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.

The disclosure includes an outer electrode and an inner electrode. The outer electrode defines an inner volume and is configured to receive injected electrons through at least one aperture. The inner electrode positioned in the inner volume. The outer electrode and inner electrode are configured to confine the received electrons in orbits around the inner electrode in response to an electric potential between the outer electrode and the inner electrode. The apparatus does not include a component configured to generate an electron-confining magnetic field.

The disclosure includes an outer electrode and an inner electrode. The outer electrode defines an inner volume and is configured to receive injected electrons through at least one aperture. The inner electrode positioned in the inner volume. The outer electrode and inner electrode are configured to confine the received electrons in orbits around the inner electrode in response to an electric potential between the outer electrode and the inner electrode. The apparatus does not include a component configured to generate an electron-confining magnetic field.

Vacuum-tight electrical feedthrough 10, comprising an electrically insulating insulator element 2 having a through-opening 23, having a first boundary surface 21 adjacent to the through-opening, and having a second boundary surface 22 also adjacent to the through-opening and opposite to the first boundary surface, and an electrically conductive conductor element 1 which extends through the through-opening 23 and which is connected to the insulator element 2 in a vacuum-tight manner along a circumferential line of the conductor element 1,

wherein the insulator element 2 is transmissive to electromagnetic radiation 25 in an optical wavelength range, and

wherein the first boundary surface 21 and/or the second 22 boundary surface is formed as a curved surface, in particular as a convex or concave surface.

The invention further relates to a vacuum pressure sensor having the vacuum-tight electrical feedthrough and a method for measuring a radiation intensity of electromagnetic radiation.

Vacuum-tight electrical feedthrough 10, comprising an electrically insulating insulator element 2 having a through-opening 23, having a first boundary surface 21 adjacent to the through-opening, and having a second boundary surface 22 also adjacent to the through-opening and opposite to the first boundary surface, and an electrically conductive conductor element 1 which extends through the through-opening 23 and which is connected to the insulator element 2 in a vacuum-tight manner along a circumferential line of the conductor element 1,

wherein the insulator element 2 is transmissive to electromagnetic radiation 25 in an optical wavelength range, and

wherein the first boundary surface 21 and/or the second 22 boundary surface is formed as a curved surface, in particular as a convex or concave surface.

The invention further relates to a vacuum pressure sensor having the vacuum-tight electrical feedthrough and a method for measuring a radiation intensity of electromagnetic radiation.

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.

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.

Example compact modular electron beam units are provided that can be used to generate electron beams using field emitter elements. A modular electron beam unit may comprise an electron beam source including a base portion, at least one field emitter element coupled to the base portion, the field emitter element including a field emitter tip, at least one gate electrode and a membrane window disposed over the at least one gate electrode.

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.