Abstract:
A method and apparatus for pulsed ion cyclotron resonance spectroscopy is disclosed in which a gas sample within an analyzer cell is ionized by means such as a pulse of an electron beam. The ions are subjected to a combined action of a plurality of static electric fields and a magnetic field thereby trapping the ions and causing them to move orbitally within the cell. Following ionization by said pulse of an electron beam and after a reaction time delay period, ions of a given charge-to-mass ratio are brought into resonance with an oscillating electric field applied transversely to the lines of force of the magnetic field. During such detection period those ions in resonance with the oscillating electric field absorb energy therefrom, which absorbed energy is detected as a measure of the resonant ions. The ions are then swept from the cell. By use of oscillating electric fields of different frequencies for resonance with ions of different charge-to-mass ratio the arrangement serves a mass spectrometer function. For ion-molecule reaction studies the above described cycle is repeated but with different reaction time delay periods whereby the concentration of the resonant ions at different times during the course of reaction is determined. From this, the thermal rate constant for such ion-molecule reaction is readily determined. The method and apparatus of this invention are readily adapted for double resonance mass spectroscopy. By irradiating the ions with a pulsed radio frequency electric field at a second frequency, ions of a given charge-to-mass ratio may be accelerated to high velocity, yet still remain trapped within the analyzer cell. As above, after a reaction time delay period following said radio frequency pulse, ions of a given charge-tomass ratio are brought into resonance with the first mentioned oscillating electric field to obtain a measure of such ions. Also as above, this double resonance cycle may be repeated with different reaction time delay periods. By this means the thermal rate constant for the reaction as a function of the kinetic energy of the ions accelerated by the pulsed radio frequency electric field at the second frequency is readily determined. The spectrometer includes a novel analyzer cell within which ions may be trapped for long periods of time on the order of 100 milliseconds, or greater. The cell includes a hollow electrode array comprising first, second and third pairs of opposite plates. A trapping potential of one polarity is applied to the one pair of opposite plates, and an opposite polarity trapping potential is applied the other two pair of opposite plates to provide an electrostatic potential well within the cell for trapping the ions for extended periods. Various experiments requiring extended ion trapping periods are possible utilizing the novel ion trap.