A cold cathode ionization vacuum gauge includes an extended anode electrode and a cathode electrode surrounding the anode electrode along its length and forming a discharge space between the anode electrode and the cathode electrode. The vacuum gauge further includes an electrically conductive guard ring electrode interposed between the cathode electrode and the anode electrode about a base of the anode electrode to collect leakage electrical current, and a discharge starter device disposed over and electrically connected with the guard ring electrode, the starter device having a plurality of tips directed toward the anode and forming a gap between the tips and the anode.

A cold cathode ionization vacuum gauge includes an extended anode electrode and a cathode electrode surrounding the anode electrode along its length and forming a discharge space between the anode electrode and the cathode electrode. The vacuum gauge further includes an electrically conductive guard ring electrode interposed between the cathode electrode and the anode electrode about a base of the anode electrode to collect leakage electrical current, and a discharge starter device disposed over and electrically connected with the guard ring electrode, the starter device having a plurality of tips directed toward the anode and forming a gap between the tips and the anode.

Method for the regeneration of a volume getter pump in a vacuum apparatus with a volume getter pump and an ion getter pump where the operating voltage of the ion getter pump is reduced, the current through the ion getter pump is recorded for determination of the pressure in the vacuum apparatus and then a heating element of the NEG is controlled as a function of the current of the ion getter pump for the purpose of heating the NEG material.

Method for the regeneration of a volume getter pump in a vacuum apparatus with a volume getter pump and an ion getter pump where the operating voltage of the ion getter pump is reduced, the current through the ion getter pump is recorded for determination of the pressure in the vacuum apparatus and then a heating element of the NEG is controlled as a function of the current of the ion getter pump for the purpose of heating the NEG material.

The invention relates to a method 100 for determining a pressure in a vacuum system, wherein the method comprises the steps of: a) generating 101 a plasma in a sample chamber which is fluid-dynamically connected to the vacuum system and which is in electrical contact with a first electrode and a second electrode; b) measuring 102 a current intensity of an electrical current flowing through the plasma between the first electrode and the second electrode; c) measuring 103 a first radiation intensity of electromagnetic radiation of a first wavelength range which is emitted from the plasma, wherein the first wavelength range contains at least a first emission line of a first plasma species of a first chemical element; d) measuring 104 a second radiation intensity of electromagnetic radiation of a second wavelength range which is emitted from the plasma, wherein the second wavelength range contains a second emission line of the first plasma species of the first chemical element or of a second plasma species of the first chemical element, and wherein the second emission line is outside the first wavelength range; and e) determining 105 the pressure in the vacuum system as a function of the measured current intensity, the measured first radiation intensity, and the measured second radiation intensity. Further, the invention relates to a vacuum pressure sensor.

A cold cathode ionization gauge includes multiple cathodes providing different spacings between the cathodes and an anode. The multiple cathodes allow for pressure measurements over wider ranges of pressure. A first cathode with a larger spacing may provide current based on Townsend discharge; whereas, a second cathode having a smaller spacing may provide current based on both Townsend discharge at higher pressures and on Paschen's Law discharge at still higher pressures. A feature on the second cathode may support Paschen's Law discharge. Large resistances between the cathodes and a return to power supply enable control of output profiles to extend the pressure ranges with accurate responses and avoid output minima. Pressure measurements may be made based on currents from respective cathodes dependent on the outputs of the cathodes through the wide pressure range of measurement. The multiple cathodes may also provide measurements that avoid the discontinuities found in current outputs of the respective cathodes.

Provided are: a vacuum gauge that, with a simple configuration, can accurately diagnose the degree of contamination of the vacuum gauge; and a contamination diagnosis method that, with a simple process, can accurately diagnose the degree of contamination of a vacuum gauge. Provided is a cold cathode ionization vacuum gauge that has a normal operation mode and a contamination diagnosis mode, the cold cathode ionization vacuum gauge comprising: an anode 1 and a cathode 3 that are for measuring vacuum pressure in the normal operation mode; an anode 7 and the cathode 3 that are for measuring the vacuum pressure in the contamination diagnosis mode; and a controller 10 that compares the size of a current measured between the anode 7 and the cathode 3 and the size of a current measured between the anode 1 and the cathode 3.

The invention relates to an ionization vacuum measuring cell (10) comprising an evacuable housing (12) with a measurement connection for a vacuum to be measured at an end portion; a measurement chamber (14) in the housing (12), said measurement chamber being fluidically connected to the measurement connection, wherein the measurement chamber (14) is designed as a replaceable component; and a first and a second electrode (16, 18) in the measurement chamber (14), said electrodes being substantially coaxial to an axis and being arranged at a distance from each other. The measuring cell further comprises an electrically insulating and vacuum-tight feedthrough (20) for an electric supply to the second electrode (18) and a magnetization assembly which is designed to generate a magnetic field in the ionization chamber. According to the invention, the measurement chamber (14), in particular at least one of the electrodes (16, 18), comprises a magnetic material.

The invention relates to an ionization vacuum measuring cell (10) comprising an evacuable housing (12) with a measurement connection for a vacuum to be measured at an end portion; a measurement chamber (14) in the housing (12), said measurement chamber being fluidically connected to the measurement connection, wherein the measurement chamber (14) is designed as a replaceable component; and a first and a second electrode (16, 18) in the measurement chamber (14), said electrodes being substantially coaxial to an axis and being arranged at a distance from each other. The measuring cell further comprises an electrically insulating and vacuum-tight feedthrough (20) for an electric supply to the second electrode (18) and a magnetization assembly which is designed to generate a magnetic field in the ionization chamber. According to the invention, the measurement chamber (14), in particular at least one of the electrodes (16, 18), comprises a magnetic material.

A system of measuring and correcting for distortions in homodyne systems and a method for operating a data processing system to provide an estimate of distortions in homodyne systems are disclosed. The method for operating a data processing system to provide an estimate of a distortion introduced by a homodyne system when the homodyne system processes a time a multi-tone time domain input signal, x(t), to obtain a time domain output signal, y(t) includes receiving a frequency spectrum, X(f), of the multi-tone time domain input signal, x(t) and measuring an output frequency spectrum, Y(f), when the homodyne system operates on x(t). A plurality of parameters of a model that represents a linear frequency response of the homodyne system when operating on X(f) to arrive at Y(f) by fitting the model to Y(f) and X(f) is determined, and the model is applied to X(f) and Y(f) to estimate the distortions.