Abstract: A method and apparatus for generating membrane targets for a laser induced plasma is disclosed herein. Membranes are advantageous targets for laser induced plasma because they are very thin and can be readily illuminated by high-power coherent light, such as a laser, and converted into plasma. Membranes are also advantageous because illumination of the membrane with coherent light produces less debris and splashing than illumination of a thicker, solid target. Spherical membranes possess additional advantages in that they can be readily illuminated from variety of directions and because they can be easily placed (i.e. blown) into a target region for illumination by coherent light. Membranes are also advantageous because they can be formed from a liquid or molten phase of the target material. According to another embodiment, membranes can be formed from a solution in which the target materials are solvated.

Abstract: A method and apparatus for generating membrane targets for a laser induced plasma is disclosed herein. Membranes are advantageous targets for laser induced plasma because they are very thin and can be readily illuminated by high-power coherent light, such as a laser, and converted into plasma. Membranes are also advantageous because illumination of the membrane with coherent light produces less debris and splashing than illumination of a thicker, solid target. Spherical membranes possess additional advantages in that they can be readily illuminated from variety of directions and because they can be easily placed (i.e. blown) into a target region for illumination by coherent light. Membranes are also advantageous because they can be formed from a liquid or molten phase of the target material. According to another embodiment, membranes can be formed from a solution in which the target materials are solvated.

Abstract: The present invention provides a high gain collimator producing generally uniform intensity profiles for use in lithography and other applications. A focusing optic is also provided. The collimator includes a reflector and guide channel. The guide channel preferably includes polycapillary tubes and/or microchannel plates. The polycapillary tubes are used to collimate or focus the central portion of the x-ray beam in a circular, elliptic, square, or rectangular shape. A conical, parabolic resonance reflector or grazing incidence reflector with a shape similar to the polycapillary collimator is used to increase the solid angle collected and produce a circular, square, etc. annular x-ray beam whose inside dimensions are approximately equal to the exit dimensions of the polycapillary collimator.

Abstract: A parallel nanotomography imaging system is provided having an x-ray source, which is preferably a laser-based x-ray source that generates x-rays that are collected using a collector optic and are received in a composite objective assembly. The composite objective assembly includes plural micro-objectives, each imaging the target. The x-ray image is received by an x-ray image formation and acquisition apparatus, and processed and/or displayed.

Abstract: A shaped plasma discharge system is provided in which a shaped radiation source emits radiation at a desired frequency and in a desired shape. In one embodiment, a laser source provides an output beam at a desired intensity level to shaping optics. The shaping optics alters the output beam into a desired shaped illumination field. In an alternate embodiment, plural laser sources provide plural output beams and the shaping optics can produce a compound illumination field. The illumination field strikes a target material forming a plasma of the desired shape that emits radiation with a desired spatial distribution, at a desired wavelength, preferably in the x-ray, soft x-ray, extreme ultraviolet or ultraviolet spectra. In another embodiment an electric discharge generates the required shaped radiation field. The shaped emitted radiation proceeds through an optical system to a photoresist coated wafer, imprinting a pattern on the wafer.

Abstract: A laser-excited X-ray source in which the efficiency of conversion of laser energy into X-ray energy, and the average X-ray output power, are increased by providing laser light, which is focussed on a target to generate X-rays, in the form of trains of very short pulses with a pulse duration in the range 1-10 picoseconds. Preferably it is arranged such that successive pulses in a train are focussed at adjacent but different points on the target.