Thermo Finnigan LLC

Finnigan Corporation

University of Texas System

Thermo Fisher Scientific (bremen) Gmbh

Thermo Finnegan LLC

Thermo Funnigan LLC

Coon, Joshua J.

Jae C Schwartz

Michael W Senko

Philip M Remes

Alexander Alekseevich Makarov

John E P Syka

Scott T Quarmby

Mark E Hardman

Linfan Li

Alexander Makarov

Viatcheslav V Kovtoun

John N Louris

Oleg Silivra

Berg A Tehlirian

John E Syka

Joshua J Coon

Eloy R Wouters

Michael William Belford

Jens Griep-Raming

Jean-Jacques Dunyach

Maurizio Splendore

Christopher Mullen

Mark E Bier

John Edward Philip Syka

Dennis M Taylor

John Glazier

Chad R Weisbrod

Yevgeniy N Zhuk

Mark M Okamura

Dustin D Holden

Jennifer S Brodbelt

Andreas F R Huhmer

Xaio-Guang Zhou

John Ep Syka

John EP Syka

Andreas Fr Huhmer

A method of ion detection comprises: (a) setting electrical potentials of a dynode and a scintillator electrode of a Daly detector and of a focusing lens disposed at an ion inlet of the Daly detector so as to detect negatively charged ions received from a mass analyzer or mass filter; (b) transferring the negatively charged ions from the mass analyzer or mass filter to the Daly detector through the lens and detecting said negatively charged ions by a photodetector of the Daly detector; (c) setting electrical potentials of the dynode, the scintillator electrode and the focusing lens of the Daly detector so as to detect positively charged ions received from the mass analyzer or mass filter; and (d) transferring the positively charged ions from the mass analyzer or mass filter to the Daly detector through the lens and detecting said positively charged ions by the photodetector.

Daly detector operable in negative ion and positive ion detection modes

An ion detector that can detect either positive or negative ions comprises: an ion inlet comprising an ion focusing lens; a dynode having a surface configured to intercept, within a zone of interception, a stream of ions passing through the ion focusing lens, wherein a plane that is tangent to the dynode surface at the zone of interception is disposed at an angle to a line that passes through the center of the dynode surface and the center of the focusing lens; a scintillator having a surface that is configured to receive secondary electrons emitted from the zone of interception; a scintillator electrode affixed to the scintillator surface; a photodetector configured to receive photons emitted by the scintillator and to generate an electric signal in response thereto; and one or more power supplies electrically coupled to the focusing lens, the dynode, the scintillator electrode and the photodetector.

A mass spectrometer system comprises: (a) an ion source; (b) a mass filter or a time-of-flight (TOF) ion separator configured to receive a stream of first-generation ions from the ion source; (c) an ion storage device having an ion inlet configured to receive a stream of filtered ions comprising a plurality of ion species from the mass filter or TOF separator and to accumulate the plurality of ion species therein; (d) an ion mobility cell having an ion inlet configured to receive an accumulated batch of ion species from the ion storage device and an ion outlet configured to release, one at a time, the individual ion species therefrom; and (e) a mass analyzer configured to receive and mass analyze each first-generation ion species or each fragment ion species generated by fragmentation or other reaction of the various first-generation ion species.

Methods and apparatus for high speed mass spectrometry

Systems, methods, and devices to dissociate ions using one or more light emitting diodes (LEDs). A mass spectrometer for ion dissociation includes an ion source for providing ions for dissociation, a mass analyzer, and a photodissociation (PD) device. The PD device includes an ion transport device. The ion transport device is configured perform one or more of: transporting the ions through the PD device, and trapping the ions within a region of the PD device. The PD device also includes one or more LEDs positioned to irradiate the ions in the PD device, resulting in fragmentation of the ions.

Devices, systems, and methods for dissociation of ions using light emitting diodes

A system includes an optical measurement unit that measures an optical property of a whole blood sample deposited on a surface of a substrate, an ion source that causes ions derived from the whole blood sample, including ions formed from an analyte of interest present in the whole blood sample, to be emitted from the substrate, a mass analyzer that receives the ions emitted from the substrate and measures an abundance of at least one ion species corresponding to the analyte of interest, and at least one computing device that determines, based on the measured optical property, a hematocrit of the whole blood sample, and determines, based on the determined hematocrit of the whole blood sample and the measured abundance of the at least one ion species, a concentration of the analyte of interest per unit volume of blood plasma.

Blood sample analysis systems and methods

A method of quantitative mass analysis of precursor ion species of different mass-to-charge (m/z) ratios from the same or common ion injection event is disclosed. A plurality of precursor ion species with different respective m/z ratios are introduced into an ion trap mass analyzer at the same time. The precursor ion species are isolated. A first subset of the isolated precursor ions, which are multiply charged and have a first m/z ratio range, is fragmented and scanned by dividing the scan into at least two separate scan windows. A first mass spectrum is generated for the fragment ions of the first subset of precursor ions. A second subset of the isolated precursor ions having a second m/z ratio is fragmented and scanned, and a second mass spectrum is generated for the fragment ions of the second subset of precursor ions.

Methods and systems for quantitative mass analysis

A mass spectrometry apparatus includes an ion source, an ion trap and a mass spectrometer controller. The ion source is configured to generating ions. The ion trap is configured to trap ions within a RF field; eject unwanted ion while retaining target ions; and fragment target ions. The mass spectrometer controller is configured to determine an injection time for the ion trap based on a precursor ion flux and a product ion flux; fill the ion trap with ions from the ion source for an amount of time equal to the injection time; isolate target precursor ions in the ion trap; fragment the target precursor ions to generate product ions; and mass analyzing the product ions.

[object Object]

A mass spectrometer includes a radio frequency ion trap and a controller. The controller is configured to cause an ion population to be injected into the radio frequency ion trap and supply an isolation waveform to the radio frequency ion trap. The isolation waveform has at least one notch at a target mass-to-charge ratio and a frequency profile determined to eject unwanted ions at a plurality of frequencies in a substantially similar amount of time.

Systems and methods for ion isolation

Techniques can increase the resolution and accuracy of mass spectra obtained using ion traps through the use of the actual shape of the ion trap peaks, which is a series of smaller ion ejection events. The peak shapes are identified as changing over a common period of the trapping signal and the excitation signal, at which point the peak shapes repeat. Peak shapes can be characterized over the common period to create N basis functions, each for a different fractional mass for a given scan rate. The N basis functions over the common period can be duplicated (e.g., shifted by the common period) to obtain a set of mass functions that characterize fractional masses over the full scan range. The mass spectrum can be obtained by fitting the set of mass functions to the measured data to obtain a best fit contribution of each mass function to the measured data.

High-resolution ion trap mass spectrometer

A mass spectrometer includes a radio frequency ion trap; and a controller. The controller is configured to cause an ion population to be injected into the radio frequency ion trap; supply a first isolation waveform to the radio frequency ion trap for a first duration, and supply a second isolation waveform to the radio frequency ion trap for a second duration. The first isolation waveform has at least a first wide notch at a first mass-to-charge ratio, and the second isolation waveform has at least a first narrow notch at the first mass-to-charge ratio. The first and second isolation waveforms are effective to isolate one or more precursor ions from the ion population.

Systems and methods for ion isolation using a dual waveform

A method of aligning a light beam within a mass spectrometer includes providing precursor ions along a longitudinal axis of the mass spectrometer at two or more precursor ion locations, the precursor ion locations being spatially separated along the longitudinal axis of the mass spectrometer, the precursor ions forming in-vacuum targets. The method then includes directing a light beam from a light source in a direction along the longitudinal axis of the mass spectrometer, the light beam photo-dissociating the precursor ions, and monitoring a mass spectrometer ion signal from each of the two or more precursor ion locations while adjusting the direction of the light beam, thereby aligning the light beam within the mass spectrometer.

Photo-dissociation beam alignment method

A method is described for identifying the occurrence and location of charging of ion optic devices arranged along the ion path of a mass spectrometer. The method includes repeatedly performing a sequence of introducing a beam of discharge ions to a location on the ion path, and subsequently measuring the intensities of opposite-polarity sample ions delivered to a mass analyzer, with the discharge ions being delivered to a location further downstream in the ion path at each successive sequence.

Identifying the occurrence and location of charging in the ion path of a mass spectrometer

An apparatus for a mass spectrometer comprises: a set of four rod electrodes defining an ion occupation volume therebetween having entrance and exit ends, at least one of the rod electrodes having a slot passing therethrough; first and second ion optics disposed adjacent to the entrance and exit ends, respectively; a voltage supply system; and at least one supplemental electrode disposed at least partially within the at least one slot, wherein the voltage supply system is configured so as to supply a radio-frequency (RF) voltage, a direct-current (DC) filtering voltage and an oscillatory dipole resonant ejection voltage across members of the set of rod electrodes and so at to supply a secondary ion-trapping RF voltage and a secondary DC filtering voltage to the at least one supplemental electrode and to supply DC voltages across the rod electrodes and each of the first and second ion optics.

Method and apparatus for a combined linear ion trap and quadrupole mass filter

Methods for operating a mass spectrometer having at least one component having mass-dependent transmission, comprising: injecting a first sample of ions having a first mass range into an ion accumulator for a first injection time under first operating conditions suitable for optimizing transmission of ions of the first range; acquiring a full-scan mass spectrum of the first sample of ions; selecting ion species having a second mass range different than the first range; calculating a second injection time, the second injection time suitable for injecting a population of the selected ion species into the ion accumulator under second operating conditions suitable for optimizing transmission of ions of the second range; injecting a second sample of ions having the selected ion species into the ion accumulator for the second injection time under the second operating conditions; and acquiring a mass spectrum of ions derived from the selected ion species.

Ion population control in a mass spectrometer having mass-selective transfer optics

A two-dimensional radial-ejection ion trap is constructed from four apertured electrodes having inwardly facing hyperbolic surfaces, with each electrode being spaced from the centerline by a distance r that is greater than the hyperbolic radius rdefined by the hyperbolic surfaces. This geometry produces a balanced symmetrical trapping field that has a negligible octopole field component and a relatively large dodecapole or icosapolar field component. In one specific implementation, the ion trap is selectably operable as a quadrupole mass filter by applying a filtering DC voltage to the electrodes.

Growing community of inventors

San Jose, CA, United States of America

Jae C Schwartz