An RF fluorescent lamp, comprising a bulbous vitreous portion of the RF fluorescent lamp comprising a vitreous envelope filled with a working gas mixture, a power coupler to induce an alternating electric field within the vitreous envelope, an electronic ballast, and a mercury amalgam accommodating structure mounted within the lamp envelope and adapted to absorb power from the electric field to rapidly heat and vaporize an amalgam of mercury to rapidly illuminate the lamp envelope during a turn-on phase of the RF fluorescent lamp, wherein the structure is comprised of a substrate material coated with a mixture of indium and gold.

A light-emitting plasma lamp bulb for solar ultraviolet simulation includes a bulb cover having a spherical shape or a rod shape through which ultraviolet rays are transmittable, discharge gas contained in the bulb cover, and a first light-emitting material and a second light-emitting material, wherein the first light-emitting material includes at least one of mercury (Hg) and mercury iodide (HgI.sub.2), and the second light-emitting material includes sulfur (S.sub.8), wherein light emitted from the bulb has a maximum optical power intensity in a range of 395 to 455 nm which is an ultraviolet-visible boundary region, wherein, when compared using a same ultraviolet dose in an ultraviolet region of 290 to 400 nm, an integrated intensity of a visible and infrared region of 400 to 850 nm is equal to or less than of an integrated intensity of a visible and infrared region of a standard solar spectrum (ASTM G173, AM 1.5G).

A plasma lamp is provided that employs excitation transfer between two atomic or molecular species so as to preferentially produce light at a specific atomic or molecular emission wavelength. The lamp includes a lamp body. The lamp body includes a top portion, a middle portion having an internal hollow space filled with an energy-donor chemical gas and an energy-acceptor chemical element, and a bottom portion. The lamp body further includes an array of a plurality of cavities connected to the internal hollow space. The internal hollow space and the array of the plurality of cavities are spaced apart from outer surfaces of the lamp body. The plasma lamp is configured to excite the energy-donor chemical gas by an ignition of a low-temperature plasma within the internal hollow space and the array of the plurality of cavities to cause an excitation transfer from the excited energy-donor chemical gas to the energy-acceptor chemical element, thereby emitting radiation having a wavelength of about 194 nm when mercury (Hg) is the energy-acceptor chemical element and helium (He) serves as the donor. Other wavelengths in the ultraviolet (UV) and vacuum ultraviolet (VUV) spectral regions are generated when other donor and acceptor atoms or molecules are employed. These lamps are well-suited as optical drivers for atomic clocks (such as the 40.5 GHz Hg ion clock), photochemical processing of materials, disinfection of water, air, and surfaces, as well as other applications requiring UV or VUV light.

A plasma lamp is provided that employs excitation transfer between two atomic or molecular species so as to preferentially produce light at a specific atomic or molecular emission wavelength. The lamp includes a lamp body. The lamp body includes a top portion, a middle portion having an internal hollow space filled with an energy-donor chemical gas and an energy-acceptor chemical element, and a bottom portion. The lamp body further includes an array of a plurality of cavities connected to the internal hollow space. The internal hollow space and the array of the plurality of cavities are spaced apart from outer surfaces of the lamp body. The plasma lamp is configured to excite the energy-donor chemical gas by an ignition of a low-temperature plasma within the internal hollow space and the array of the plurality of cavities to cause an excitation transfer from the excited energy-donor chemical gas to the energy-acceptor chemical element, thereby emitting radiation having a wavelength of about 194 nm when mercury (Hg) is the energy-acceptor chemical element and helium (He) serves as the donor. Other wavelengths in the ultraviolet (UV) and vacuum ultraviolet (VUV) spectral regions are generated when other donor and acceptor atoms or molecules are employed. These lamps are well-suited as optical drivers for atomic clocks (such as the 40.5 GHz Hg ion clock), photochemical processing of materials, disinfection of water, air, and surfaces, as well as other applications requiring UV or VUV light.

Embodiments of the present invention describe electrical potential energy to electrical kinetic energy converters, ozone generators, and light emitters. A system for energy conversion from electrical potential energy to electrical kinetic energy may include a discharge device and a power supply. The power supply can be coupled with the discharge device, and supplies energy to the discharge device to form an initial electric field. The discharge device may further include at least two electrodes that are either mesh electrodes or wire-array electrodes. Furthermore, a space between the at least two electrodes is filled with a gas medium and an electric field is created by the power supply in a normal direction relative to planes formed by the elements of electrodes.

Embodiments of the present invention describe electrical potential energy to electrical kinetic energy converters, ozone generators, and light emitters. A system for energy conversion from electrical potential energy to electrical kinetic energy may include a discharge device and a power supply. The power supply can be coupled with the discharge device, and supplies energy to the discharge device to form an initial electric field. The discharge device may further include at least two electrodes that are either mesh electrodes or wire-array electrodes. Furthermore, a space between the at least two electrodes is filled with a gas medium and an electric field is created by the power supply in a normal direction relative to planes formed by the elements of electrodes.

A line-narrowed KrF excimer laser apparatus includes a laser chamber, a line narrow optical system, an actuator, an output coupling mirror, a wavelength detecting unit, and a wavelength controller. The actuator is capable of changing a wavelength of light selected by the line narrow optical system. The wavelength detecting unit includes a low-pressure mercury lamp accommodating mercury, a getter material that adsorbs at least a part of the mercury, and a hot cathode that excites at least a part of the mercury, an etalon provided at a position where reference light emitted from the low-pressure mercury lamp and detected light emitted from the output coupling mirror are incident on the etalon, and a light intensity distribution sensor configured to detect an intensity distribution profile of interference fringes of the reference light and an intensity distribution profile of interference fringes of the detected light.

The present invention generally relates to a system for treating a fluid and specifically to a treatment system configured for improved bacterial reduction, wherein the system comprises a field emission based UV light source adapted to emit light within a ultraviolet C (UVC) spectrum with a wavelength range having an upper range limit being higher compared to light emitted from a mercury based UV light source.

The present invention generally relates to a system for treating a fluid and specifically to a treatment system configured for improved bacterial reduction, wherein the system comprises a field emission based UV light source adapted to emit light within a ultraviolet C (UVC) spectrum with a wavelength range having an upper range limit being higher compared to light emitted from a mercury based UV light source.

A system, method, and computer program product for optimizing the cooling of a UV bulb during a UV irradiation process is described. A power level in which to operate the UV bulb is received. In addition, a particular type of UV bulb being used in the UV irradiation process is received. Thereafter, at least one optimal UV cooling parameter that corresponds to the power level and the type of UV bulb is retrieved from a UV source parameters database. At least one control signal is then sent to a cooling device that is based on the retrieved optimal UV cooling parameter, and the control signal instructs the cooling device to cool the particular type of UV bulb according to the retrieved optimal UV cooling parameter during the UV irradiation process.