The present disclosure proposes a mass spectrometer including a linear ion trap section and an analyzer that analyzes the ions ejected from the linear ion trap section having a multipole rod electrode including a plurality of segments arranged in a direction of a center axis of the linear ion trap section. A first radio frequency voltage in opposite phase is applied to adjacent rod electrodes. An electrostatic voltage having the same amplitude and a second radio frequency voltage are applied to the segments having the same position in the direction of the center axis. The electrostatic voltage is applied to the segments such that the electrostatic voltage decreases from an inlet to an outlet of the linear ion trap section. The second radio frequency voltage is applied to the segments such that the second radio frequency voltage increases from the inlet to the outlet of the linear ion trap section.

A method of operating a quadrupole mass filter is disclosed. A first set of RF and resolving DC voltages are applied to electrodes of a quadrupole mass filter to selectively transmit first ions having a first mass-to-charge ratio (m/z). A second set of RF and resolving DC voltages are applied to electrodes of the quadrupole mass filter to selectively transmit second ions having a second m/z. Detection of the second ions is initiated after completion of a settling time. The settling time is determined in accordance with the relationship: Eq. 1, where t.sub.s is the settling time, (m/z).sub.1 is the first mass-to-charge ratio, (m/z).sub.2 is the second mass-to-charge ratio and A, B and C are empirically derived coefficients.

A method for driving a linear ion trap having rod electrodes arranged so as to surround a central axis includes: an ion-introducing step for introducing ions into an ion-capturing space surrounded by the rod electrodes, and for capturing the ions by a multipole RF electric field created within the ion-capturing space; and an ion-ejecting step for creating both a DC electric field for ion extraction extending from an external area outside the ion-capturing space into the ion-capturing space through a space between two predetermined rod electrodes neighboring each other around the central axis among the plurality of rod electrodes and the multipole RF electric field, and for sequentially ejecting ions according to their m/z from the ion-capturing space toward the external area through the space between the two predetermined rod electrodes by changing at least one of the multipole RF electric field and the DC electric field.

A gas analyzing apparatus includes: an ionization device that generates an ion flow of a sample gas; an analyzer that analyzes the ion flow supplied from the ionization device; a first ion path that non-linearly guides the ion flow from the ionization device to an inlet of the analyzer; and a blocking device for intermittently blocking and releasing, using an electric field or a magnetic field, the ion flow on at least part of a path of the ion flow through the first ion path to a mass filter of the analyzer. It is possible to perform measurement in a state where the ion flow is blocked and measurement in a state where the ion flow is not blocked.

This system and method disclosed herein are configured to improve high mass range ion trap performance by use of a multi-directional segmented scan approach. In some embodiments of the system and method disclosed herein, the mass range of conventional ion trap technology may be extended/increased without changing the hardware or compromising lower range mass/charge efficiency. Specifically, the system and methods disclosed herein use a segmented, bi-directional scan that increases the mass range of an ion trap mass spectrometer and circumvents the problem of mass discrimination during mass analysis in the high Thompson value range.

An ion trap mass spectrometer and methods for obtaining a mass spectrum of ions by scanning an RF frequency applied to the linear ion trap for mass selective ejection of the ions by using two power amplifiers to apply opposite phases of the RF to x and y electrodes.

A mass spectrometer is disclosed comprising a mass selective ion trap and a quadrupole rod set mass filter arranged downstream of the mass selective ion trap. Ions are mass selectively ejected from the ion trap in a substantially synchronized manner with the scanning of the mass filter in order to increase the duty cycle of the mass filter.

The invention generally relates to mass spectrometry via frequency tagging.

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.

An object of the invention is to provide a mass spectrometer system capable of obtaining a mass spectrum with high resolution as the mass number of an ion becomes higher. In the mass spectrometer system of the invention, a control unit 8 controls a mass spectrometry unit 4 so that a direct current voltage U, an amplitude V of a radio-frequency voltage, and a frequency F of the radio-frequency voltage, which are applied to a quadrupole electrode 13, are increased as a mass-to-charge ratio m/z of an ion of a target for mass spectrometry becomes larger. By controlling in this manner, the ion frequency when the ion passes through the inside of the mass spectrometry unit 4 is increased as the mass number of an ion becomes higher, and therefore, it is possible to obtain the mass spectrum with higher resolution.