Abstract:
The disclosure includes an ionization chamber, a first electron multiplier, and a second electron multiplier. The ionization chamber is configured to receive gas molecules from an environment at a pressure. The first electron multiplier is configured to receive a plurality of photons from a photon source, generate a first plurality of electrons from the plurality of photons, and discharge the first plurality of electrons into the ionization chamber to generate a plurality of gas ions from at least a portion of the gas molecules. The second electron multiplier is configured to receive the plurality of gas ions from the ionization chamber and generate a second plurality of electrons from the plurality of gas ions that is proportional to a quantity of the plurality of gas ions. A quantity of electrons of the second plurality of electrons is indicative of the pressure.
Abstract:
An ionization gauge to measure pressure, while controlling the location of deposits resulting from sputtering when operating at high pressure, includes at least one electron source that emits electrons, and an anode that defines an ionization volume. The ionization gauge also includes a collector electrode that collects ions formed by collisions between the electrons and gas molecules and atoms in the ionization volume, to provide a gas pressure output. The electron source can be positioned at an end of the ionization volume, such that the exposure of the electron source to atom flux sputtered off the collector electrode and envelope surface is minimized. Alternatively, the ionization gauge can include a first shade outside of the ionization volume, the first shade being located between the electron source and the collector electrode, and, optionally, a second shade between the envelope and the electron source, such that atoms sputtered off the envelope are inhibited from depositing on the electron source.
Abstract:
A cold cathode ionization vacuum gauge, including: two electrodes disposed such that one of the electrodes is surrounded by the other electrode to thereby form a discharge space therebetween; and an electrode protection member disposed in the discharge space and configured to protect an inner wall surface of the other electrode, wherein the electrode protection member has electric conductivity and is elastically deformed along a shape of the inner wall surface to be electrically connected to the other electrode.
Abstract:
An ionization gauge including a source of electrons; an open anode defining an anode volume, where the source of electrons is disposed outside the anode volume; a plurality of ion collector electrodes disposed within the anode volume; a plurality of axially extending anode support posts for supporting the open anode, the anode support posts being electrically connected to the open anode; and the plurality of ion collector electrodes being respectively located sufficiently close to the plurality of axially extending anode support posts so as to substantially repel the electrons from the anode support posts.
Abstract:
For measuring the charge transported in an ion or electron beam, collecting grids are provided in a cascaded manner and the galvanic currents occurring there are measured. The same surface range is measured on the collecting cascade with respect to the particle current in the vacuum. The process and apparatus have particular applicability in partial-pressure and total-pressure measuring apparatuses, e.g. mass spectrometers and Bayard-d'Alpert tubes.
Abstract:
Ionization gauge and method of operating same where the gauge may be of the Bayard-Alpert type and include a shield which completely encloses the electron source, the anode, and the collector electrode so that potentials external to the shield do not disturb the electric charge distribution within the shielded volume to thus stabilize the sensitivity of the gauge. The ionization gauge is further characterized by the following features which may be present either alone or in combination including: (a) the anode is provided with end caps which extend radially inward at least 25% of the radius of the anode but not more than 75% of the radius; (b) the ion collector has a diameter of not less than 0.015 in. and not more than 0.080 in.; (c) the ion collector extends at its free end at least through one of the partial end caps of the anode; (d) the electron source is not substantially longer axially than the region within the anode volume in which the electric field is predominantly directed radially inward and where the electron source is located substantially only adjacent to the foregoing region; (e) the anode is provided with a substantially uniformly transparent grid structure in the regions where the electrons enter the anode volume and where they exit from the anode volume. Moreover, the above features may be utilized in other hot cathode ionization gauges where, for example, the above features (a) and (d) may be utilized in triode gauges.
Abstract:
Heavy-weight, fast-moving molecular ions are slowed down in a light-weight collision gas to very low velocities and small distributions of velocity before their mass-spectrometric analysis. The velocity reduction of the ions which occurs in the collision gas reduces both ion energy and phase space. In accordance with one embodiment, in order to minimize fragmentation of large molecular ions, an ultrasonic gas jet traveling in the same direction as the ions is used for slowing down the ions. In accordance with another embodiment, the ions are examined in storage mass spectrometers such as ICR spectrometers or ion traps.