The Boeing Company

Theboeing Company

John L Adamski

Richard Henry Bossi

Clarence Lavere Gordon, Iii

William G Bartholet

Benjamin Emerson Carl Koltenbah

James M Nelson

A method and apparatus for identifying and tagging a target, such an individual or an item, are described that provide an improved mechanism for identifying the target without alerting the target. In this regard, a method and apparatus can irradiate the target so as to create a radioisotope signature for the target. By thereafter monitoring the radioisotope signature, the target can be identified and tracked in a covert manner.

Method and apparatus for tagging and identifying a target

An apparatus for merging a low energy electron flow into a high energy electron flow may include: a high energy electron path for accommodating the high energy electron flow; and a plurality of magnetic elements arranged to guide the low energy electron flow through a chicane presenting a path having a first end and a second end. The path intersects the high energy electron path at the second end. The path has a plurality of turns and path segments intermediate the first and second ends. Respective adjacent path segments intersect at each respective turn. The path establishes a respective bend radius and subtends a respective path angle between respective adjacent path segments at each respective turn. Each respective path angle is maximized within predetermined path angle limits. Each respective bend radius is minimized within predetermined bend radius limits.

Apparatus and method for merging a low energy electron flow into a high energy electron flow

A method and apparatus for measuring a structure. An x-ray system and the structure are positioned relative to each other. The x-ray system comprises a gas source configured to provide a gas, a laser system configured to emit a laser beam, a steering system, and a detector. The steering system is configured to direct a first portion of the laser beam into the gas such that an electron beam is generated by the laser beam interacting with the gas and is configured to direct a second portion of the laser beam into the electron beam such that a collimated x-ray beam is formed. The detector is configured to detect the collimated x-ray beam. The collimated x-ray beam is emitted with the structure positioned relative to the x-ray system.

Tangent radiography using brilliant x-ray source

A method and apparatus, such as a spectrometer, are provided for facilitating the detection of an gamma signal in a manner that effectively discriminates the gamma signal from noise. A spectrometer may be provided which includes an gamma converter for converting gamma signals which impinge thereupon into corresponding pairs of electrons and positrons. The spectrometer also includes a deflector for separately deflecting the electrons and the positrons as well as electron and positron detectors for separately detecting the deflected electrons and positrons, respectively. As such, an gamma signal can be identified in instances in which the deflected electrons and positrons are detected in coincidence.

Method and apparatus for detecting x-rays having improved noise discrimination

A method and apparatus for multi-energy object inspection using a brilliant x-ray source. A first mono-energetic x-ray image of an object at a first selected energy is generated. A second mono-energetic x-ray image of the object at a second selected energy is generated. The first selected energy is different than the second selected energy. Additional mono-energetic x-ray images may be generated at energies different than previous energies up to n selected energies. The mono-energetic x-ray images are mathematically combined and processed to form a result. The result of processing the mono-energetic x-ray images is presented. The result comprises processed mono-energetic x-ray image data describing materials in the object with greater sensitivity, identifying the layers, and identifying the material composition than in the first image or the second image.

Multi-energy radiography using monoenergetic pulsed source

A system for imaging in a structure may include an energy beam source to direct an energy beam at the structure and a detector to detect a backscatter of the energy beam from any object in the structure. The system may also include a time-resolved function to generate an image of any object in the structure using the backscatter of the energy beam.

Energy beam pulse echo system for imaging in a structure

A terahertz imaging system uses a terahertz light source to illuminate a target object with a series of short pulses of terahertz light. The pulses have a low average output power but a high peak output power, thereby enabling imaging of the suspicious object or person at a safe distance while avoiding injury to the person being imaged. For each pulse, the reflection of the light is imaged by a detector array. The terahertz light pulses are individually narrow band and the emitted pulse train is rapidly tuned in wavelength across a wide frequency range in the terahertz band. Within the terahertz frequency range, molecules have unique absorption spectra. The energy reflected from the illuminated threat object is measured for each of the discrete narrow frequency bands and compared to the absorption spectra of known dangerous materials to determine whether the threat object contains or carries a known dangerous material.

Terahertz imaging system and associated method

The electrode is circular in configuration, with a central opening, so that it has inner and outer rims. The electrode structure comprises a plurality of spiral-shaped vanes of conducting material which are separated by relatively thin slit-like openings. The spiral vanes begin at an inner boundary which is close to the inner rim of the electrode and rotate approximately one-half turn to the outer rim of the electrode. A portion of the electron beam, which is typically produced from a cathode energized by a high voltage source, strikes the electrode near the central opening, and travels along the vanes of the electrode to ground, thereby establishing a plurality of spiral current paths in the electrode. These spiral currents create a magnetic field about the center of the anode in the region of the electron beam, focusing the remainder of electron beam through the opening in the electrode.

Electrode having spiral-shaped electrically conducting regions therein

The accelerator includes a source of an ensemble or bunch of ions and a plurality of relatavistic electron beam stages, each of which generate a high current electron beam which in turn are injected along the accelerator centerline in a timed sequence to accelerate the ion bunch to increasingly high kinetic energy levels. In each relatavistic electron beam stage, a region of high electric charge is created by the discharge of a high current, short duration pulse between a cathode and anode. The electron beam created by the discharge stops a short distance beyond the anode, due to the buildup of its electric charge, thereby creating a region of high charge which accelerates the ion bunch. Each successive relatavistic electron beam stage is timed to fire when the ion bunch arrives at the region of high charge of that stage, and in operation, increases the kinetic energy of the ion bunch by a factor equal to or greater than the kinetic energy of the electron beam.

Growing community of inventors

Kenmore, WA, United States of America

John L Adamski