Abstract:
A nebuliser outlet (20) comprises one or more first channels (24), wherein the nebuliser outlet (20) is configured such that liquid received by the nebuliser outlet (20) can pass to one or more nebulisation regions via the one or more first channels (24), and one or more second channels (25), wherein the nebuliser outlet (20) is configured such that gas received by the nebuliser outlet (20) can pass to the one or more nebulisation regions via the one or more second channels (25). The one or more first channels (24) comprise a first portion (24a) and a second portion (24b), wherein the first portion (24a) comprises a tubular channel, and wherein the second portion (24b) comprises multiple channels, an annular channel, or a segmented annular channel. The one or more second channels (25) converge with the second portion (24b) at the one or more nebulisation regions.
Abstract:
A dual-mode ion detector for a mass and/or ion mobility spectrometer comprising a first conversion electrode (20) that is maintained, in use, at a negative potential and arranged for converting incident positive ions (32) into secondary electrons (34), and a second conversion electrode (22) that is maintained, in use, at a positive potential and arranged for converting incident negative ions (42) into secondary positive ions (44) and/or secondary electrons (74). The detector also comprises an electron detecting surface (26) and an entrance electrode (24) for drawing ions into the ion detector. The ion detector is switchable between a first mode for detecting positive ions and a second mode for detecting negative ions.
Abstract:
A pulsed ion source is disclosed wherein the ion source is energised one or more times to generate a first group of ions and a second group of ions. The first and second groups of ions are simultaneously transmitted through an ion guide whilst keeping the first and second groups of ions isolated from each other.
Abstract:
Apparatus for a mass spectrometer is disclosed comprising an ion source, a heater (230) for heating a gas flow (224) to the ion source, a temperature sensor for monitoring the temperature of the heater (230), and a control system (236). The control system (236) is arranged and adapted to determine a flow rate of the gas flow (224) by monitoring the power supplied to the heater (230) and the temperature of the heater (230).
Abstract:
A mass spectrometer or ion mobility spectrometer is disclosed comprising means for detecting a blockage in an inlet orifice (6) arranged between an ion source and a vacuum chamber (2). The blockage is detected as a result of a reduction in pressure within the vacuum chamber (2). This change in pressure is detected indirectly by monitoring the amount of power that a vacuum pump (10) is using, the amount of current that a vacuum pump (10) is drawing, the temperature of a vacuum pump (10) or a region in proximity to the vacuum pump (10), or the flow rate of gas out of a vacuum pump (10).
Abstract:
A miniature mass spectrometer is disclosed comprising an atmospheric pressure ionisation source (701) and a first vacuum chamber having an atmospheric pressure sampling orifice or capillary, a second vacuum chamber located downstream of the first vacuum chamber and a third vacuum chamber located downstream of the second vacuum chamber. An ion detector (705) is located in the third vacuum chamber. A first RF ion guide is located within the first vacuum chamber and a second RF ion guide (703) is located within the second vacuum chamber. The ion path length from the atmospheric pressure sampling orifice or capillary to an ion detecting surface of the ion detector (705) is ≤ 400 mm. The mass spectrometer further comprises a tandem quadrupole mass analyser,a 3D ion trap mass analyser, a 2D or linear ion trap mass analyser, a Time of Flight mass analyser, a quadrupole-Time of Flight mass analyser or an electrostatic mass analyser arranged in the third vacuum chamber. The product of the pressure P 1 in the vicinity of the first RF ion guide and the length L 1 of the first RF ion guide is in the range 10-100 mbar-cm and the product of the pressure P 2 in the vicinity of the second RF ion guide (703) and the length L 2 of the second RF ion guide (703) is in the range 0.05-0.3 mbar-cm.
Abstract:
A miniature mass spectrometer is disclosed comprising an atmospheric pressure ionisation source (701), a first vacuum chamber having an atmospheric pressure sampling orifice or capillary, a second vacuum chamber located downstream of the first vacuum chamber and a third vacuum chamber located downstream of the second vacuum chamber. An ion detector (705) is located in the third vacuum chamber. A first RF ion guide is located within the first vacuum chamber and a second RF ion guide (703) is located within the second vacuum chamber. The ion path length from the atmospheric pressure sampling orifice or capillary to an ion detecting surface of the ion detector (705) is ≤ 400 mm. The product of the pressure P 1 in the vicinity of the first RF ion guide and the length L 1 of the first RF ion guide is in the range 10-100 mbar-cm and the product of the pressure P 2 in the vicinity of the second RF ion guide (703) and the length L 2 of the second RF ion guide (703) is in the range 0.05-0.3 mbar-cm.
Abstract:
A RF only quadrupole rod set mass filter or mass analyser and a linear quadrupole ion trap with axial ejection are disclosed comprising a first pair of rod electrodes, a second pair of rod electrodes and an energy filter. The first pair of rod electrodes is longer than the second pair of rod electrodes. Ions having desired mass to charge ratios experience fringing fields at an exit region which results in the ions possessing sufficient axial kinetic energy to be transmitted by the energy filter. Other ions possess insufficient axial kinetic energy to be transmitted by the energy filter and are attenuated.
Abstract:
A mass or mass to charge ratio selective ion trap is disclosed which directs ions into a small ejection region. A RF voltage acts to confine ions in a first (y) direction within the ion trap. A DC or RF voltage acts to confine ions in a second (x) direction. A quadratic DC potential well acts to confine ions in a third (z) direction within the ion trap. The profile of the quadratic DC potential well progressively varies along the second (x) direction.
Abstract:
A mass spectrometer is disclosed comprising two vacuum chambers maintained at different pressures. The two vacuum chambers are interconnected by a differential pumping aperture (5a). The effective area of the opening (5a) between the two vacuum chambers may be varied by rotating a disk (7) having an aperture (7) a in front of the differential pumping aperture (5a) so as to vary the gas flow rate through the opening (5a) and between the two chambers.