Sigray, Inc.

Xradia, Inc.

Rec Solar Pte. Ltd.

Carl Zeiss X-ray Microscopy, Inc.

Other

University of California

Air Techniques, Inc.

Alan Francis Lyon

Wenbing Yun

Janos Kirz

Sylvia Jia Yun Lewis

Michael Feser

Richard Hamilton Sewell

Srivatsan Seshadri

Andreas Bentzen

Claude A Goodman

Daniel N Wildermuth

Sharon Chen

David Charles Reynolds

Young Seen Lee

Lawrence Schloss

Yuxin Wang

Thomas Anthony Case

Benjamin Donald Stripe

Victor Perez-Mendez

David Vine

Yan Feng

Nemia Grubisich

Roger Thompson

Toshio Itoh

Hiroaki Hayashigatani

An x-ray imaging system includes an x-ray source, a beam-splitting grating having a plurality of structures arranged in a two-dimensional periodic array, a stage configured to hold an object to be imaged, and an x-ray detector having a two-dimensional array of x-ray detecting elements and positioned to detect x-rays diffracted by the beam-splitting grating and perturbed by the object to be imaged.

X-ray imaging system

A method for performing x-ray absorption spectroscopy and an x-ray absorption spectrometer system to be used with a compact laboratory x-ray source to measure x-ray absorption of the element of interest in an object with both high spatial and high spectral resolution. The spectrometer system comprises a compact high brightness laboratory x-ray source, an optical train to focus the x-rays through an object to be examined, and a spectrometer comprising a single crystal analyzer (and, in some embodiments, also a mosaic crystal) to disperse the transmitted beam onto a spatially resolving x-ray detector. The high brightness/high flux x-ray source may have a take-off angle between 0 and 105 mrad. and be coupled to an optical train that collects and focuses the high flux x-rays to spots less than 500 micrometers, leading to high flux density. The coatings of the optical train may also act as a 'low-pass' filter, allowing a predetermined bandwidth of x-rays to be observed at one time while excluding the higher harmonics.

Method of performing X-ray spectroscopy and X-ray absorption spectrometer system

This disclosure presents systems for x-ray microscopy using an array of micro-beams having a micro- or nano-scale beam intensity profile to provide selective illumination of micro- or nano-scale regions of an object. An array detector is positioned such that each pixel of the detector only detects x-rays corresponding to a single micro- or nano-beam. This allows the signal arising from each x-ray detector pixel to be identified with the specific, limited micro- or nano-scale region illuminated, allowing sampled transmission image of the object at a micro- or nano-scale to be generated while using a detector with pixels having a larger size and scale. Detectors with higher quantum efficiency may therefore be used, since the lateral resolution is provided solely by the dimensions of the micro- or nano-beams. The micro- or nano-scale beams may be generated using an arrayed x-ray source or a set of Talbot interference fringes.

Method and apparatus for x-ray microscopy

An x-ray interferometric imaging system includes an x-ray source with a target having a plurality of discrete structures arranged in a periodic pattern. The system further includes a beam-splitting x-ray grating, a stage configured to hold an object to be imaged, and an x-ray detector having a two-dimensional array of x-ray detecting elements. The object is positioned between the beam-splitting x-ray grating and the x-ray detector, the x-ray detector is positioned to detect the x-rays diffracted by the beam-splitting x-ray grating and perturbed by the object to be imaged.

X-ray interferometric imaging system

An x-ray illumination beam system includes an electron emitter and a target having one or more target microstructures. The one or more microstructures may be the same or different material, and may be embedded or placed atop a substrate formed of a heat-conducting material. The x-ray source may emit x-rays towards an optic system, which can include one or more optics that are matched to one or more target microstructures. The matching can be achieved by selecting optics with the geometric shape, size, and surface coating that collects as many x-rays as possible from the source and at an angle that satisfies the critical reflection angle of the x-ray energies of interest from the target. The x-ray illumination beam system allows for an x-ray source that generates x-rays having different spectra and can be used in a variety of applications.

X-ray illumination system with multiple target microstructures

A compact source for high brightness x-ray generation is disclosed. The higher brightness is achieved through electron beam bombardment of multiple regions aligned with each other to achieve a linear accumulation of x-rays. This may be achieved through the use of x-ray targets that comprise microstructures of x-ray generating materials fabricated in close thermal contact with a substrate with high thermal conductivity. This allows heat to be more efficiently drawn out of the x-ray generating material, and allows bombardment of the x-ray generating material with higher electron density and/or higher energy electrons, leading to greater x-ray brightness. The orientation of the microstructures allows the use of a take-off angle at or near 0&#xb0;, allowing the accumulation of x-rays from several microstructures to be aligned and be used to form a beam in the shape of an annular cone.

Diverging X-ray sources using linear accumulation

A compound x-ray lens and method of fabricating these lenses are disclosed. These compound lenses use multiple zone plate stacking to achieve a pitch frequency increase for the resulting combined zone plate. The compound equivalent zone plate includes a first zone plate having an initial pitch frequency stacked onto a second zone plate to form an equivalent compound zone plate. The equivalent zone plate has a pitch frequency that is at least twice the initial pitch frequency. Also, in one example, the equivalent zone plate has a mark-to-space ratio of 1:1.

Stacked zone plates for pitch frequency multiplication

A compact source for high brightness x-ray generation is disclosed. The higher brightness is achieved through electron beam bombardment of multiple regions aligned with each other to achieve a linear accumulation of x-rays. This may be achieved by aligning discrete x-ray sub-sources, or through the use of x-ray targets that comprise microstructures of x-ray generating materials fabricated in close thermal contact with a substrate with high thermal conductivity. This allows heat to be more efficiently drawn out of the x-ray generating material, and in turn allows bombardment of the x-ray generating material with higher electron density and/or higher energy electrons, leading to greater x-ray brightness. The orientation of the microstructures allows the use of an on-axis collection angle, allowing the accumulation of x-rays from several microstructures to be aligned to appear to have a single origin, also known as 'zero-angle' x-ray radiation.

X-ray sources using linear accumulation

A compact source for high brightness x-ray generation is disclosed. The higher brightness is achieved through electron beam bombardment of multiple regions aligned with each other to achieve a linear accumulation of x-rays. This may be achieved by aligning discrete x-ray sub-sources, or through the use of x-ray targets that comprise microstructures of x-ray generating materials fabricated in close thermal contact with a substrate with high thermal conductivity. This allows heat to be more efficiently drawn out of the x-ray generating material, and in turn allows bombardment of the x-ray generating material with higher electron density and/or higher energy electrons, leading to greater x-ray brightness. Some embodiments of the invention comprise x-ray optical elements placed between sub-sources of x-rays. These x-ray optical elements may form images of one or more x-ray sub-sources in alignment with other x-ray sub-sources, and may enhance the linear accumulation that can be achieved.

The present invention relates to cost effective production methods of high efficiency silicon based back-contacted back-junction solar panels and solar panels thereof having a multiplicity of alternating rectangular emitter- and base regions on the back-side of each cell, each with rectangular metallic electric finger conductor above and running in parallel with the corresponding emitter- and base region, a first insulation layer in-between the wafer and finger conductors, and a second insulation layer in between the finger conductors and cell interconnections.

Back junction back contact solar cell module and method of manufacturing the same

The present invention relates to cost effective methods for metallization and or metallization and interconnection of high efficiency silicon based back-contacted back-junction solar panels and solar panels thereof having a multiplicity of alternating rectangular emitter- and base regions on the back-side of each cell, each with rectangular metallic electric finger conductor above and running in parallel with the corresponding emitter- and base region, a first insulation layer in-between the wafer and finger conductors, and a second insulation layer in between the finger conductors and cell interconnections.

Method for metallization or metallization and interconnection of back contact solar cells

A compound zone plate comprising a first zone plate frame including a first zone plate, a second zone plate frame including a second zone plate, and a base frame to which the first zone plate frame and the second zone plate frame are bonded. In examples, two more zone plates are added to make a four element optic. In the assembly process, the microbeads are used to ensure the parallelism, dial in the distance precisely between the zone plates by selecting the microbead size, possibly in response to the width of the frames, and ensure low friction lateral movement enabling nanometer precision alignment of the zone plates with respect to each other prior to being fixed by the adhesive. That is, when the frames are pressed together to ensure parallelism, it is still possible to align them to each other since the microbead layer facilitates the inplane movement of the alignment process.

Compound x-ray lens having multiple aligned zone plates

Compound X-ray lens having multiple aligned zone plates

A metrology system that uses an imaging system to monitor alignment features on the sample or sample holder of an X-ray laminography or tomography system. the metrology system has the capability to provide both sample shift and sample rotation movement data to a data acquisition system. These shift and rotation data can be used in alignment routines to produce 3D reconstructions from the X-ray images/projections. The metrology system is based on an imaging and focusing measurement of intrinsic feature of the sample or artificial features fabricated on the sample or sample holder.

Metrology and registration system and method for laminography and tomography

A method to stabilize planar nanostructures, for example grating and zone plate lenses that are typically used for directing or focusing x-ray radiation, includes the deposition of a top, stabilizing layer. The structures are typically made on a flat substrate, and therefore are only fixed at the bottom. At high aspect ratio, the stability can be poor since small forces such as electrostatic forces and van de Waals forces that are often present can alter the structure. The top coating of a metallic material such as titanium constrains the nanostructures at the top and at the same time eliminates electrostatic forces and reduces any thermal gradient that may be present across the device.

Growing community of inventors

Berkeley, CA, United States of America

Alan Francis Lyon