Material Analysis Using Wave/Particle Radiation TRIZ Cases

Segmented injection ports and diverters in a super-stage optimize fracturing efficiency while reducing the number of stages required.

A radiation detector uses an inert gas filled closed space to protect circuit elements from deterioration.

Interconnected blade fins in a 2D collimator assembly resolve mechanical instability and scatter rejection challenges in wide-area CT scanning.

Estimates background radiation using measured and simulated data offsets to separate primary and scatter components in cone-beam computed tomography.

An X-ray analysis device uses an energy-dependent filter to block low-energy radiation before the capillary lens focuses the beam.

Processing circuitry predicts artifacts for candidate X-ray tube tracks using two-dimensional images to guide operator selection.

A time-resolved imaging system dynamically adjusts a C-arm position to maintain an optimal view of moving anatomical structures.

A detector module uses a sealed cover assembly with integrated cooling channels to circulate refrigerant and maintain uniform component temperatures.

Defining the first derivative as a polynomial solves image registration errors caused by sample drift and spatial quantization noise in particle-optical lenses.

A vitrification apparatus positions a biological sample on a pin and moves it along an inclined path to a liquefied gas bath.

Multi-band photo-acoustic detection replaces complex NDIR optics with acoustic signals, resolving low-ppm ammonia measurement precision issues.

A CT scanner control system dynamically adjusts conveyor and gantry speeds to switch between scanning pitch modes.

Automated FIB sectioning eliminates manual alignment workload while maintaining high-resolution 3D reconstruction accuracy.

A rotatable cutting bevel adjusts orientation within a cutting plane to maintain perpendicular alignment with the particle beam axis.

A surface analyzer generates polygonal cluster region boundaries from scatter diagram data to streamline analyst workflows.

Electronic beamforming replaces mechanical collimators to consolidate radiation for precise imaging.

Segmented detector elements with finite gaps create an irregular active area, eliminating dead space while supporting fan and cone beam imaging modes.

A multi-source cone beam computed tomography apparatus uses rotating divergent radiation beams to capture and stitch high-resolution images.

E-beam array irradiators and detectors inspect mask patterns while calculating positional offsets for registration accuracy.

A pixel-by-pixel lookup table corrects thermal gain drift in x-ray detectors using diode temperature measurements, eliminating ring artifacts from CT scans.

A rock permeability estimation process segments volume-based aspect ratio distributions into discrete pore types for accurate characterization.

A charged particle beam apparatus measures electron current density distributions to determine optimal probe positions.

A solution/non-recrystallization heat treatment relaxes internal strain in gamma phase crystal grains of used turbine components.

X-ray backscatter imaging detects Compton signals to estimate crop weight, bypassing foliage occlusion limits of visual sensors.

Computer subsystems overlay design information with detected defects to select representative samples from semiconductor array regions.

An adjustable collimator focuses x-ray beams on breast regions of interest, reducing radiation scatter and noise that degrade conventional projection images.

Flexible vacuum bellows and interlocking shields separate HAXPES chambers to block X-ray leakage while allowing independent positioning of the source.

Photoelectron spectroscopy measures core and shell binding energies to determine precise band structures in semiconductor nanoparticles.

A data analysis device calculates relative concentration profiles using angle-resolved photoelectron spectroscopy signals.

A divergent polychromatic X-ray beam generates multiple diffractions for rapid three-dimensional grain structure reconstruction.

A segmented acquisition method triggers image capture during specific breathing phases to reconstruct sharp 3D x-ray data.

Auxiliary dot sequences detect pattern tracks to calculate inclination angles, enabling high-accuracy measurements that suppress edge roughness influence.

Virtual diffraction frames process electron intensities with dynamical theory, resolving measurement precision issues in non-precession data.

Gas-phase deposition connects a specimen carrier to a sample across a gap, preventing misalignment during welding.

Electronic beam steering replaces mechanical parts to eliminate sampling gaps and overlaps during vehicle inspection.

Inclined gantry rotation plane directs X-ray beams at an angle to the intervention axis, minimizing scattered radiation from metallic instruments.

Radiographic scans identify internal log orientation, resolving recognition failures on smooth surfaces.

A pulser injects calibration pulses into X-ray detection electronics to stabilize gain and energy scale accuracy.

A CT detector module interconnect system uses wire bonds and bump bonds to connect sensor elements directly to integrated circuits.

Ozone oxidizes hydrocarbon contaminants into volatile products pumped away, restoring image contrast and resolution.

Motion correction algorithms process multiple low-dose fluoroscopy frames into a single enhanced image, eliminating the need for high-radiography exposures.

Dual-energy CT imaging acquires two x-ray images at different energy levels to isolate iron deposits within arterial plaques.

Dual helium gas introduction ports eliminate organic films to prevent X-ray absorption and improve analysis precision.

Condensing spectral data during acquisition delivers preliminary composition results without waiting for full hyperspectral cube completion.

Inverting layered samples enables dual-surface X-ray fluorescence measurements to extract multiple independent intensity values.

A processing device performs angular Fourier decomposition on small angle scattering images to determine the tilt angle of substrate structures.

A nondestructive method calculates wafer damage depth by matching simulated and measured X-ray rocking curves.