G01N2223/6116

X-RAY FLUORESCENCE ANALYZER
20220404297 · 2022-12-22 · ·

In order to provide an X-ray fluorescence analyzer that can accurately obtain a concentration of an element to be measured by generating a fluorescent X-ray only from an element to be measured or generating a very small amount of fluorescent X-ray from an element to be excluded, even in the case where, for example, atomic numbers of a plurality of elements contained in a liquid sample are close to each other such as in phosphorus (P) and silicon (Si), an X-ray fluorescence analyzer is configured to analyze a liquid sample containing a first element to be measured and a second element having the atomic number larger than the atomic number of the first element, the X-ray fluorescence analyzer including: an X-ray source that emits a first X-ray; a secondary target that generates the second X-ray by being excited by the first X-ray; a detector and a concentration calculator.

LARGE DIE WAFER, LARGE DIE AND METHOD OF FORMING THE SAME
20220399282 · 2022-12-15 ·

The present invention provides a large die, a method of forming the large die and a large die wafer. The method includes: providing a wafer containing a plurality of large dies each having a size greater than that of a maximum field of exposure of a stepper, each large die including at least two die portions to be stitched together, the die portions including a substrate and a first metal layer, the first metal layer including at least to-be-interconnected metal layers for interconnection of the die portions; and forming a second metal layer including at least inter-die interconnecting metal layers crossing dummy dicing margins between adjacent die portions and coming into electrical connection with the to-be-interconnected metal layers of the adjacent die portions. The present invention allows interconnection of the die portions to be stitched together in each large die.

SEGMENTED MULTI-CHANNEL, BACKSIDE ILLUMINATED, SOLID STATE DETECTOR WITH A THROUGH-HOLE FOR DETECTING SECONDARY AND BACKSCATTERED ELECTRONS

A segmented detector device with backside illumination. The detector is able to collect and differentiate between secondary electrons and backscatter electrons. The detector includes a through-hole for passage of a primary electron beam. After hitting a sample, the reflected secondary and backscatter electrons are collected via a vertical structure having a P+/P−/N+ or an N+/N−/P+ composition for full depletion through the thickness of the device. The active area of the device is segmented using field isolation insulators located on the front side of the device.

SNR for x-ray detectors in SEM systems by using polarization filter
11525791 · 2022-12-13 · ·

A method of performing x-ray spectroscopy surface material analysis of a region of interest of a sample with an evaluation system that includes a scanning electron microscope (SEM) column, an x-ray detector and an x-ray polarizer, comprising: positioning a sample within a field of view of the scanning electron microscope; generating an electron beam having a landing energy about equal to an ionization energy of the materials within the region of interest of the sample; scanning the region of interest with the electron beam set to collide with the sample thereby generating x-rays emitted from near a surface of the sample, the x-rays including characteristic x-rays and Bremsstrahlung radiation; and detecting x-rays generated while the region of interest is scanned by the electron after the x-rays pass through the x-ray polarizer that blocks a higher percentage of the Bremsstrahlung radiation than the characteristic x-rays.

METHOD AND APPARATUS FOR EFFICIENT HIGH HARMONIC GENERATION
20220390388 · 2022-12-08 · ·

A high harmonic radiation source and associated method of generating high harmonic radiation is disclosed. The high harmonic radiation source is configured to condition a gas medium by irradiating the gas medium with a pre-pulse of radiation, thereby generating a plasma comprising a pre-pulse plasma distribution; and irradiate the gas medium with a main pulse of radiation to generate said high harmonic radiation. The conditioning step is such that the plasma comprising a pre-pulse plasma distribution acts to configure a wavefront of said main pulse to improve one or both of: the efficiency of the high harmonic generation process and the beam quality of the high harmonic radiation. The high harmonic radiation source further may comprise a beam shaping device configured to shape said customized pre-pulse prior to said conditioning.

Transmission small-angle X-ray scattering metrology system

Methods and systems for characterizing dimensions and material properties of semiconductor devices by transmission small angle x-ray scatterometry (TSAXS) systems having relatively small tool footprint are described herein. The methods and systems described herein enable Q space resolution adequate for metrology of semiconductor structures with reduced optical path length. In general, the x-ray beam is focused closer to the wafer surface for relatively small targets and closer to the detector for relatively large targets. In some embodiments, a high resolution detector with small point spread function (PSF) is employed to mitigate detector PSF limits on achievable Q resolution. In some embodiments, the detector locates an incident photon with sub-pixel accuracy by determining the centroid of a cloud of electrons stimulated by the photon conversion event. In some embodiments, the detector resolves one or more x-ray photon energies in addition to location of incidence.

Methods and systems for real time measurement control
11519869 · 2022-12-06 · ·

Methods and systems for improving a measurement recipe describing a sequence of measurements employed to characterize semiconductor structures are described herein. A measurement recipe is repeatedly updated before a queue of measurements defined by the previous measurement recipe is fully executed. In some examples, an improved measurement recipe identifies a minimum set of measurement options that increases wafer throughput while meeting measurement uncertainty requirements. In some examples, measurement recipe optimization is controlled to trade off measurement robustness and measurement time. This enables flexibility in the case of outliers and process excursions. In some examples, measurement recipe optimization is controlled to minimize any combination of measurement uncertainty, measurement time, move time, and target dose. In some examples, a measurement recipe is updated while measurement data is being collected. In some examples, a measurement recipe is updated at a site while data is collected at another site.

Measurement and control of wafer tilt for x-ray based metrology

Methods and systems for measuring the orientation of a wafer at or near an X-ray scatterometry measurement location are described herein. In one aspect, an X-ray scatterometry based metrology system includes a wafer orientation measurement system that measures wafer orientation based on a single measurement without intervening stage moves. In some embodiments, an orientation measurement spot is coincident with an X-ray measurement spot. In some embodiments, an X-ray scatterometry measurement and a wafer orientation measurement are performed simultaneously. In another aspect, signals detected by a wafer orientation measurement system are filtered temporally, spatially, or both, to improve tracking. In another aspect, a wafer orientation measurement system is calibrated to identify the orientation of the wafer with respect to an incident X-ray beam. In another aspect, a wafer under measurement is positioned based on the measured orientation in a closed loop or open loop manner.

SYSTEMS AND METHODS FOR VOLTAGE CONTRAST DEFECT DETECTION

Systems and methods of providing a probe spot in multiple modes of operation of a charged-particle beam apparatus are disclosed. The method may comprise activating a charged-particle source to generate a primary charged-particle beam and selecting between a first mode and a second mode of operation of the charged-particle beam apparatus. In the flooding mode, the condenser lens may focus at least a first portion of the primary charged-particle beam passing through an aperture of the aperture plate to form a second portion of the primary charged-particle beam, and substantially all of the second portion is used to flood a surface of a sample. In the inspection mode, the condenser lens may focus a first portion of the primary charged-particle beam such that the aperture of the aperture plate blocks off peripheral charged-particles to form the second portion of the primary charged-particle beam used to inspect the sample surface.

Thin film analyzing device and thin film analyzing method

A thin film analyzing device includes a processing and analyzing chamber for performing processing and analyzing of a subject having a thin film on a substrate. The processing and analyzing chamber includes a sample holder arranged to hold the subject, an X-ray irradiation source arranged to irradiate the subject with X-rays, a fluorescent X-ray detector configured to detect fluorescent X-rays which are emitted from the subject, a diffracted/reflected X-ray detector configured to detect reflected X-rays and diffracted X-rays which are emitted from the subject, and a substrate remover arranged to remove the substrate.