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Electrospray ionization interface to high pressure mass spectrometry and related methods

專利號(hào)
US10867781B2
公開(kāi)日期
2020-12-15
申請(qǐng)人
The University of North Carolina at Chapel Hill(US NC Chapel Hill)
發(fā)明人
John Michael Ramsey; William McKay Gilliland, Jr.
IPC分類
H01J49/16; H01J49/24; H01J49/00; H01J49/04; B01L3/00
技術(shù)領(lǐng)域
mass,esi,analyzer,about,mm,inlet,chamber,ion,vacuum,trap
地域: NC NC Chapel Hill

摘要

An electrospray ionization (ESI)-mass spectrometer analysis systems include an ESI device with at least one emitter configured to electrospray ions and a mass spectrometer in fluid communication with the at least one emitter of the ESI device. The mass spectrometer includes a mass analyzer held in a vacuum chamber. The vacuum chamber is configured to have a high (background/gas) pressure of about 50 mTorr or greater during operation. During operation, the ESI device is configured to either; (a) electrospray ions into a spatial region external to the vacuum chamber and at atmospheric pressure, the spatial extent being adjacent to an inlet device attached to the vacuum chamber, the inlet device intakes the electrosprayed ions external to the vacuum chamber with the mass analyzer and discharges the ions into the vacuum chamber with the mass analyzer; or (b) electrospray ions directly into the vacuum chamber with the mass analyzer.

說(shuō)明書(shū)

The terms “miniature cylindrical ion trap”, “miniature CIT” and “mini-CIT” refer to a cylindrical ion trap “CIT” with a critical dimension that is in the millimeter to submillimeter range, typically with associated apertures in one or more electrodes of the ion trap having a critical dimension between about 0.001 mm to about 5 mm, and any sub-range thereof. The ion trap electrode central aperture can take on different geometries such as a cylindrical or slit shaped void and arrays of voids are possible.

The term “microfluidic chip” is used interchangeably with “microchip” and refers to a fluidic sample processing device with sub-millimeter sized fluidic channels with at least one integrated emitter for processing samples.

Mass spectrometry has historically been performed under conditions of high vacuum. The reason for this condition is that performance is enhanced if ions do not collide with background gas molecules during their trajectory from an ion source through a mass analyzer arriving at a detector. Ion-molecule collision events scatter the ions away from their intended trajectory, often degrading mass resolution and signal strength. The vacuum that achieves sufficient resolution in conventional systems can be formalized through the Knudsen number, Kn. Mass spectrometry is typically performed in the molecular flow regime defined as Kn>1, and in conventional practice, Kn is between about 100 and over 10,000 for mass analyzers of mass spectrometers.

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