Identification of sample subspecies based on particle charge behavior under structural change-inducing sample conditions
US-2024242955-A1 · Jul 18, 2024 · US
US9202680B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9202680-B2 |
| Application number | US-201013376132-A |
| Country | US |
| Kind code | B2 |
| Filing date | Jun 3, 2010 |
| Priority date | Jun 3, 2009 |
| Publication date | Dec 1, 2015 |
| Grant date | Dec 1, 2015 |
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Disclosed herein are systems and methods for mass spectrometry using laserspray ionization (LSI). LSI can create multiply-charged ions at atmospheric pressure for analysis and allows for analysis of high molecular weight molecules including molecules over 4000 Daltons. The analysis can be solvent-based or solvent-free. Solvent-free analysis following LSI allows for improved spatial resolution beneficial in surface and/or tissue imaging.
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What is claimed is: 1. A method for producing predominantly multiply-charged ions for analysis of a material consisting of, applying the material and a matrix to a surface as a material/matrix analyte; ablating the material/matrix analyte at or near atmospheric pressure with a laser; and passing the laser-ablated material/matrix analyte through a heated region before the material/matrix analyte enters the high vacuum area of a mass spectrometer thereby producing predominantly multiply-charged ions. 2. The method of claim 1 , wherein the matrix is composed of small molecules that absorb energy at the laser's wavelength. 3. The method of claim 2 , wherein the small molecules are selected from the group consisting of a dihydroxybenzoic acid, 2,5-dihydroxybenzoic acid (2,5-DHB); a dihydroxyacetophenones, 2,5-dihydroxyacetophenone (2,5-DHAP), 2,6-dihydroxyacetophenone (2,6-DHAP), 2-aminobenzyl alcohol (2-ABA) and combinations thereof. 4. The method of claim 1 , wherein the laser has an output in the ultraviolet region. 5. The method of claim 1 , wherein the laser is a nitrogen laser (337 nm) or a frequency tripled Nd/YAG laser (355 nm). 6. The method of claim 1 , wherein the heated region is a heated tube. 7. The method of claim 6 , wherein the tube is constructed of heat-tolerant material that does not emit vapors detrimental to the mass spectrometer vacuum system. 8. The method of claim 7 , wherein the tube is constructed of metal or quartz. 9. The method of claim 6 , wherein the tube is heated to a temperature between 50-600° C. 10. The method of claim 6 , wherein the tube is heated to a temperature between 150-450° C. 11. The method of claim 1 , wherein an electric field in an ion source region defined by the point of laser ablation of the material/matrix analyte and the ion entrance to the vacuum of the mass spectrometer is less than 800 V. 12. The method of claim 11 , wherein the electric field in the ion source region is less than 100 V. 13. The method of claim 11 , wherein the electric field in the ion source region is 0 V. 14. The method of claim 1 , wherein the material is a biological material or a non-biological material. 15. The method of claim 14 wherein the material is a biological material selected from the group consisting of a protein, a peptide, a carbohydrate, and a lipid. 16. The method of claim 14 wherein the material is a non-biological material selected from the group consisting of a polymer and an oil. 17. A system for carrying out the methods of claim 1 . 18. The method of claim 1 wherein the laser is aligned in transmission geometry or reflection geometry. 19. The method of claim 1 wherein no electric field is required to produce the predominantly multiply-charged ions. 20. A method for producing predominantly multiply-charged ions for analysis of a material comprising, applying the material and a matrix to a surface as a material/matrix analyte; ablating the material/matrix analyte at or near atmospheric pressure with a laser; and passing the laser-ablated material/matrix analyte through a heated region before the material/matrix analyte enters the high vacuum area of a mass spectrometer thereby producing predominantly multiply-charged ions wherein no electric field is required to produce the predominantly multiply-charged ions. 21. The method of claim 20 further comprising analyzing the material/matrix analyte using solvent-free material/matrix analyte preparation methods. 22. The method of claim 21 wherein the analyzing includes surface imaging and/or MS/MS fragmentation for structural characterization. 23. The method of claim 20 further comprising separating and analyzing the predominantly multiply-charged ions using ion mobility spectrometry. 24. The method of claim 20 further comprising fragmenting and characterizing the predominantly multiply-charged ions using MS/MS fragmentation selected from collision induced dissociation fragmentation, charge remote fragmentation, electron transfer dissociation fragmentation or electron capture dissociation fragmentation. 25. The method of claim 22 wherein the laser is aligned in transmission geometry or reflection geometry. 26. The method of claim 23 wherein the separating and analyzing includes surface imaging. 27. The method of claim 20 wherein no electric field is used to produce the predominantly multiply-charged ions. 28. The method of claim 20 wherein the electric field in an ion source region defined by the point of laser ablation of the material/matrix analyte and the ion entrance to the vacuum of the mass spectrometer is 0 V.
using photo-ionisation, e.g. using laser beam · CPC title
with means for heating or cooling the sample · CPC title
Laser desorption/ionisation, e.g. matrix-assisted laser desorption/ionisation [MALDI] (sample holders H01J49/0418) · CPC title
with means for preventing droplets from entering the analyzer; Desolvation of droplets · CPC title
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