Abstract:
Two-channel electrical and photo-electrical TOF ion detection systems are provided. These systems maintain the resolution and dynamic range advantages of four-channel systems but at a lower cost. Electrodes or light pipes are configured to direct electrons or photons produced by ion impacts into two separate channels. The first channel receives electrons or photons resulting from the inner or central part of the rectangular pattern of each ion impact. The second channel receives electrons or photons resulting from the two outer ends of the rectangular pattern of each ion impact. In a two-channel digitizer, the first channel and the second channel are independently calibrated to align the first digital value and the second digital value in time and account for the convex shape of the ion impacts of each ion packet and/or the curvature of a microchannel plate.
Abstract:
In a first location of a mass spectrometer, a plurality of ionized molecules of an ion source are selected that have mass-to-charge ratios within a mass-to-charge ratio window width. The plurality of selected ionized molecules are transmitted from a first to a second location. Reagent ions are transmitted to the second location to reduce a charge state of one or more of the plurality of selected ionized molecules. A mass analyzer is used to analyze the plurality of reduced ionized molecules and produce a mass spectrum. A compound is identified from a peak of the spectrum that has a mass-to-charge ratio less than or equal to the highest mass-to-charge ratio in the window width if the noise is multiply charged and greater than the highest mass-to-charge ratio in the window width if the noise is singly charged.
Abstract:
Systems and methods are disclosed for dynamically switching an ion guide and a TOF mass analyzer between concentrating or not concentrating ions in a targeted acquisition. Product ions are ejected from the ion guide into the TOF mass analyzer and the intensity of a known product ion is measured at two or more time steps. The ion guide initially ejects product ions using a sequential or Zeno pulsing mode that concentrates product ions with different m/z values within the TOF mass analyzer at the same time. If the intensity of the product ion is increasing and greater than a threshold intensity, the ion guide switches to a continuous or normal pulsing mode that does not concentrate ions with different m/z values in the TOF mass analyzer at the same time. Similarly, if the intensity decreases below a threshold in continuous mode, the ion guide switches back to sequential mode.
Abstract:
During an accumulation time period of each time cycle of an ion guide and before a ramped AC voltage is applied to at least one set of axial rods to eject ions according to m/z value, a number of steps are performed. Ions are received from outside of the ion guide through an entrance aperture and into a first cell. A low DC voltage is applied to a barrier electrode to receive ions from the first cell into a second cell. And, a high DC voltage is applied to an exit electrode to prevent ions from exiting the ion guide. During a cooling time period before the AC time period, a high DC voltage is applied to the barrier electrode to trap and cool ions in the second cell and to continue to receive ions into the first cell without being affected by the ramped AC voltage.
Abstract:
Two-channel electrical and photo-electrical TOF ion detection systems are provided. These systems maintain the resolution and dynamic range advantages of four-channel systems but at a lower cost. Electrodes or light pipes are configured to direct electrons or photons produced by ion impacts into two separate channels. The first channel receives electrons or photons resulting from the inner or central part of the rectangular pattern of each ion impact. The second channel receives electrons or photons resulting from the two outer ends of the rectangular pattern of each ion impact. In a two-channel digitizer, the first channel and the second channel are independently calibrated to align the first digital value and the second digital value in time and account for the convex shape of the ion impacts of each ion packet and/or the curvature of a microchannel plate.
Abstract:
Systems and methods are provided for calculating and storing an average amplitude response for each peak of a mass spectrum during data acquisition. A mass analyzer is instructed to analyze N extractions of an ion beam, producing N sub-spectra. For each sub-spectrum of the N sub-spectra, a nonzero amplitude from an ADC detector subsystem is counted as one ion, producing a count of one for each ion. The ADC amplitudes and counts of the N sub-spectra are summed, producing a spectrum that includes a summed ADC amplitude and a total count for each ion. For each ion of the spectrum, an estimated ion count is calculated from a Poisson distribution of the total count of each ion for the N sub-spectra. For each ion of the spectrum, an average amplitude response is calculated by dividing the summed amplitude by the estimated ion count and stored.
Abstract:
In a first location of a mass spectrometer, a plurality of ionized molecules of an ion source are selected that have mass-to-charge ratios within a mass-to-charge ratio window width. The plurality of selected ionized molecules are transmitted from a first to a second location. Reagent ions are transmitted to the second location to reduce a charge state of one or more of the plurality of selected ionized molecules. A mass analyzer is used to analyze the plurality of reduced ionized molecules and produce a mass spectrum. A compound is identified from a peak of the spectrum that has a mass-to-charge ratio less than or equal to the highest mass-to-charge ratio in the window width if the noise is multiply charged and greater than the highest mass-to-charge ratio in the window width if the noise is singly charged.