An x-ray optical filter includes at least one x-ray optical mirror configured to receive a plurality of x-rays having a first x-ray spectrum with a first intensity as a function of energy in a predetermined solid angle range and to separate at least some of the received x-rays by multilayer reflection or total external reflection into reflected x-rays and non-reflected x-rays and to form an x-ray beam including at least some of the reflected x-rays and/or at least some of the non-reflected x-rays. The x-ray beam has a second x-ray spectrum with a second intensity as a function of energy in the solid angle range, the second intensity greater than or equal to 50% of the first intensity across a first continuous energy range at least 3 keV wide, the second intensity less than or equal to 10% of the first intensity across a second continuous energy range at least 100 eV wide.

A spectrometer includes a crystal analyzer having a radius of curvature that defines a Rowland circle, a sample stage configured to support a sample such that the sample is offset from the Rowland circle, an x-ray source configured to emit unfocused x-rays toward the sample stage, and a position-sensitive detector that is tangent to the Rowland circle. A method performed via a spectrometer includes emitting, via an x-ray source, unfocused x-rays toward a sample that is mounted on a sample stage such that the sample is offset from the Rowland Circle, thereby causing the sample to emit x-rays that impinge on the crystal analyzer or transmit a portion of the unfocused x-rays to impinge on the crystal analyzer; scattering, via the crystal analyzer, the x-rays that impinge on the crystal analyzer; and detecting the scattered x-rays via a position-sensitive detector that is tangent to the Rowland circle.

The present invention relates to a hard X-ray photoelectron spectroscopy (HAXPES) system comprising an X-ray tube, an X-ray monochromator, and a sample. The X-ray tube provides a beam of photons, which via the X-ray monochromator is directed through the system so as to excite electrons from the illuminated sample. The X-ray tube is connected to a monochromator vacuum chamber in which the X-ray monochromator is configured to monochromatize and focus the beam onto the sample. The monochromator vacuum chamber is connected to an analysis vacuum chamber, the illuminated sample being mounted inside the analysis vacuum chamber and the analysis vacuum chamber being connected to an electron energy analyser. The electron energy analyser is mounted onto the analysis vacuum chamber.

Further, the beam of photons provided from the X-ray tube is divergent and has an energy above 6 keV. The X-ray monochromator also comprises a curved optical element arranged to both monochromatize and focus the diverging beam of photons.

An X-ray generation apparatus comprising: an X-ray generating unit; a dispersive crystal whose surface is irradiated with an X-ray generated from the X-ray generating unit in order to monochromatize the X-ray; and a detecting unit that detects an X-ray generated from a sample irradiated with the X-ray monochromatized by the dispersive crystal. The dispersive crystal has a single-bent shape containing the surface that is a concave surface formed by integrating concave curve lines continuously along an axis perpendicular to a plane including the concave curve line. A direction in which a position on the surface irradiated with the X-ray generated from the X-ray generating unit moves is the direction along the axis.

An X-ray system for providing a converging X-rays comprises: (a) an X-ray source having an optical axis thereof; and an X-ray lens comprising at least one ring having a Bragg reflecting surface formed by a plurality of single-crystal tiles. Each tile individually comprises an adjusting arrangement enabling a tridimensional individual displacement thereof in angular and translational manner.

The invention utilizes one exposure without moving parts to provide multiple x-ray views of an object. It relies on a 3D detector, which can be a stack of film plates, and a specified focusing x-ray optic. The x-ray optic, discussed below, allows collection of x-rays from a localized volume, just like an ordinary optical lens, and the stacked film plate, or other 3D detector design, allows collection of the multiple focal plane information from one line of sight.

Systems and methods relate to arranging atoms into 1D and/or 2D arrays; exciting the atoms into Rydberg states and evolving the array of atoms, for example, using laser manipulation techniques and high-fidelity laser systems described herein; and observing the resulting final state. In addition, refinements can be made, such as providing high fidelity and coherent control of the assembled array of atoms. Exemplary problems can be solved using the systems and methods for arrangement and control of atoms.

Embodiments provide a multi-cone X-ray imaging Bragg crystal spectrometer for spectroscopy of small x-ray sources with a well-defined spectral resolution. The spectrometer includes a glass substrate machined to a multi-cone form; and a thin crystal slab attached to the glass substrate, whereby the multi-cone X-ray imaging Bragg crystal spectrometer provides rotational symmetry of a ray pattern, providing for accurate imaging, for each wavelength in the spectral range of interest. One or more embodiments include a streak camera and/or a gated strip detector.

A spectrometer focusing apparatus is provided that includes a hollow cylinder for x-rays to traverse a length thereof, a defracting element configured as a ring on an interior circumference of a portion of the hollow cylinder, at least one disk having an edge defining a circle aligned with the defracting element, and an aperture formed between the defracting element and the edge of the at least one disk.

An x-ray optical filter includes at least one x-ray optical mirror configured to receive a plurality of x-rays having a first x-ray spectrum with a first intensity as a function of energy in a predetermined solid angle range and to separate at least some of the received x-rays by multilayer reflection or total external reflection into reflected x-rays and non-reflected x-rays and to form an x-ray beam including at least some of the reflected x-rays and/or at least some of the non-reflected x-rays. The x-ray beam has a second x-ray spectrum with a second intensity as a function of energy in the solid angle range, the second intensity greater than or equal to 50% of the first intensity across a first continuous energy range at least 3 keV wide, the second intensity less than or equal to 10% of the first intensity across a second continuous energy range at least 100 eV wide.