A waveguide gas laser having a laser resonator cavity of a variable length is subjected to cyclical varying of the length of the cavity during generation of a laser beam a length variation amount sufficient to force a laser beam generated in the resonator cavity though a substantially complete optical longitudinal cavity mode at a rate operable to smooth at least one laser beam parameter variation. In this manner variation in the laser beam parameter is averaged by moving through at least a portion of an optical longitudinal cavity mode.

A waveguide gas laser having a laser resonator cavity of a variable length is subjected to cyclical varying of the length of the cavity during generation of a laser beam a length variation amount sufficient to force a laser beam generated in the resonator cavity though a substantially complete optical longitudinal cavity mode at a rate operable to smooth at least one laser beam parameter variation. In this manner variation in the laser beam parameter is averaged by moving through at least a portion of an optical longitudinal cavity mode.

A system for generating an energy beam based laser includes an apparatus for receiving an energy beam and for generating an energy beam based laser. The apparatus is configurable or controllable for tuning an output wavelength of the laser generated by the apparatus using the energy beam. The apparatus includes a first component for producing a first magnetic field oriented in a first direction and a second component for producing a second magnetic field oriented in a second direction substantially opposite to the first direction. A channel through the apparatus is defined by the first component and the second component through which the energy beam passes to generate the laser at an output of the apparatus. The apparatus is configurable or controllable for modifying at least one of the first magnetic field and the second magnetic field for tuning the output wavelength of the laser.

A system for generating an energy beam based laser includes an apparatus for receiving an energy beam and for generating an energy beam based laser. The apparatus is configurable or controllable for tuning an output wavelength of the laser generated by the apparatus using the energy beam. The apparatus includes a first component for producing a first magnetic field oriented in a first direction and a second component for producing a second magnetic field oriented in a second direction substantially opposite to the first direction. A channel through the apparatus is defined by the first component and the second component through which the energy beam passes to generate the laser at an output of the apparatus. The apparatus is configurable or controllable for modifying at least one of the first magnetic field and the second magnetic field for tuning the output wavelength of the laser.

To cool a capacitor including a first electrode and a second electrode, a capacitor cooling structure includes: a conducting part electrically connected with the first electrode; an insulating part that has a first surface including a first position and a second surface including a second position, and is connected with the conducting part at the first position; a first fastening part configured to fasten the conducting part and the insulating part to each other; and a cooling part connected with the second position facing the first position, the conducting part and the cooling part being electrically insulated from each other by the insulating part.

To cool a capacitor including a first electrode and a second electrode, a capacitor cooling structure includes: a conducting part electrically connected with the first electrode; an insulating part that has a first surface including a first position and a second surface including a second position, and is connected with the conducting part at the first position; a first fastening part configured to fasten the conducting part and the insulating part to each other; and a cooling part connected with the second position facing the first position, the conducting part and the cooling part being electrically insulated from each other by the insulating part.

A dielectric electrode assembly, and a method (600) of manufacture thereof, including: a dielectric tube (226) having a cylindrical cross-section and a relative dielectric constant, .sub.2, the dielectric tube (226) filled with a gas having a relative dielectric constant, .sub.1; a structural dielectric (225) having a relative dielectric constant, .sub.3 surrounding the dielectric tube (226); metal electrodes (224) on opposite sides of the structural dielectric (225), the metal electrodes (224) having a flat cross-sectional geometry; and the structural dielectric (225) made from a material selected such that the relative dielectric constants of the structural dielectric (225), the dielectric tube (226), and the gas are interrelated and an approximately uniform electric field is generated within the dielectric tube (226) when power is applied to the metal electrodes (224).

A dielectric electrode assembly, and a method (600) of manufacture thereof, including: a dielectric tube (226) having a cylindrical cross-section and a relative dielectric constant, .sub.2, the dielectric tube (226) filled with a gas having a relative dielectric constant, .sub.1; a structural dielectric (225) having a relative dielectric constant, .sub.3 surrounding the dielectric tube (226); metal electrodes (224) on opposite sides of the structural dielectric (225), the metal electrodes (224) having a flat cross-sectional geometry; and the structural dielectric (225) made from a material selected such that the relative dielectric constants of the structural dielectric (225), the dielectric tube (226), and the gas are interrelated and an approximately uniform electric field is generated within the dielectric tube (226) when power is applied to the metal electrodes (224).

Systems and techniques for multilayer electrode assemblies are generally described. In some examples, a multilayer electrode assembly may comprise a first dielectric material. In some examples, the first dielectric material may be shaped so as to form a channel defined by an interior surface. In various examples the multilayer electrode assemblies may comprise a first metal layer disposed adjacent to a first portion of the exterior surface of the first dielectric material. In various further examples, the multilayer electrode assemblies may comprise a second metal layer disposed adjacent to a second portion of the exterior surface of the first dielectric material. In some examples, the first metal layer may be disposed in a first spaced relationship with the second metal layer. In various examples, a substantially uniform electric field may be generated in the channel of the first dielectric material when a voltage is applied to the multilayer electrode assembly.

A dielectric resonator is excited at its natural resonant frequency to produce a highly uniform electric field for the generation of plasma. The plasma may be used as a desolvator, atomizer excitation source and ionization source in an optical spectrometer or a mass spectrometer.