A doubly bent X-ray spectroscopic device (1) according to the present invention includes: a glass plate (3) which is deformed into a shape having a doubly bent surface by being sandwiched between a doubly curved convex surface (21a) of a convex forming die (21) and a doubly curved concave surface (22a), of a concave forming die (22), that matches the doubly curved convex surface (21a), and being heated to a temperature of 400° C. to 600° C.; and a reflection coating (5) configured to reflect X-rays, which is formed on a concave surface (3a) of the deformed glass plate (3 ).

An optical component has a diffraction structure for diffractively influencing a direction of emergence of light of at least one wavelength incident on the optical component. The diffraction structure includes at least two diffraction substructures superimposed in at least one portion of the optical component and having first positive diffraction structures and first negative diffraction structures. A first diffraction substructure has first positive diffraction structures and first negative diffraction structures arranged to have a symmetry following a first symmetry condition. A second diffraction substructure has second positive diffraction structures and second negative diffraction structures arranged to have a second symmetry condition differing from the first symmetry condition. This can result in an optical component for which a production of a diffraction structure with a diffraction effect for different target wavelengths and/or an improved diffraction effect for one and the same target wavelength is made more flexible.

A reflector comprising a hollow body having an interior surface defining a passage through the hollow body, the interior surface having at least one optical surface part configured to reflect radiation and a supporter surface part, wherein the optical surface part has a predetermined optical power and the supporter surface part does not have the predetermined optical power. The reflector is made by providing an axially symmetric mandrel; shaping a part of the circumferential surface of the mandrel to form at least one inverse optical surface part that is not rotationally symmetric about the axis of the mandrel; forming a reflector body around the mandrel; and releasing the reflector body from the mandrel whereby the reflector body has an optical surface defined by the inverse optical surface part and a supporter surface part defined by the rest of the outer surface of the mandrel.

The present techniques relate to various aspects of forming and filling high-aspect ratio trench structures (e.g., trench structures having an aspect ratio of 20 or greater, including aspect ratios in the range of 20:1 up to and including 50:1 or greater) combined with trench opening widths ranging from 0.5 micron to 50 microns. In one implementation a method to fabricate high-aspect ratio trenches in silicon is provided using a patterned photoresist on evaporated aluminum. In accordance with this approach, a high-aspect ratio trench can be formed having vertical side walls and defect-free trench bottoms. In some instances it may be desirable to fill such high-aspect ratio trench structures with a metal or other substrate to provide certain functionality associated with the fill material. Further processes and structures are related in which such trench structures are filled using a mixture of high-Z nano-particles within an epoxy resin matrix.

A phase contrast X-ray imaging system includes: an illumination source adapted to illuminate a region of interest; a diffraction grating adapted to receive illumination from the illuminated region of interest, the diffraction grating comprising a spatial structure having a first periodicity superimposed with a second periodicity that is different from the first periodicity; and a detector adapted to detect illumination passing through the diffraction grating, wherein the spatial structure is defined by varying height and/or pitch, and wherein the spatial structure imparts a first phase dependence based on the first periodicity and an additional phase dependence based on the second periodicity on the illumination passing through the diffraction grating.

A method for applying a carbon-based reflective overcoating on a grazing incidence optical unit comprising a substrate and a coating of a high-density material chosen from the group comprising gold, platinum, iridium, palladium, rhodium, ruthenium, chrome and nickel or a low-density material such as carbon or B4C; the method comprises the step of treating the optical unit with a solution or gaseous phase containing at least one polymer precursor material to create the overcoating through absorption of the polymer material on the coating.

An EUV collector has a reflection surface with a basic mirror shape of a spherical section. A diffraction grating for EUV used light is applied to the reflection surface. The diffraction grating is designed so that the EUV used light, which emanates from a sphere center of the spherical section, is diffracted by the diffraction grating toward a collection region. The collection region is spatially spaced apart from the sphere center. This creates an EUV collector in which an effective separation between EUV used light, which is to be collected with the aid of the collector, and extraneous light having a wavelength that differs from a used light wavelength is made possible.

Improvements to atom interferometers. An improved atom interferometer has a single polarization-preserving fiber, coupled for propagation of beams of two Raman frequencies, and a parallel displacement beamsplitter for separating the laser beams into respective free-space-propagating parallel beams traversing at least one ensemble of atoms. A reflector generates one or more beams counterpropagating through the ensemble of atoms. Other improvements include interposing a beam-splitting surface common to a plurality of parallel pairs of beams counterpropagating through the ensemble of atoms, generating interference fringes between reflections of the beams to generate a detector signal; and processing the detector signal to derive at least one of relative phase and relative alignment between respective pairs of the counterpropagating beams.

An illumination system for an EUV projection lithographic projection exposure apparatus comprises an EUV light source, which generates an output beam of EUV illumination light with a predetermined polarization state. An illumination optical unit guides the output beam along an optical axis, as a result of which an illumination field in a reticle plane is illuminated by the output beam. The light source comprises an electron beam supply device, an EUV generating device and a polarization setting device. The EUV generating device is supplied with an electron beam by the electron beam supply device. The polarization setting device exerts an adjustable deflecting effect on the electron beam for setting the polarization of the output beam. This results in an illumination system, which operates on the basis of an electron beam-based EUV light source and provides an output beam, which is improved for a resolution-optimized illumination.

A multilayer mirror (M) reflecting extreme ultraviolet (EUV) radiation from a first wavelength range in an EUV spectral region includes a substrate (SUB) and a stack of layers (SL). The stack of layers has layers having a low index material and layers having a high index material. The low index material has a lower real part of the refractive index than does the high index material at a given operating wavelength in the first wavelength range. The stack of layers also includes a spectral purity filter on the stack of layers. The spectral purity filter is effective as an anti-reflection layer for ultraviolet (UV) radiation from a second wavelength range in a UV spectral region to increase an EUV-UV-reflectivity ratio of the multilayer mirror. The spectral purity filter (SPF) includes a non-diffractive graded-index anti-reflection layer (GI-AR) effective to reduce reflectivity in the second wavelength range.