges simultaneously with the at least one primary ion detector detecting the spatially separated ions and each providing a respective background signal based on its respective detected ions. At least one mass intensity measurement is provided for the received ions having a mass-to-charge ratio within the desired range, based on the at least one main beam signal and the at least one background signal.

First claim

The invention claimed is:

1. A mass spectrometer, comprising:
a mass-to-charge dispersive element, configured to receive ions and separate the ions spatially according to their mass-to-charge ratios, to provide a dispersed ion beam thereby, wherein the mass to charge dispersive element comprises a magnetic sector mass analyzer;
the ion detection arrangement for detecting ions in the dispersed ion beam, including at least one primary ion detector, each arranged to detect spatially separated ions having mass-to-charge ratios within a respective desired range and each configured to provide a respective main beam signal based on its respective detected ions, and at least one secondary ion detector, each arranged to detect ions having mass-to-charge ratios outside all of the desired ranges simultaneously with the at least one primary ion detector detecting the spatially separated ions and each of the at least one secondary ion detectors being configured to provide a respective background signal based on its respective detected ions; and,
a processor, configured to provide at least one mass intensity measurement for the received ions having a mass-to-charge ratio within the desired range, based on the at least one main beam signal and the at least one background signal, wherein the background signal is subtracted from the main beam signal in order to correct the main beam signal.

2. The mass spectrometer of claim 1 , wherein the at least one primary ion detector comprises a plurality of primary ion detectors, each arranged to detect spatially separated ions having mass-to-charge ratios within a respective desired range.

3. The mass spectrometer of claim 2 , wherein the at least one primary ion detector further comprises: a first primary ion detector, arranged to detect spatially separated ions having mass-to-charge ratios within a first desired range; and a second primary ion detector, arranged to detect spatially separated ions having mass-to-charge ratios within a second desired range, the at least one secondary ion detector including a secondary ion detector arranged to detect ions having mass-to-charge ratios in an intermediate range, the intermediate range being between the first and second desired ranges.

4. The mass spectrometer of claim 2 , wherein the plurality of desired ranges define an overall range extending continuously from the lowest mass-to-charge ratio within the desired ranges to the highest mass-to-charge ratio within the desired ranges and wherein the at least one secondary ion detector comprises a secondary ion detector arranged to detect ions having mass-to-charge ratios outside the overall range.

5. The mass spectrometer of claim 2 , wherein each of the desired ranges corresponds with a range of mass-to-charge ratios for an isotope of an element or an isotopologue of a molecule and wherein the at least one secondary ion detector includes a secondary ion detector arranged to detect spatially separated ions having mass-to-charge ratios that do not correspond with a range of mass-to-charge ratios for an isotope of the element or an isotopologue of the molecule.

6. The mass spectrometer of claim 5 , wherein the element comprises uranium, helium or thorium or wherein the molecule comprises carbon dioxide.

7. The mass spectrometer of claim 5 , wherein the processor is configured to determine a first mass intensity measurement, based on the main beam signal provided by a first primary ion detector and the at least one background signal and to determine a second mass intensity measurement, based on the main beam signal provided by a second primary ion detector and the at least one background signal and to determine an isotope ratio based on the first and second mass intensity measurements.

8. The mass spectrometer of claim 2 , wherein the plurality of primary ion detectors are configured to measure ion intensities having a dynamic range of at least 1:100.

9. The mass spectrometer of claim 1 , wherein the processor is configured to provide each of the at least one mass intensity measurement by: determining a respective uncorrected mass intensity measurement on the basis of a main beam signal from the at least one main beam signal; determining a background mass intensity measurement on the basis the at least one background signal; and correcting the uncorrected mass intensity measurement using the background mass intensity measurement.

10. The mass spectrometer of claim 9 , wherein the processor is configured to correct the uncorrected mass intensity measurement by subtracting the background mass intensity measurement, scaled by a factor, from the uncorrected mass intensity measurement.

11. The mass spectrometer of claim 10 , wherein the factor is a constant.

12. The mass spectrometer of claim 1 , wherein the mass-to-charge dispersive element is configured to provide the dispersed ion beam together with scattered background ions, the ion detection arrangement further comprising:
a protection plate, positioned to shield the at least one primary ion detector from at least a portion of the scattered background ions.

13. The mass spectrometer of claim 1 , configured such that ions spatially separated by the mass-to-charge dispersive element are received at each of the at least one primary ion detector without energy filtering in between.

14. The mass spectrometer of claim 1 , wherein each of the at least one primary ion detector and/or each of the at least one secondary ion detector comprises one or more of: a Faraday cup; an ion counting channel; a secondary electron multiplier; a photomultiplier; a compact discrete dynode detector.

15. The mass spectrometer of claim 14 , wherein the at least one primary ion detector comprises a plurality of primary ion detectors, each primary ion detector including a Faraday cup and wherein one or more of the plurality of primary ion detectors is configured to detect a main part of the dispersed ion beam, said one or more of the plurality of primary ion detectors being wider than a remainder of the plurality of primary ion detectors.

16. The mass spectrometer of claim 1 , further comprising:
an ion source, configured to generate ions; and
ion optics, configured to provide the generated ions to the mass-to-charge dispersive element.

17. A method of mass spectrometry, comprising:
spatially separating received ions according to their mass-to-charge ratios using a mass-to-charge dispersive element, to provide a dispersed ion beam thereby, wherein the mass to charge dispersive element comprises a magnetic sector mass analyzer;
detecting, at each of at least one primary ion detector, spatially separated ions having mass-to-charge ratios within a respective desired range and providing a respective main beam signal based on the respective detected ions;
detecting, at each of at least one secondary ion detector, ions having mass-to-charge ratios outside all of the desired ranges, simultaneously with the at least one primary ion detector, and providing at each of at least one secondary ion detector a respective background signal based on the respective detected ions; and,
providing at least one mass intensity measurement for the received ions having a mass-to-charge ratio within the desired range, based on the at least one main beam signal and the at least one background signal, wherein the background signal is subtracted from the main beam signal in order to correct the main beam signal.

18. The method of claim 17 , wherein the at least one primary ion detector detects a high ion intensity relative to the ion intensity detected by

Assignees

• Thermo Fisher Scient Bremen Gmbh

Inventors

• Radke Jens
• Hilkert Andreas
• Trinquier Anne
• Schwieters Johannes

Classifications

• B01D59/44

  Separation by mass spectrography (particle spectrometers or separator tubes H01J49/00) · CPC title

• G01N27/62 Primary

  by investigating the ionisation of gases, e.g. aerosols; by investigating electric discharges, e.g. emission of cathode · CPC title

• H01J49/30 Primary

  using magnetic analysers {, e.g. Dempster spectrometer} · CPC title

• H01J49/0036

  Step by step routines describing the handling of the data generated during a measurement · CPC title

• H01J49/009 Primary

  Spectrometers having multiple channels, parallel analysis · CPC title