Abstract: A method for parallel accumulation and serial fragmentation of ions, wherein ions are injected into a device capable of serial ejection using a pseudopotential barrier created by an RF voltage. In all instances, the ions may be filtered prior to accumulation in the device capable of serial ejection. In some cases this filtering may take the form of discrete isolation windows using isolation waveforms with multiple notches. In some cases these waveforms may be applied to a quadrupole mass filter. Following accumulation of the precursor ions, the initial population may be serially ejected using a pseudopotential barrier created by an RF voltage. Following serial ejection, the individual precursor ion populations are analyzed. In some cases, this analysis might involve additional rounds of ion isolation and manipulation (e.g., MSn, CID, ETD, etc.).

Abstract: A method for parallel accumulation and serial fragmentation of ions, wherein ions are injected into a device capable of serial ejection using a pseudopotential barrier created by an RF voltage. In all instances, the ions may be filtered prior to accumulation in the device capable of serial ejection. In some cases this filtering may take the form of discrete isolation windows using isolation waveforms with multiple notches. In some cases these waveforms may be applied to a quadrupole mass filter. Following accumulation of the precursor ions, the initial population may be serially ejected using a pseudopotential barrier created by an RF voltage. Following serial ejection, the individual precursor ion populations are analyzed. In some cases, this analysis might involve additional rounds of ion isolation and manipulation (e.g., MSn, CID, ETD, etc.).

Abstract: A method of operating an electrostatic trapping mass analyzer, comprising: introducing a sample of ions into a trapping region of the mass analyzer, wherein a trapping field within the trapping region is such that the ions exhibit radial motion with respect to a central longitudinal axis of the trapping region while undergoing harmonic motion in a dimension defined by the central longitudinal axis, the frequency of harmonic motion of a particular ion being a function of its mass-to-charge ratio; superimposing a modulation field onto the trapping field within the trapping region, the modulation field acting to either increase or reduce the harmonic motion energies of the ions by an amount varying according to the frequency of harmonic motion; and acquiring a mass spectrum of the ions in the trapping region by measuring a signal representative of an image current induced by the harmonic motion of the ions.

Abstract: A method is described that involves simplification of UVPD mass spectra and comprises selecting precursor ions for UVPD fragmentation, performing UVPD fragmentation on selected precursor ions to give UVPD fragment ions. PTR may then be performed on the UVPD fragment ions with optional ion parking to yield charge-state reduced UVPD fragment ions. The UVPD-PTR steps may be repeated above n times where n=1 to 50. Ion parking may enhance the intensity of selected lower fragment ion charge states or to increase the intensity of peaks in selected m/z ranges. After a number of PTR-UVPD iterations, fragment ions are mass analyzed. The method provides a way of simplifying UVPD mass spectral product ions by lowering fragment ion charge states and spreading out resulting product ions in m/z mass spectral space when compared to using UVPD fragmentation alone.

Abstract: A method of operating an electrostatic trapping mass analyzer, comprising: introducing a sample of ions into a trapping region of the mass analyzer, wherein a trapping field within the trapping region is such that the ions exhibit radial motion with respect to a central longitudinal axis of the trapping region while undergoing harmonic motion in a dimension defined by the central longitudinal axis, the frequency of harmonic motion of a particular ion being a function of its mass-to-charge ratio; superimposing a modulation field onto the trapping field within the trapping region, the modulation field acting to either increase or reduce the harmonic motion energies of the ions by an amount varying according to the frequency of harmonic motion; and acquiring a mass spectrum of the ions in the trapping region by measuring a signal representative of an image current induced by the harmonic motion of the ions.

Abstract: A method of operating an electrostatic trapping mass analyzer, comprising: introducing a sample of ions into a trapping region of the mass analyzer, wherein a trapping field within the trapping region is such that the ions exhibit radial motion with respect to a central longitudinal axis of the trapping region while undergoing harmonic motion in a dimension defined by the central longitudinal axis, the frequency of harmonic motion of a particular ion being a function of its mass-to-charge ratio; superimposing a modulation field onto the trapping field within the trapping region, the modulation field acting to either increase or reduce the harmonic motion energies of the ions by an amount varying according to the frequency of harmonic motion; and acquiring a mass spectrum of the ions in the trapping region by measuring a signal representative of an image current induced by the harmonic motion of the ions.

Abstract: A method is described that involves simplification of UVPD mass spectra and comprises selecting precursor ions for UVPD fragmentation, performing UVPD fragmentation on selected precursor ions to give UVPD fragment ions. PTR may then be performed on the UVPD fragment ions with optional ion parking to yield charge-state reduced UVPD fragment ions. The UVPD-PTR steps may be repeated above n times where n=1 to 50. Ion parking may enhance the intensity of selected lower fragment ion charge states or to increase the intensity of peaks in selected m/z ranges. After a number of PTR-UVPD iterations, fragment ions are mass analyzed. The method provides a way of simplifying UVPD mass spectral product ions by lowering fragment ion charge states and spreading out resulting product ions in m/z mass spectral space when compared to using UVPD fragmentation alone.

Abstract: A method is described that produces product ions for mass analysis, the method comprising the steps of: introducing precursor ions into an RF electric field ion containment device, introducing reagent ions into the RF electric field ion containment device and performing an ion-ion interaction in the RF electric field ion containment device by co-trapping the precursor ions with the reagent ions. Precursor ions and product ions may be retained and/or isolated in the RF electric field ion containment device. The steps above may be repeated until a predetermined amount of reaction completeness is attained. Mass analysis of at least some of the ions in the RF electric field ion containment device may be performed where the ions are mass analyzed either directly from the RF electric field ion containment device.

Abstract: A method of operating an electrostatic trapping mass analyzer, comprising: introducing a sample of ions into a trapping region of the mass analyzer, wherein a trapping field within the trapping region is such that the ions exhibit radial motion with respect to a central longitudinal axis of the trapping region while undergoing harmonic motion in a dimension defined by the central longitudinal axis, the frequency of harmonic motion of a particular ion being a function of its mass-to-charge ratio; superimposing a modulation field onto the trapping field within the trapping region, the modulation field acting to either increase or reduce the harmonic motion energies of the ions by an amount varying according to the frequency of harmonic motion; and acquiring a mass spectrum of the ions in the trapping region by measuring a signal representative of an image current induced by the harmonic motion of the ions.

Abstract: A method is described that produces product ions for mass analysis, the method comprising the steps of: introducing precursor ions into an RF electric field ion containment device, introducing reagent ions into the RF electric field ion containment device and performing an ion-ion interaction in the RF electric field ion containment device by co-trapping the precursor ions with the reagent ions. Precursor ions and product ions may be retained and/or isolated in the RF electric field ion containment device. The steps above may be repeated until a predetermined amount of reaction completeness is attained. Mass analysis of at least some of the ions in the RF electric field ion containment device may be performed where the ions are mass analyzed either directly from the RF electric field ion containment device.

Abstract: 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.

Abstract: A method and apparatus are disclosed for dissociation of precursor ions, such as polypeptides, by ultraviolet photodissociation (UVPD) for mass spectrometry analysis. Precursor ions are confined within an ion trap and irradiated with ultraviolet (UV) light, which may take the form of pulses emitted by a laser. The precursor ions absorb the UV light and dissociate into product ions. To avoid the condition of overfragmentation arising from further dissociation of the product ions, an excitation field is established within the ion trap such that the product ions, but not the precursor ions, are kinetically excited to trajectories that extend outside of the irradiated region.