Hand-held portable backscatter inspection system

Information

  • Patent Grant
  • 11561320
  • Patent Number
    11,561,320
  • Date Filed
    Friday, December 18, 2020
    3 years ago
  • Date Issued
    Tuesday, January 24, 2023
    a year ago
Abstract
The present specification describes a compact, hand-held probe or device that uses the principle of X-ray backscatter to provide immediate feedback to an operator about the presence of scattering and absorbing materials, items or objects behind concealing barriers irradiated by ionizing radiation, such as X-rays. Feedback is provided in the form of a changing audible tone whereby the pitch or frequency of the tone varies depending on the type of scattering material, item or object. Additionally or alternatively, the operator obtains a visual scan image on a screen by scanning the beam around a suspect area or anomaly.
Description
FIELD

The present specification generally relates to a portable backscatter scanning system, and in particular, relates to a system which can be carried by an operator by hand to sites of inspection, including confined locations, and subsequently used to scan for detection of concealed materials and objects.


BACKGROUND

Materials, such as narcotics, explosives or currency, and objects, such as weapons or people, are concealed within or behind barriers with the intention that the materials or objects remain undetected by routine or targeted security checks.


Today, scanning devices are well known which use a variety of sensing methods to detect concealed materials and objects. These scanning devices include transmission X-ray imaging systems, Compton scatter-based backscatter imaging systems, chemical sniffing trace detection equipment, thermal imaging camera systems and so on. Such scanning devices may be used alone or in combination to provide a comprehensive level of security. However, such devices tend either to be large and expensive (e.g. transmission X-ray imaging systems) or insensitive to carefully hidden materials (e.g. trace detection equipment and camera systems) which means that their utility is restricted to certain high throughput situations such as sea ports and land borders, airport checkpoints and so on.


Therefore, what is needed is a compact, light-weight, portable and hand-held system or device that can be maneuvered to reach relatively inaccessible locations and scan behind concealing barriers that are otherwise opaque against chemical and optical probes. Such a system or device should be able to provide immediate feedback if a suspicious material, object or anomaly is detected and should allow an operator to obtain information about the concealed material or object, for threat resolution, without the need to breach the concealing barrier.


SUMMARY

In some embodiments, the present specification discloses a method for scanning an object by projecting a shaped X-ray beam from a hand-held imaging device, where the device includes a housing enclosing an X-ray tube that emits the shaped X-ray beam, a plurality of detectors for generating scan data corresponding to a plurality of detected X-ray beams scattered from the object, a processor in communication with a gyroscope and an accelerometer, and an acquisition system in communication with a speaker, a display, the processor and the plurality of detectors. In some embodiments, the method includes using the processor for calculating a plurality of active pixels corresponding to a location of interaction of the shaped X-ray beam on the object; using the processor for calculating a time duration, at each of said plurality of active pixels, for which the shaped X-ray beam is present over each of said plurality of active pixels; and using the processor to generate an image, on said display, of the object after correcting the scan data, at each of said plurality of active pixels, using said time duration.


In some embodiments, the shaped X-ray beam is a pencil beam.


In some embodiments, the shaped X-ray beam is a cone beam.


In some embodiments, the shaped X-ray beam is a fan beam.


In some embodiments, the shaped X-ray beam is a single-axis rotating beam.


In some embodiments, the shaped X-ray beam is a dual-axis rotating beam.


In some embodiments, the hand-held imaging device is swept to scan the object using a coarse scanning pattern to identify at least one anomaly, with reference to the object, prior to calculating said plurality of active pixels, calculating said time duration and generating said image. Optionally, the anomaly is identified based on a change in audible tone generated by the speaker. Optionally, the processor and speaker are adapted to generate said audible tone such that a pitch or frequency of said audible tone varies in proportion to said scan data.


Optionally, upon identification of said at least one anomaly, the hand-held imaging device is swept to scan the object using a fine scanning pattern for calculating said plurality of active pixels, calculating said time duration and generating said image.


In some embodiments, the processor receives second data which is generated by the accelerometer and is indicative of a movement of the shaped X-ray beam being projected on the object. In some embodiments, the method includes based on said second data: using the processor for calculating a plurality of active pixels corresponding to a new location of interaction of the shaped X-ray beam on the object; using the processor for calculating a time duration, at each of said plurality of active pixels, for which the shaped X-ray beam is present over each of said plurality of active pixels; and using the processor for generating an updated image, on said display, of the object after correcting the scan data, at each of said plurality of active pixels, using said time duration.


In some embodiments, the new location is associated with an updated first data generated by the gyroscope, and wherein said updated first data is indicative of a new direction of the shaped X-ray beam being projected on the object.


In some embodiments, the acquisition system sums said detected scan data over a sampling duration ranging between 0.01 ms and 100 ms.


In some embodiments, the acquisition system sums said detected scan data over a sampling duration of 1 ms.


In some embodiments, a voltage of the X-ray tube ranges between 30 kV and 100 kV.


In some embodiments, a current of the X-ray tube ranges between 0.1 mA and 5 mA.


In some embodiments, the location is associated with a first data generated by the gyroscope, and wherein said first data is indicative of a direction of the shaped X-ray beam being projected on the object.


In some embodiments, the present specification discloses a system for a hand-held imaging device for scanning an object by projecting a shaped X-ray beam. In some embodiments, the system includes a housing having a central longitudinal axis and including: a plurality of detectors for generating scan data corresponding to a plurality of detected X-ray beams scattered from the object; a gyroscope; an accelerometer; an acquisition system in communication with a display and said plurality of detectors; and a processor in communication with said gyroscope, said accelerometer and said acquisition system. In some embodiments, said processor is configured for: calculating a plurality of active pixels corresponding to a location of interaction of the shaped X-ray beam on the object; calculating a time duration, at each of said plurality of active pixels, for which the shaped X-ray beam is present over each of said plurality of active pixels; and generating an image, on said display, of the object after correcting the scan data, at each of said plurality of active pixels, using said time duration.


In some embodiments, the shaped X-ray beam is a pencil beam.


In some embodiments, the shaped X-ray beam is a cone beam.


In some embodiments, the shaped X-ray beam is a fan beam.


In some embodiments, the shaped X-ray beam is a single-axis rotating beam.


In some embodiments, the shaped X-ray beam is a dual-axis rotating beam.


In some embodiments, the housing has an upper surface, a base opposite and parallel to said upper surface, a front surface, a rear surface opposite and parallel to said front surface, a first side and a second side opposite and parallel to said first side, and wherein said upper surface has at least one handle. Optionally, the housing is configured as a first cuboid, bearing said front surface, which tapers along the central longitudinal axis into a trapezoidal prism culminating in said rear surface.


Optionally, the shaped X-ray beam emerges through an opening at a center of said front surface in a direction substantially perpendicular to said front surface. Optionally, the plurality of detectors are positioned adjacent to and behind said front surface surrounding said opening at the center of said front surface.


In some embodiments, the system includes a speaker, wherein said processor and speaker are adapted to generate an audible tone such that a pitch or frequency of said audible tone varies in proportion to said scan data.


Optionally, the housing further comprises a plurality of vanes for collimating a plurality of X-ray beams scattered from the object. Optionally, said plurality of vanes are arranged in planes that are substantially parallel to each other. Optionally, said plurality of vanes are arranged in planes that are substantially parallel to each other and in a direction substantially perpendicular to an orientation of a plane of a fan beam. Optionally, said plurality of vanes is arranged in planes in a substantially diverging orientation with respect to each other. Optionally, said plurality of vanes is arranged in planes in a substantially converging orientation with respect to each other.


Optionally, the housing further comprises a grid of a plurality of collimator elements for collimating a plurality of X-ray beams scattered from the object. Still optionally, said grid comprises first and second sets of a plurality of combs, each of said plurality of combs having teeth, wherein the teeth of said first set of combs in a first direction interlock with the teeth of said second set of combs in a second direction, and wherein said second direction is substantially orthogonal to said first direction. Optionally, said teeth are arranged in planar directions substantially parallel to an orientation of said shaped X-ray beam. Still optionally, said teeth are arranged in planar directions substantially parallel to each other. Optionally, said teeth are arranged in planar orientations that are substantially divergent with respect to each other. Optionally, said teeth are arranged in planar orientations that are substantially convergent with respect to each other. Optionally, each of said plurality of detectors maps to an area on the object, wherein said area is defined by a solid angle of a cone beam and an acceptance angle of each of said plurality of collimator elements.


Optionally, the housing further comprises a first rotating collimator having a first transmission pattern and a second rotating collimator having a second transmission pattern, said first and second transmission patterns defining said shaped X-ray beam. Optionally, said first transmission pattern defines a radial position of a pencil beam while said second transmission pattern defines an azimuthal angle of said pencil beam. Optionally, said first and second collimators rotate in lock step with each other, and wherein said first collimator rotates at a first speed while said second collimator rotates at a second speed. Optionally, said second speed is greater than said first speed. Optionally, said first and second collimators are substantially circular disks having differing radii. Optionally, said first and second collimators are substantially circular disks having equal radii. Optionally, said first transmission pattern is a slit extending in a spirally curved configuration from a point proximate to a center point of said first collimator to a point proximate to a circumference of said first collimator, and wherein said second transmission pattern is a slit extending radially from a point proximate to a center of said second collimator to a point proximate to a circumference of said second collimator.


Optionally, said housing further comprises a rotating collimator having a transmission pattern defining the shaped X-ray beam, the rotating collimator supported and partially surrounded by an oscillating shaped cradle. Optionally, said collimator rotates at a speed ranging between 100 to 5000 RPM. Optionally, said collimator rotates at a speed of 2000 RPM. Optionally, said rotating collimator causes said shaped X-ray beam to sweep a trajectory in a substantially vertical plane such that a focal spot of said shaped X-ray beam is in a plane of said rotating collimator and on a central longitudinal axis of said housing, and wherein said oscillating shaped cradle causes said shaped X-ray beam to sweep left to right, repeatedly, over said substantially vertical plane. Optionally, said collimator is a substantially circular disk having a first radius while said shaped cradle is substantially semi-circular having a second radius, and wherein said second radius is greater than said first radius. Optionally, said collimator is a substantially circular disk having a radius while said shaped cradle is substantially ‘U’ or ‘C’ shaped. Optionally, said transmission pattern is an opening at a point between a center and a circumference of said collimator, and wherein said rotating and oscillating movements together cause said shaped X-ray beam to move in a raster pattern over a two dimensional area of the object.


In some embodiments, the present specification is directed toward a method of scanning an object by projecting a shaped X-ray beam from a hand-held imaging device. In some embodiments, the device includes a housing enclosing an X-ray tube that emits the shaped X-ray beam, a plurality of detectors for generating scan data corresponding to a plurality of detected X-ray beams scattered from the object, a processor in communication with a gyroscope and an accelerometer, and an acquisition system in communication with a speaker, a display, said processor and said plurality of detectors. In some embodiments, the method incudes receiving first data by the processor, wherein said first data is generated by the gyroscope and is indicative of a direction of the shaped X-ray beam being projected on the object; using the processor for calculating a plurality of active pixels corresponding to a location of interaction of the shaped X-ray beam on the object, wherein said location is associated with said first data; using the processor for calculating a time duration, at each of said plurality of active pixels, for which the shaped X-ray beam is present over each of said plurality of active pixels; and using the processor for generating an image, on said display, of the object after correcting the scan data, at each of said plurality of active pixels, using said time duration.


In some embodiments, the shaped X-ray beam is in the form of a pencil beam.


In some embodiments, the hand-held imaging device is swept to scan the object using a coarse scanning pattern to identify at least one anomaly, with reference to the object, prior to receiving said first data, calculating said plurality of active pixels, calculating said time duration and generating said image. Optionally, the anomaly is identified based on a change in audible tone generated by the speaker. Still optionally, a pitch or frequency of said audible tone is proportional to said generated scan data.


Optionally, upon identification of said at least one anomaly, the hand-held imaging device is swept to scan the object using a fine scanning pattern for receiving said first data, calculating said plurality of active pixels, calculating said time duration and generating said image. Optionally, the method further includes receiving second data by the processor, wherein said second data is generated by the accelerometer and is indicative of a movement of the shaped X-ray beam being projected on the object. In some embodiments, based on said second data, the method includes receiving updated first data by the processor indicative of a new direction of the shaped X-ray beam being projected on the object; using the processor for calculating a plurality of active pixels corresponding to a location of interaction of the shaped X-ray beam on the object, wherein said location is associated with said updated first data indicative of the new direction; using the processor for calculating a time duration, at each of said plurality of active pixels, for which the shaped X-ray beam is present over each of said plurality of active pixels; and using the processor for generating an updated image, on said display, of the object after correcting the scan data, at each of said plurality of active pixels, using said time duration.


In some embodiments, the acquisition system sums said detected scan data over a sampling duration ranging between 0.01 ms and 100 ms.


In some embodiments, the acquisition system sums said detected scan data over a sampling duration of 1 ms.


In some embodiments, a voltage of the X-ray tube ranges between 30 kV and 100 kV.


In some embodiments, a current of the X-ray tube ranges between 0.1 mA and 5 mA.


In some embodiments, the present specification is directed towards a system for a hand-held imaging device for scanning an object by projecting a shaped X-ray beam, where the device includes a housing having a central longitudinal axis. In some embodiments, the housing includes a plurality of detectors for generating scan data corresponding to a plurality of detected X-ray beams scattered from the object; a gyroscope; an accelerometer; an acquisition system in communication with a speaker, a display and said plurality of detectors; and a processor in communication with said gyroscope, said accelerometer and said acquisition system. In some embodiments, said processor is configured for receiving first data generated by the gyroscope and indicative of a direction of the shaped X-ray beam being projected on the object; calculating a plurality of active pixels corresponding to a location of interaction of the shaped X-ray beam on the object, wherein said location is associated with said first data; calculating a time duration, at each of said plurality of active pixels, for which the shaped X-ray beam is present over each of said plurality of active pixels; and generating an image, on said display, of the object after correcting the scan data, at each of said plurality of active pixels, using said time duration.


In some embodiments, the shaped X-ray beam is in the form of a pencil beam.


In some embodiments, the housing has an upper surface, a base opposite and parallel to said upper surface, a front surface, a rear surface opposite and parallel to said front surface, a first side and a second side opposite and parallel to said first side, and wherein said upper surface has at least one handle. Optionally, the housing is configured as a first cuboid, bearing said front surface, which tapers along the central longitudinal axis into a second cuboid culminating in said rear surface. Optionally, the shaped X-ray beam emerges through an opening at a center of said front surface in a direction substantially perpendicular to said front surface. Optionally, the plurality of detectors are positioned adjacent to and behind said front surface surrounding said opening at the center of said front surface. Optionally, there are four sets of detectors.


In some embodiments, the present specification is directed towards a method of scanning an object by projecting a shaped X-ray beam from a hand-held imaging device. In some embodiments, the device includes a housing enclosing an X-ray tube that emits the shaped X-ray beam, a plurality of vanes for collimating a plurality of X-ray beams scattered from the object, a plurality of detectors for generating scan data corresponding to the plurality of collimated X-ray beams detected by said plurality of detectors, a processor in communication with a gyroscope and an accelerometer, and an acquisition system in communication with a speaker, a display, said processor and said plurality of detectors. In some embodiments, the method includes using the processor for calculating a plurality of active pixels corresponding to a location of interaction of the shaped X-ray beam on the object; using the processor for calculating a time duration, at each of said plurality of active pixels, for which the shaped X-ray beam is present over each of said plurality of active pixels; and using the processor for generating an image, on said display, of the object after correcting the scan data, at each of said plurality of active pixels, using said time duration.


In some embodiments, the shaped X-ray beam is in the form of a fan beam.


In some embodiments, the hand-held imaging device is swept to scan the object using a coarse scanning pattern to identify at least one anomaly, with reference to the object, prior to calculating said plurality of active pixels, calculating said time duration and generating said image. Optionally, the one anomaly is identified based on a change in audible tone generated by the speaker. Still optionally, a pitch or frequency of said audible tone is proportional to said generated scan data. Optionally, upon identification of said at least one anomaly, the hand-held imaging device is swept to scan the object using a fine scanning pattern for calculating said plurality of active pixels, calculating said time duration and generating said image. Still optionally, the method further includes receiving second data by the processor, wherein said second data is generated by the accelerometer and is indicative of a movement of the shaped X-ray beam being projected on the object and wherein based on said second data using the processor for calculating a plurality of active pixels corresponding to a new location of interaction of the shaped X-ray beam on the object; using the processor for calculating a time duration, at each of said plurality of active pixels, for which the shaped X-ray beam is present over each of said plurality of active pixels; and using the processor for generating an updated image, on said display, of the object after correcting the scan data, at each of said plurality of active pixels, using said time duration. Optionally, the new location is associated with an updated first data generated by the gyroscope, and wherein said updated first data is indicative of a new direction of the shaped X-ray beam being projected on the object.


In some embodiments, the acquisition system sums said detected scan data over a sampling duration of 1 ms.


In some embodiments, a voltage of the X-ray tube ranges between 30 kV and 100 kV.


In some embodiments, a current of the X-ray tube ranges between 0.1 mA and 5 mA.


In some embodiments, the location is associated with a first data generated by the gyroscope, and wherein said first data is indicative of a direction of the shaped X-ray beam being projected on the object.


In some embodiments, the present specification discloses a system for a hand-held imaging device for scanning an object by projecting a shaped X-ray beam, where the device includes a housing having a central longitudinal axis. In some embodiments, the housing includes a plurality of vanes for collimating a plurality of X-ray beams scattered from the object;


a plurality of detectors for generating scan data corresponding to the plurality of collimated X-ray beams detected by said plurality of detectors; a gyroscope; an accelerometer; an acquisition system in communication with a speaker, a display and said plurality of detectors; and a processor in communication with said gyroscope, said accelerometer and said acquisition system. In some embodiments, the processor is configured for calculating a plurality of active pixels corresponding to a location of interaction of the shaped X-ray beam on the object; calculating a time duration, at each of said plurality of active pixels, for which the shaped X-ray beam is present over each of said plurality of active pixels; and generating an image, on said display, of the object after correcting the scan data, at each of said plurality of active pixels, using said time duration.


In some embodiments, the shaped X-ray beam is in the form of a fan beam.


In some embodiments, the hand-held imaging device is swept to scan the object using a coarse scanning pattern to identify at least one anomaly, with reference to the object, prior to said processor calculating said plurality of active pixels, calculating said time duration and generating said image. Optionally, the anomaly is identified based on a change in audible tone generated by the speaker. Still optionally, a pitch or frequency of said audible tone is proportional to said generated scan data. Optionally, upon identification of said at least one anomaly, the hand-held imaging device is swept to scan the object using a fine scanning pattern for calculating said plurality of active pixels, calculating said time duration and generating said image.


In some embodiments, the housing has an upper surface, a base opposite and parallel to said upper surface, a front surface, a rear surface opposite and parallel to said front surface, a first side and a second side opposite and parallel to said first side, and wherein said upper surface has at least one handle. Optionally, the housing is configured as a first cuboid, bearing said front surface, which tapers along the central longitudinal axis into a second cuboid culminating in said rear surface. Optionally, the shaped X-ray beam emerges through an opening at a center of said front surface in a direction substantially perpendicular to said front surface. Optionally, the plurality of detectors are positioned adjacent to and behind said front surface surrounding said opening at the center of said front surface, and wherein said plurality of vanes are positioned in front of said plurality of detectors and behind said front surface.


In some embodiments, the plurality of detectors include four sets of detectors.


In some embodiments, planes of said plurality of vanes are arranged in a direction substantially perpendicular to an orientation of a plane of said fan beam. Optionally, planes of said plurality of vanes are arranged one of substantially parallel to each other, in a substantially diverging orientation with respect to each other, and in a substantially converging orientation with respect to each other.


In some embodiments, the present specification discloses a method for scanning an object by projecting a shaped X-ray beam from a hand-held imaging device. In some embodiments, the device includes a housing enclosing an X-ray tube that emits the shaped X-ray beam, a grid of a plurality of collimator elements for collimating a plurality of X-ray beams scattered from the object, a plurality of detectors for generating scan data corresponding to the plurality of collimated X-ray beams detected by said plurality of detectors, a processor in communication with a gyroscope and an accelerometer, and an acquisition system in communication with a speaker, a display, said processor and said plurality of detectors. In some embodiments, the method includes using the processor for calculating a plurality of active pixels corresponding to a location of interaction of the shaped X-ray beam on the object; using the processor for calculating a time duration, at each of said plurality of active pixels, for which the shaped X-ray beam is present over each of said plurality of active pixels; and using the processor for generating an image, on said display, of the object after correcting the scan data, at each of said plurality of active pixels, using said time duration.


In some embodiments, the shaped X-ray beam is in the form of a cone beam.


In some embodiments, the hand-held imaging device is swept to scan the object using a coarse scanning pattern to identify at least one anomaly, with reference to the object, prior to calculating said plurality of active pixels, calculating said time duration and generating said image. Optionally, the anomaly is identified based on a change in audible tone generated by the speaker. Still optionally, a pitch or frequency of said audible tone is proportional to said generated scan data. Optionally, upon identification of said at least one anomaly, the hand-held imaging device is swept to scan the object using a fine scanning pattern for calculating said plurality of active pixels, calculating said time duration and generating said image. Still optionally, the method further includes receiving second data by the processor, wherein said second data is generated by the accelerometer and is indicative of a movement of the shaped X-ray beam being projected on the object and wherein based on said second data the method includes using the processor for calculating a plurality of active pixels corresponding to a new location of interaction of the shaped X-ray beam on the object; using the processor for calculating a time duration, at each of said plurality of active pixels, for which the shaped X-ray beam is present over each of said plurality of active pixels; and using the processor for generating an updated image, on said display, of the object after correcting the scan data, at each of said plurality of active pixels, using said time duration. Still optionally, the new location is associated with an updated first data generated by the gyroscope, and wherein said updated first data is indicative of a new direction of the shaped X-ray beam being projected on the object.


In some embodiments, the acquisition system sums said detected scan data over a sampling duration ranging between 0.01 ms and 100 ms.


In some embodiments, the acquisition system sums said detected scan data over a sampling duration of 1 ms.


In some embodiments, a voltage of the X-ray tube ranges between 30 kV and 100 kV.


In some embodiments, a current of the X-ray tube ranges between 0.1 mA and 5 mA.


In some embodiments, the location is associated with a first data generated by the gyroscope, and wherein said first data is indicative of a direction of the shaped X-ray beam being projected on the object.


In some embodiments, the present specification discloses a system for a hand-held imaging device for scanning an object by projecting a shaped X-ray beam, where the device includes a housing having a central longitudinal axis and including a grid of a plurality of collimator elements for collimating a plurality of X-ray beams scattered from the object; a plurality of detectors for generating scan data corresponding to the plurality of collimated X-ray beams detected by said plurality of detectors; a gyroscope; an accelerometer; an acquisition system in communication with a speaker, a display and said plurality of detectors; and a processor in communication with said gyroscope, said accelerometer and said acquisition system. In some embodiments, the processor is configured for calculating a plurality of active pixels corresponding to a location of interaction of the shaped X-ray beam on the object; calculating a time duration, at each of said plurality of active pixels, for which the shaped X-ray beam is present over each of said plurality of active pixels; and generating an image, on said display, of the object after correcting the scan data, at each of said plurality of active pixels, using said time duration.


In some embodiments, the shaped X-ray beam is in the form of a cone beam.


In some embodiments, the housing has an upper surface, a base opposite and parallel to said upper surface, a front surface, a rear surface opposite and parallel to said front surface, a first side and a second side opposite and parallel to said first side, and wherein said upper surface has at least one handle. Optionally, the housing is configured as a first cuboid, bearing said front surface, which tapers along the central longitudinal axis into a second cuboid culminating in said rear surface. Optionally, the shaped X-ray beam emerges through an opening at a center of said front surface in a direction substantially perpendicular to said front surface. Optionally, the plurality of detectors are positioned adjacent to and behind said front surface surrounding said opening at the center of said front surface, and wherein said grid is positioned behind said front surface and in front of said plurality of detectors such that at least one of said plurality of detectors is present per said collimator element.


In some embodiments, the grid comprises first and second sets of a plurality of combs, each of said plurality of combs having teeth, wherein the teeth of said first set of combs in a first direction interlock with the teeth of said second set of combs in a second direction, and wherein said second direction is substantially orthogonal to said first direction. Optionally, planes of said teeth are arranged in one of a direction substantially parallel to an orientation of said shaped X-ray beam, substantially parallel to each other, substantially diverging orientation with respect to each other, and substantially converging orientation with respect to each other.


In some embodiments, each of said plurality of detectors maps to an area on the object, wherein said area is defined by a solid angle of said cone beam and an acceptance angle of each of said plurality of collimator elements.


In some embodiments, the present specification discloses a method for scanning an object by projecting a shaped X-ray beam from a hand-held imaging device. In some embodiments, the device includes a housing enclosing an X-ray tube that emits the shaped X-ray beam, a first rotating collimator having a first transmission pattern and a second rotating collimator having a second transmission pattern, said first and second transmission patterns defining said shaped X-ray beam, a plurality of detectors for generating scan data corresponding to a plurality of detected X-ray beams, a processor in communication with a gyroscope and an accelerometer, and an acquisition system in communication with a speaker, a display, said processor and said plurality of detectors. In some embodiments, the method includes using the processor for calculating a plurality of active pixels corresponding to a location of interaction of the shaped X-ray beam on the object; using the processor for calculating a time duration, at each of said plurality of active pixels, for which the shaped X-ray beam is present over each of said plurality of active pixels; and using the processor for generating an image, on said display, of the object after correcting the scan data, at each of said plurality of active pixels, using said time duration.


In some embodiments, the shaped X-ray beam is in the form of a pencil beam. Optionally, the first transmission pattern defines a radial position of said pencil beam while said second transmission pattern defines an azimuthal angle of said pencil beam.


In some embodiments, the hand-held imaging device is swept to scan the object using a coarse scanning pattern to identify at least one anomaly, with reference to the object, prior to calculating said plurality of active pixels, calculating said time duration and generating said image. Optionally, the anomaly is identified based on a change in audible tone generated by the speaker. Still optionally, a pitch or frequency of said audible tone is proportional to said generated scan data. Optionally, upon identification of said at least one anomaly, the hand-held imaging device is swept to scan the object using a fine scanning pattern for calculating said plurality of active pixels, calculating said time duration and generating said image.


In some embodiments, the method further includes receiving second data by the processor, wherein said second data is generated by the accelerometer and is indicative of a movement of the shaped X-ray beam being projected on the object and wherein based on said second data the method includes using the processor for calculating a plurality of active pixels corresponding to a new location of interaction of the shaped X-ray beam on the object; using the processor for calculating a time duration, at each of said plurality of active pixels, for which the shaped X-ray beam is present over each of said plurality of active pixels; and using the processor for generating an updated image, on said display, of the object after correcting the scan data, at each of said plurality of active pixels, using said time duration. Optionally, the new location is associated with an updated first data generated by the gyroscope, and wherein said updated first data is indicative of a new direction of the shaped X-ray beam being projected on the object.


In some embodiments, the acquisition system sums said detected scan data over a sampling duration ranging between 0.01 ms and 100 ms.


In some embodiments, the acquisition system sums said detected scan data over a sampling duration of 1 ms.


In some embodiments, a voltage of the X-ray tube ranges between 30 kV and 100 kV.


In some embodiments, a current of the X-ray tube ranges between 0.1 mA and 5 mA.


In some embodiments, the location is associated with a first data generated by the gyroscope, and wherein said first data is indicative of a direction of the shaped X-ray beam being projected on the object.


In some embodiments, the present specification discloses a system for a hand-held imaging device for scanning an object by projecting a shaped X-ray beam, where the device includes a housing having a central longitudinal axis. In some embodiments, the housing includes a first rotating collimator having a first transmission pattern and a second rotating collimator having a second transmission pattern, said first and second transmission patterns defining said shaped X-ray beam; a plurality of detectors for generating scan data corresponding to a plurality of detected X-ray beams; a gyroscope; an accelerometer; an acquisition system in communication with a speaker, a display and said plurality of detectors; and a processor in communication with said gyroscope, said accelerometer and said acquisition system. In some embodiments, the processor is configured for calculating a plurality of active pixels corresponding to a location of interaction of the shaped X-ray beam on the object; calculating a time duration, at each of said plurality of active pixels, for which the shaped X-ray beam is present over each of said plurality of active pixels; and generating an image, on said display, of the object after correcting the scan data, at each of said plurality of active pixels, using said time duration.


In some embodiments, the shaped X-ray beam is in the form of a pencil beam. Optionally, the first transmission pattern defines a radial position of said pencil beam while said second transmission pattern defines an azimuthal angle of said pencil beam.


In some embodiments, the first and second collimators rotate in lock step with each other, and wherein said first collimator rotates at a first speed while said second collimator rotates at a second speed. Optionally, the second speed is greater than said first speed.


In some embodiments, the first and second collimators are substantially circular disks having differing radii.


In some embodiments, the first and second collimators are substantially circular disks having same radii.


In some embodiments, the first transmission pattern is a slit extending in a spirally curved configuration from a point proximate a center of said first collimator to a point proximate a circumference of said first collimator, and wherein said second transmission pattern is a slit extending radially from a point proximate a center of said second collimator to a point proximate a circumference of said second collimator.


In some embodiments, the housing has an upper surface, a base opposite and parallel to said upper surface, a front surface, a rear surface opposite and parallel to said front surface, a first side and a second side opposite and parallel to said first side, and wherein said upper surface has at least one handle. Optionally, the housing is configured as a first cuboid, bearing said front surface, which tapers along the central longitudinal axis into a second cuboid culminating in said rear surface. Optionally, the shaped X-ray beam emerges through an opening at a center of said front surface in a direction substantially perpendicular to said front surface. Optionally, the plurality of detectors are positioned adjacent to and behind said front surface surrounding said opening at the center of said front surface. Optionally, the first collimator is arranged coaxially in front of said second collimator along a central longitudinal axis of said housing, and wherein said first and second collimators are positioned between said opening of said front surface and an opening of said X-ray tube.


In some embodiments, the present specification discloses a method for scanning an object by projecting a shaped X-ray beam from a hand-held imaging device. In some embodiments, the device incudes a housing enclosing an X-ray tube that emits the shaped X-ray beam, a rotating collimator having a transmission pattern defining said shaped X-ray beam, said rotating collimator supported and partially surrounded by an oscillating shaped cradle, a plurality of detectors for generating scan data corresponding to a plurality of detected X-ray beams, a processor in communication with a gyroscope and an accelerometer, and an acquisition system in communication with a speaker, a display, said processor and said plurality of detectors. In some embodiments, the method includes using the processor for calculating a plurality of active pixels corresponding to a location of interaction of the shaped X-ray beam on the object; using the processor for calculating a time duration, at each of said plurality of active pixels, for which the shaped X-ray beam is present over each of said plurality of active pixels; and using the processor for generating an image, on said display, of the object after correcting the scan data, at each of said plurality of active pixels, using said time duration.


In some embodiments, the shaped X-ray beam is in the form of a pencil beam.


In some embodiments, the hand-held imaging device is swept to scan the object using a coarse scanning pattern to identify at least one anomaly, with reference to the object, prior to calculating said plurality of active pixels, calculating said time duration and generating said image. Optionally, the anomaly is identified based on a change in audible tone generated by the speaker. Still optionally, a pitch or frequency of said audible tone is proportional to said generated scan data. Optionally, upon identification of said at least one anomaly, the hand-held imaging device is swept to scan the object using a fine scanning pattern for calculating said plurality of active pixels, calculating said time duration and generating said image.


In some embodiments, the method further includes receiving second data by the processor, wherein said second data is generated by the accelerometer and is indicative of a movement of the shaped X-ray beam being projected on the object and wherein based on said second data the method includes using the processor for calculating a plurality of active pixels corresponding to a new location of interaction of the shaped X-ray beam on the object; using the processor for calculating a time duration, at each of said plurality of active pixels, for which the shaped X-ray beam is present over each of said plurality of active pixels; and using the processor for generating an updated image, on said display, of the object after correcting the scan data, at each of said plurality of active pixels, using said time duration. Optionally, the new location is associated with an updated first data generated by the gyroscope, and wherein said updated first data is indicative of a new direction of the shaped X-ray beam being projected on the object.


In some embodiments, the acquisition system sums said detected scan data over a sampling duration ranging between 0.01 ms and 100 ms.


In some embodiments, the acquisition system sums said detected scan data over a sampling duration of 1 ms.


In some embodiments, a voltage of the X-ray tube ranges between 30 kV and 100 kV.


In some embodiments, a current of the X-ray tube ranges between 0.1 mA and 5 mA.


In some embodiments, the location is associated with a first data generated by the gyroscope, and wherein said first data is indicative of a direction of the shaped X-ray beam being projected on the object.


In some embodiments, the present specification discloses a system for a hand-held imaging device for scanning an object by projecting a shaped X-ray beam, where the device includes a housing having a central longitudinal axis. In some embodiments, the housing includes a rotating collimator having a transmission pattern defining said shaped X-ray beam, said rotating collimator supported and partially surrounded by an oscillating shaped cradle; a plurality of detectors for generating scan data corresponding to a plurality of detected X-ray beams; a gyroscope; an accelerometer; an acquisition system in communication with a speaker, a display and said plurality of detectors; and a processor in communication with said gyroscope, said accelerometer and said acquisition system. In some embodiments, the processor is configured for calculating a plurality of active pixels corresponding to a location of interaction of the shaped X-ray beam on the object; calculating a time duration, at each of said plurality of active pixels, for which the shaped X-ray beam is present over each of said plurality of active pixels; and generating an image, on said display, of the object after correcting the scan data, at each of said plurality of active pixels, using said time duration.


In some embodiments, the shaped X-ray beam is in the form of a pencil beam.


In some embodiments, the collimator rotates at a speed ranging between 100 to 5000 RPM. In some embodiments, the collimator rotates at a speed of 2000 RPM.


In some embodiments, the rotating collimator causes said shaped X-ray beam to sweep a trajectory in a substantially vertical plane such that a focal spot of said shaped X-ray beam is in a plane of said rotating collimator and on a central longitudinal axis of said housing, and wherein said oscillating shaped cradle causes said shaped X-ray beam to sweep left to right, repeatedly, over said substantially vertical plane.


In some embodiments, the collimator is a substantially circular disk having a first radius while said shaped cradle is substantially semi-circular having a second radius, and wherein said second radius is greater than said first radius.


In some embodiments, the collimator is a substantially circular disk having a radius while said shaped cradle is substantially ‘U’ or ‘C’ shaped.


In some embodiments, the transmission pattern is an opening at a point between a center and a circumference of said collimator, and wherein said rotating and said oscillating movements together cause said shaped X-ray beam to move in a raster pattern over a two dimensional area of the object.


In some embodiments, the housing has an upper surface, a base opposite and parallel to said upper surface, a front surface, a rear surface opposite and parallel to said front surface, a first side and a second side opposite and parallel to said first side, and wherein said upper surface has at least one handle. Optionally, the housing is configured as a first cuboid, bearing said front surface, which tapers along the central longitudinal axis into a second cuboid culminating in said rear surface. Optionally, the shaped X-ray beam emerges through an opening at a center of said front surface in a direction substantially perpendicular to said front surface. Still optionally, the plurality of detectors are positioned adjacent to and behind said front surface surrounding said opening at the center of said front surface. Still optionally, respective centers of said collimator and said shaped cradle are substantially coaxial with a central longitudinal axis of said housing, and wherein said collimator and said shaped cradle are positioned between said opening of said front surface and an opening of said X-ray tube.


The aforementioned and other embodiments of the present specification shall be described in greater depth in the drawings and detailed description provided below.





BRIEF DESCRIPTION OF THE DRAWINGS

These and other features and advantages of the present specification will be appreciated, as they become better understood by reference to the following detailed description when considered in connection with the accompanying drawings, wherein:



FIG. 1A is a perspective view of a hand-held portable scanning device, in accordance with an embodiment of the present specification;



FIG. 1B is a vertical cross-sectional view of the hand-held portable scanning device of FIG. 1A;



FIG. 1C illustrates the hand-held portable scanning device of the present specification projecting an X-ray beam over an object under inspection, in an embodiment;



FIG. 2A is a perspective view of a hand-held portable scanning device, in accordance with another embodiment of the present specification;



FIG. 2B is a vertical cross-sectional view of the hand-held portable scanning device of FIG. 2A;



FIG. 2C illustrates the hand-held portable scanning device of the present specification projecting an X-ray beam over an object under inspection, in an embodiment;



FIG. 3A is a perspective view of a hand-held portable scanning device, in accordance with another embodiment of the present specification;



FIG. 3B is a vertical cross-sectional view of the hand-held portable scanning device of FIG. 3A;



FIG. 3C illustrates the hand-held portable scanning device of the present specification projecting an X-ray beam over an object under inspection, in an embodiment;



FIG. 3D illustrates a collimator grid fabricated by assembling or arranging a plurality of combs having a plurality of teeth, in accordance with an embodiment;



FIG. 3E illustrates a sensing module formed by coupling an array of detectors to a card with a single signal control and readout cable, in accordance with an embodiment;



FIG. 3F illustrates a collimator grid coupled to a sensing module, in accordance with an embodiment;



FIG. 4A is a perspective view of a hand-held portable scanning device, in accordance with yet another embodiment of the present specification;



FIG. 4B is a vertical cross-sectional view of the hand-held portable scanning device of FIG. 4A;



FIG. 4C illustrates first and second collimator disks having first and second transmission patterns, respectively, in accordance with an embodiment;



FIG. 4D illustrates various exemplary positions of a moving or sweeping pencil X-ray beam defined by first and second transmission patterns of the first and second collimator disks shown in FIG. 4C;



FIG. 4E illustrates a motor driven assembly of first and second gears which, in turn, rotate the first and second collimator disks, shown in FIG. 4C;



FIG. 4F illustrates two sets of free running drive wheels or gears used to support the first and second collimator disks, shown in FIG. 4C;



FIG. 4G illustrates the hand-held portable scanning device of the present specification projecting an X-ray beam over an object under inspection, in an embodiment;



FIG. 5A is a perspective view of a hand-held portable scanning device, in accordance with still another embodiment of the present specification;



FIG. 5B is a vertical cross-sectional view of the hand-held portable scanning device of FIG. 5A;



FIG. 5C is a front view of a motor driven collimator assembly comprising a collimator and support or cradle, in accordance with an embodiment;



FIG. 5D is a side view of the motor driven collimator assembly of FIG. 1C;



FIG. 5E is a substantially spherical head portion of an X-ray tube positioned within the collimator assembly, in accordance with an embodiment;



FIG. 5F illustrates the hand-held portable scanning device of the present specification projecting an X-ray beam over an object under inspection, in an embodiment;



FIG. 6A is a block diagram illustrating a data acquisition system and a processing element in data communication with a plurality of detectors, a collimator motor, an azimuth motor, and a rotary encoder, in an embodiment of the present specification;



FIG. 6B is a block diagram illustrating a data acquisition system and a processing element in data communication with a plurality of detectors, a gyroscope and an accelerometer, in an embodiment of the present specification; and,



FIG. 7 is a flow chart illustrating exemplary steps of a method of scanning an object using the hand-held portable device of the present specification.





DETAILED DESCRIPTION

In some embodiments, the present specification discloses a system for scanning an object by projecting a shaped X-ray beam from a hand-held imaging device, where the device includes a housing enclosing an X-ray tube that emits the shaped X-ray beam, a plurality of detectors for generating scan data, a processor in communication with a gyroscope and an accelerometer, and an acquisition system. In some embodiments, the method includes using the processor for calculating a plurality of active pixels corresponding to a location of interaction of the shaped X-ray beam on the object; using the processor for calculating a time duration, at each of said plurality of active pixels, for which the shaped X-ray beam is present over each of said plurality of active pixels; and using the processor for generating an image, on said display, of the object after correcting the scan data, at each of said plurality of active pixels, using said time duration.


In some embodiments, the shaped X-ray beam is a pencil beam.


In some embodiments, the shaped X-ray beam is a cone beam.


In some embodiments, the shaped X-ray beam is a fan beam.


In some embodiments, the shaped X-ray beam is a single-axis rotating beam.


In some embodiments, the shaped X-ray beam is a dual-axis rotating beam.


The present specification is directed towards multiple embodiments. The following disclosure is provided in order to enable a person having ordinary skill in the art to practice the invention. Language used in this specification should not be interpreted as a general disavowal of any one specific embodiment or used to limit the claims beyond the meaning of the terms used therein. The general principles defined herein may be applied to other embodiments and applications without departing from the spirit and scope of the invention. Also, the terminology and phraseology used is for the purpose of describing exemplary embodiments and should not be considered limiting. Thus, the present invention is to be accorded the widest scope encompassing numerous alternatives, modifications and equivalents consistent with the principles and features disclosed. For purpose of clarity, details relating to technical material that is known in the technical fields related to the invention have not been described in detail so as not to unnecessarily obscure the present invention. In the description and claims of the application, each of the words “comprise” “include” and “have”, and forms thereof, are not necessarily limited to members in a list with which the words may be associated.


Pencil Beam



FIG. 1A illustrates an embodiment of a hand-held portable X-ray based scanning system 100, also referred to as an imaging system or device, for use in screening objects such as, but not limited to, baggage, containers/boxes, and other similar items for threat materials, items or people concealed therein. The system 100 is configured, in one embodiment, in the form of an enclosure or housing 105 having an upper surface 110, a base (not visible in FIG. 1A, but opposite, and substantially parallel to, the upper surface 110), a front surface 114, a rear surface (not visible in FIG. 1A, but opposite, and parallel to, the front surface 114), a first side 118, and a second side (not visible in FIG. 1A, but opposite, and parallel to, the first side 118). In accordance with one embodiment, the size and weight of system 100 is optimized for enabling an operator to conveniently hold and maneuver the housing 105 while scanning an object under inspection. In one embodiment, housing 105 is in the form of a first cuboid 125 (bearing the front surface 114) that tapers, along a central longitudinal axis 130, into a second cuboid 135 culminating in the rear surface. In accordance with an embodiment, a height ‘H’ of the first cuboid 125 is greater than a height ‘h’ of the second cuboid 135. It should, however, be appreciated that the shape of the housing 105 can be cylindrical, conical, pyramidal or any other suitable shape in various embodiments. Specifically, in one embodiment, housing 105 is in the form of a first cuboid 125 that attaches, at a back face and along a central longitudinal axis 130, to a first trapezoidal prism 118 that tapers and, at its back face, attaches a second trapezoidal prism 135.


At least one handle 112 is provided on, for example, the upper surface 110 to allow the operator to hold the housing 105 conveniently in one or both hands and manipulate the device 100 to point the front surface 114 towards and at different regions on the object under inspection. In alternate embodiments one or more handles are provided on one or more areas or regions such as the upper surface 110, the base, the first side 118 and/or the second side so that single-handed or two-handed operation of device 100 is facilitated, depending on what is easiest for the operator.


Conventionally, X-rays are generated using a thermionic source of electrons, such as a hot tungsten wire in vacuum. The thermionic electrons are then accelerated in an electric field towards an anode or target at a high electrical potential relative to the electron source. Typically the anode is made from a refractory metal of high atomic number, such as tungsten or molybdenum. When electrons hit the anode at high potential, X-rays are created as the electrons lose energy in the anode material. Typically it is through the photoelectric and Bremsstrahlung interactions by which the electrons lose their energy and so create X-rays. The net result is a broad spectrum of X-ray energies, from close to zero up to the maximum energy of the accelerated electrons.


The principles described above are applicable throughout each of the embodiments described in the present specification and will not be repeated with respect to each embodiment.


Referring now to FIGS. 1A and 1B, the housing 105 comprises an X-ray tube 140 whose anode 141, also referred to as a target, emits a spatially localized X-ray beam 145 through an opening 142, also referred to as an aperture. At least one shield 143, formed of an X-ray absorptive material, such as tungsten or uranium, surrounds and encloses anode 141 to absorb stray radiation emitted from anode 141. Opening 142, defined through shield 143, is provided with a size and thickness which enables opening 142 to act as a collimator in forming or shaping and limiting the X-ray radiation, emitted from anode 141, into a shaped beam of X-rays 145. In one embodiment, X-ray beam 145 is shaped into a pencil beam.


A cathode and heater filament assembly (enclosed within housing 105) is held at a substantial potential difference (using a chargeable battery also enclosed within the housing 105) with reference to anode 141 by a kilovolt power supply (wrapped around at least one tube shielding 143, in one embodiment). This potential difference causes thermionic electrons freed by the heated cathode (heated using the heater filament) to be directed and drawn to anode 141 at sufficiently high velocity to result in the generation of X-ray beam 145.


In accordance with an embodiment, shaped X-ray beam 145 emerges through an opening 144 at the center of front surface 114 of housing 105, in a direction substantially perpendicular to front surface 114. At least one or a plurality of X-ray backscatter detectors 150, also referred to as sensors, are positioned adjacent to and behind front surface 114 such that they surround the area or region of emergence of X-ray beam 145 at opening 144 and cover a substantial area of front surface 114 in order to maximize detected backscatter signal. An embodiment of the present specification comprises four sets of detectors 150. In other embodiments, a different number of detectors 150 may be utilized.


In accordance with an aspect, detectors 150 advantageously comprise high density inorganic scintillators (such as NaI, BGO, LYSO, CsI) coupled to a suitable optical readout such as a photomultiplier tube, an array of semiconductor photomultipliers or an array of photodiodes. Other detector types include inorganic scintillators (such as poly-vinyl toluene) coupled to photomultiplier tubes or room temperature semiconductor detectors (such as CdTe, CdZnTe, TlBr, HgI). As will be evident to one skilled in the art, many detector topologies are possible, such as, but not limited to, square segmented, circular segmented or annular, while the endeavor is to balance cost against complexity and overall detection efficiency. The detector surface adapted to received scattered X-ray radiation is positioned proximate the front surface 114 of housing 105.


Also, detectors 150 can be operated in a plurality of ways. For example, each detector can be operated in a pulse-counting, energy discriminating mode to build up an energy spectrum of the interacting X-rays, whereby these spectra are sampled over short scanning periods to build up a map of count rate and associated energy spectrum for each scatter source point location on the surface of the object under inspection. As an example, assume that the operator is scanning the beam at a rate of 0.2 m/second over the surface of the object and the projected X-ray beam width at the object is 10 mm. Therefore, in an embodiment, the update rate is equal to a movement of half the X-ray beam width (5 mm in this case) corresponding to a dwell time of (5 mm)/(200 mm/s)=25 ms. The energy distribution in the spectrum is analyzed to find those X-rays of higher energy which are more likely to have come from a greater depth in the object compared to those at lower energy which are more likely to have come from the surface of the object. It is also possible to separate out those photons whose energy is higher than the maximum emitted from the X-ray tube since these are either summed events (in which more than one scattered X-ray interacted in the detector at the same time) or are events due to naturally occurring background radiation. In either case, these are used to compensate for artifacts that would otherwise be present in the signal data.


It should be noted that the maximum energy of the X-rays produced by X-ray tube 140 determines the ability of these X-rays to penetrate into the object under inspection—that is, the higher the maximum X-ray energy, the more penetration can be achieved. Similarly, the higher the energy of the scattered X-ray photon, the more likely it is to escape through the object under inspection back to an X-ray detector 150. Therefore, in accordance with an aspect it is desirable to have high X-ray energy to maximize depth of inspection within the object.


To improve signal quality, device 100 of the present specification maximizes the number of scattered X-rays that are detected within a given signal integration or sampling period. The number of scattered X-rays for a given type of object under inspection is dependent on the number of X-rays that are incident on the object under inspection directly from the X-ray source. In the case of a fixed tube voltage, it is the anode current that affects the size of the scattered X-ray signal—that is, the higher the anode current, the greater the scattered signal. Most detection systems, such as the detectors 150, are operated close to the Gaussian point whereby the variance in the signal is equal to the mean value of the signal. For example, if the mean number of scattered X-rays reaching the detector in a certain counting period were 100, then the variance would be 100 and the standard deviation would be square root of 100 (=10). Signal-to-noise ratio (SNR) is defined as mean divided by standard deviation, therefore, SNR in this example would be 100/10=10.


Therefore, in a preferred embodiment, device 100 has high X-ray tube voltage (to improve penetration performance) and high anode current (to improve signal-to-noise ratio in the scattered X-ray signal). However, such a combination of factors will result in a device which is likely to be heavy due to the physical size of the X-ray tube components (to provide suitable clearance and creepage distance in the high voltage components) and the associated radiation shielding that will be needed to collimate the primary shaped beam and to shield the operator and radiation detectors from stray radiation from the X-ray tube target. Therefore, in various embodiments the tube voltage of the X-ray tube 140 ranges between 30 kV and 100 kV with tube currents ranging between 0.1 mA and 5 mA.


During operation, as shown in FIG. 1C, shaped X-ray beam 145 interacts with an object 160 under inspection, to produce scattered X-rays 146. As shown, object 160 conceals therein, an item, person or material 161. Scattered X-rays 146 are detected by the detectors 150 to produce scan data signal whose intensity is related to the effective atomic number (Z) near to the surface of object 160.


Compton scattering describes the interaction of an X-ray photon with an electron that is generally thought of as being at rest. Here, the angle of the exit X-ray photon is related to the direction of the incoming X-ray photon according to the Compton scattering equation:








λ


-
λ

=


h


m
e


c




(

1
-

cos


(
θ
)



)







where λ=incident photon energy, λ′=exit photon energy, me=mass of the electron and θ=angle between incident and exit photon directions. Thus, the energy of the scattered X-ray is always less than the incident X-ray, the energy being dependent on both the scattering angle and the incident X-ray photon energy.


The above principles related to Compton scattering described here are applicable throughout each of the embodiments described in the present specification and will not be repeated with respect to each embodiment.


Fan Beam



FIG. 2A illustrates another embodiment of a hand-held portable X-ray based scanning system 200, also referred to as an imaging system or device, for use in screening objects such as, but not limited to, baggage, containers/boxes, and other items for threat materials, items or people concealed therein. In embodiments, components of system 200, such as—a housing 205, an upper surface 210, a base, a handle 212, a front surface 214, a rear surface, a first side 218, a second side, a first cuboid 225, a central longitudinal axis 230, and a second cuboid (or trapezoidal prism) 235—are configured similar to corresponding components described above in context of FIG. 1A. These components, and the associated variations, are not described herein as they have been described in detail above.


Referring now to FIGS. 2A and 2B, housing 205 comprises an X-ray tube 240 whose anode 241, also referred to as a target, emits a spatially localized X-ray beam 245 through an opening 242, also referred to as an aperture. A shield 243, formed of an X-ray absorptive material, such as tungsten or uranium, surrounds anode 241 so as to absorb stray radiation emitted from anode 241. Opening 242 is provided with a size and thickness which enables opening 242 to act as a collimator in forming or shaping and limiting the X-ray radiation, emitted from anode 241, into a shaped beam of X-rays 245. In one embodiment, X-ray beam 245 is fan shaped.


A cathode and heater filament assembly (not shown) may be configured, similar to embodiments described in above relation to the pencil beam embodiment. Similarly, energy of the X-rays and signal quality can be maintained in a manner described above in context of the pencil beam embodiments.


A plurality of collimator vanes, blades, fins or plates 255 are positioned in front of detectors 250 and behind front surface 214, resulting in the formation of a plurality of collimation elements 256 between adjacent collimator vanes 255. In one embodiment, the planes of the plurality of collimator vanes 255 are arranged or configured in a direction substantially perpendicular to the orientation of shaped X-ray beam 245 (that is, to the plane of fan beam 245) or substantially perpendicular to the front surface of the housing. In some embodiments, plurality of collimator vanes 255 are arranged in a parallel configuration, wherein planes of vanes 255 are substantially parallel to each other, such that a vertical dimension, such as height, of a vertical region is viewed through collimators 255 to be of the same size as the extent or height ‘H’ of front surface 214. In some embodiments, collimator vanes 255 are alternatively arranged in a focused configuration, wherein the planes of vanes 255 together form a diverging or converging orientation, such that collimator vanes 255 view either a smaller or larger of the vertical dimension, such as height, of the vertical region than the extent or the height ‘H’ of front surface 214.


In various embodiments, detectors 250 are arranged behind collimator vanes 255 such that at least one of detectors 250 is present per collimation element 256 in order to create a one-dimensional linear image.


During operation, as shown in FIG. 2C, shaped X-ray beam 245 interacts with an object 260 under inspection, to produce scattered X-rays 246. As shown, object 260 conceals therein, an item, person or material 261. Scattered X-rays 246 are collimated by the plurality of collimator vanes 255 and are then detected by detectors 250 to produce scan data signal whose intensity is related to the effective atomic number (Z) near to the surface of object 260. In accordance with an embodiment, each detector 250 maps to a specific focus area (of the object 260) which is defined by a width of X-ray fan beam 245 and an acceptance angle of the individual collimator vanes 255.


Cone Beam



FIG. 3A illustrates another embodiment of a hand-held portable X-ray based scanning system 300, also referred to as an imaging system or device, for use in screening objects such as, but not limited to, baggage, containers/boxes, and other similar items for threat materials, items or people concealed therein. In embodiments, components of system 300, such as—a housing 305, an upper surface 310, a base, a handle 312, a front surface 314, a rear surface, a first side 318, a second side, a first cuboid 325, a central longitudinal axis 330, and a second cuboid (or trapezoidal prism) 335—are configured similar to corresponding components described above in context of FIG. 1A. These components, and associated variations, are not described herein as they have been described in detail above.


Referring now to FIGS. 3A and 3B, housing 305 comprises an X-ray tube 340 whose anode 341, also referred to as a target, emits a spatially localized X-ray beam 345 through an opening 342, also referred to as an aperture. Housing 305 may include corresponding components such as a shield 343, configured in a manner disclosed above in context of FIGS. 1A and 1B. In one embodiment, X-ray beam 345 is cone shaped.


A cathode and heater filament assembly may be configured, similar to embodiments described in above relation to the pencil beam embodiment.


In accordance with an embodiment, shaped X-ray beam 345 emerges through an opening 344 at the center of front surface 314, in a direction substantially perpendicular to front surface 314. A plurality of X-ray backscatter detectors 350 are configured and operated similar to detectors 150 already described in context of FIGS. 1A and 1B. As shown in FIG. 3E, in accordance with an embodiment, an array of ‘m’ rowsבn’ columns of detectors 350 are arranged onto a modular daughter card 351 with a single signal control and readout cable 352 to form a sensing module 353.


Similarly, the energy of the X-rays and signal quality can be maintained in a manner described above in context of the pencil beam embodiments.


Referring now to FIGS. 3A, 3D through 3F, in accordance with an embodiment of the present specification, a collimator grid 355 is positioned in front of detectors 350 and behind front surface 314. Collimator grid 355 comprises a plurality of combs 365a, 365b, made of a suitable attenuating material (such as tungsten, molybdenum or steel), each of plurality of combs 365a, 365b including a plurality of teeth 370a, 370b. In accordance with an embodiment, plurality of combs 365a, 365b are assembled or arranged such that teeth 370a of a first set of combs 365a in a first direction 371a interlock with teeth 370b of a second set of combs 365b in a second direction 371b to thereby generate the collimator grid 355 having a plurality of grid collimators or collimator elements 374. In one embodiment, second direction 371b is generally or approximately traverse or orthogonal to first direction 371a. In accordance with an embodiment, the first set comprises ‘m’ number of combs 365a while the second set comprises ‘n’ number of combs 365b to generate a collimator grid 355 that has ‘m×n’ matrix of substantially rectangular grid collimators 374 at top surface 375.


In one embodiment, the planes of teeth 370a, 370b, forming the grid collimators or collimator elements 374, are in a direction substantially parallel to the orientation of the shaped X-ray beam 345 (that is, cone shaped beam 345) or perpendicular to the front surface of the housing. In some embodiments, the plurality of grid collimators or collimator elements 374 are arranged in a parallel configuration, wherein the planes of teeth 370a, 370b are substantially parallel to each other, such that a vertical dimension, such as height, of a vertical region is viewed through the collimators 374 to be of the same size as the extent or height ‘H’ of front surface 314. In some embodiments, the plurality of grid collimators or collimator elements 374 are alternatively arranged in a focused configuration, wherein the planes of teeth 370a, 370b together form a diverging or converging orientation, such that the collimator elements 374 view either a smaller or larger of the vertical dimension, such as height, of the vertical region than the extent or the height ‘H’ of front surface 314. In still various embodiments, the plurality of grid collimators or collimator elements 374 is arranged in a combination of parallel and focused configurations.


In various embodiments, detectors 350 are arranged behind the interlocking collimator structure or collimator grid 355 such that at least one of detectors 350 is present per collimator element or grid collimator 374 in order to create a two-dimensional scan image. As shown in FIG. 3F, collimator grid 355 is coupled to sensing module 353 (comprising the detector module 350 coupled to the daughter card 351 with the signal control and readout cable 352) such that the array of ‘m×n’ detectors 350 are positioned behind grid 355.


During operation, as shown in FIG. 3C, shaped X-ray beam 345 interacts with an object 360 under inspection to produce scattered X-rays 346. As shown, object 360 conceals therein, an item or material 361. Scattered X-rays 346 is collimated by the plurality of grid collimators or collimator elements 374 and is then detected by the detectors 350 to produce scan data signal whose intensity is related to the effective atomic number (Z) near to the surface of object 360. In accordance with an embodiment, each detector 350 maps to a specific focus area (of the object 360) which is defined by a solid angle of X-ray cone beam 345 and an acceptance angle of the individual collimator elements or grid collimators 374.


Conventional backscatter imaging systems typically use a tightly collimated pencil beam of X-rays and an un-collimated large area detector (referred to as “pencil beam geometry”) compared to the use of the collimated cone-shaped beam of X-rays and collimated detectors (referred to as “cone beam geometry”) in accordance with an aspect of the present specification. With reference to FIG. 3A, the handheld device of the present specification has, in one embodiment, an outer diameter of 192 mm (considering a circular cross-section of the housing 105) of front surface 314 and is located at a distance of 100 mm from the object under inspection. Detector element 350 is, in an embodiment, 3 mm×3 mm with the X-ray source (X-ray tube 140) located a further 30 mm behind detector array 350 to provide room for radiation shielding around the source. In this embodiment, a total of 4096 detector elements are employed (to create a 64 pixel by 64 pixel image) with an equivalent dwell time of 500 microseconds for pencil beam geometry.


To establish the relative efficiency of the pencil beam versus cone beam configuration, it is useful to calculate the relative solid angles of the whole detector face (pencil beam) and of a single detector to the equivalent inspection area as scanned by the pencil beam (for the cone beam case). This calculation shows that the solid angle for the collimated detector (used in cone beam geometry) is 290 times smaller than for the whole detector face (used in pencil beam geometry).


Taking the assumed pencil beam dwell time of 500 microseconds and multiplying by the number of pixel locations to form an image (4096 in this case) yields an estimated image formation time in pencil beam geometry of 2 seconds. The calculation in the case of the cone beam geometry of the present specification suggests that the dwell time should be 290 times longer than for the pencil beam case to achieve equivalent image statistics, but with a single exposure since all pixel data is collected in parallel. Also, in the case of the cone beam geometry, the image exposure time is more than 50% less than an equivalent pencil beam. This yields an image exposure time in a range of 0.03 seconds 0.1 seconds. Therefore, near real-time two-dimensional image inspection is possible using Compton backscatter inspection in the cone beam geometry of the present specification.


Single-Axis Rotating Beam



FIG. 4A illustrates an embodiment of a hand-held portable X-ray based scanning system 400, also referred to as an imaging system or device, for use in screening objects such as, but not limited to, baggage, containers/boxes, and other similar items for threat materials, items or people concealed therein. In embodiments, components of system 400, such as—a housing 405, an upper surface 410, a base, a handle 412, a front surface 414, a rear surface, a first side 418, a second side, a first cuboid 425, a central longitudinal axis 430, and a second cuboid (or trapezoidal prism) 435—are configured similar to corresponding components described above in context of FIG. 1A. These components, and associated variations, are not described herein as they have been described in detail above.


Referring now to FIGS. 4A and 4B, housing 405 comprises an X-ray tube 440 whose anode 441, also referred to as a target, emits a spatially localized X-ray beam 445a through an opening 442, also referred to as an aperture. A shield 443, formed of an X-ray absorptive material, such as tungsten or uranium, surrounds anode 441 to absorb stray radiation emitted from anode 441. Opening 442 is defined through a highly absorbing block or material (typically tungsten, steel and/or lead) to limit the X-ray radiation, emitted from anode 441, and allow the X-ray radiation to emanate from X-ray tube 440 in the form of beam 445a of X-rays. A cathode and heater filament assembly may be configured, similar to embodiments described in above relation to the pencil beam embodiment.


In accordance with an embodiment of the present specification, X-ray beam 445a is collimated by a collimator assembly 470, enclosed within housing 405, to generate a shaped X-ray beam 445b. In one embodiment, X-ray beam 445b is shaped into a pencil beam. In accordance with an embodiment, shaped X-ray beam 445b emerges through an opening 444 at the center of front surface 414, in a direction substantially perpendicular to front surface 414. A plurality of X-ray backscatter detectors 450 are positioned adjacent to and behind front surface 414 such that they surround the area or region of emergence of X-ray beam 445b at opening 444 and cover a substantial area of front surface 414 in order to maximize detected backscatter signal. An embodiment of the present specification comprises four sets of detectors 450, also referred to as sensors.


An embodiment of collimator assembly 470 comprises a first collimator 472, also referred to as a first limiting element, arranged coaxially in front of a second collimator 474, also referred to as a second limiting element. In one embodiment first and second collimators 472, 474 are positioned between openings 443 and 444 such that collimator assembly 470 defines, shapes, or forms X-ray beam 445a into the shaped X-ray beam 445b.


Referring now to FIGS. 4A through 4F, in one embodiment, first and second collimators 472, 474 are substantially circular disks having differing or same radii. In an embodiment, the respective centers of the first and second collimators 472, 474 are coaxial with the central longitudinal axis 430 of housing 405. First collimator 472 has a first transmission pattern in the form of a through slit 473 extending in a spirally curved configuration from a point proximate center 475 to a point proximate the circumference of element 472. Second collimator 474 has a second transmission pattern in the form of through slit 477 extending radially from a point proximate center 476 to a point proximate the circumference of element 474. Thus, when two collimators 472, 474 are concurrently rotating, the respective first and second transmission patterns or slits 473, 477 generate or define the scanning X-ray pencil beam 445b across the surface of the object under inspection.


In accordance with an embodiment, the first transmission pattern 473 defines a radial position of pencil beam 445b while the second transmission pattern 477 defines an azimuthal angle of pencil beam 445b. For example, as shown in FIG. 4D, when collimators 472, 474 (the two collimator disks 472, 474 are visible as a single disk since they are shown overlapping each other in FIG. 4D) are rotated relative to each other the position of pencil beam 445b moves or sweeps from a position 480a at the circumference to a position 480d at the coaxial centers 475, 476 (of the collimators 472, 474) through intermediate positions 480b and 480c.



FIG. 4E illustrates a motor 485 driving the first and second collimators 472, 474 using a first and a second gear or drive wheels 486, 487 respectively. As would be evident to those of ordinary skill in the art, gears 486, 487, also referred to as drive wheels, engage with mating gear teeth fabricated on the respective circumferences of two collimator disks 472, 474. In accordance with an embodiment, first and second gears 486, 487 rotate the collimator disks 472, 474 such that two collimators 472, 474 are in lock step with each other but rotate at varying speeds to form beam 445a into the shaped X-ray beam 445b. In one embodiment, collimator disk 474 rotates more quickly compared to the speed of rotation of collimator disk 472. In one embodiment, collimator disk 472 rotates more quickly compared to the speed of rotation of collimator disk 474. In one embodiment, the drive wheel or gears 486, 487 affixed to a common spindle (not visible) are driven by motor 485 to rotate collimator disks 472, 474 while two sets of additional free running wheels 488, 489 (not driven by motor 485), shown in FIG. 4F, support collimator disks 472, 474 to maintain their position or orientation relative to X-ray tube 440 (or opening 442).


A plurality of X-ray backscatter detectors 450 are configured and operated similar to detectors 150 already described in context of FIGS. 1A and 1B. Similarly, energy of the X-rays and signal quality can be maintained in a manner described earlier in context of the pencil beam embodiments.


During operation, as shown in FIG. 4G, shaped X-ray beam 445b interacts with an object 460 under inspection to produce scattered X-rays 446. As shown, object 460 conceals therein, an item or material 461. Scattered X-rays 446 are then detected by detectors 450 to produce scan data signal whose intensity is related to the effective atomic number (Z) near to the surface of object 460. Any one or more of the aforementioned collimation systems can be combined with this single-axis rotating beam embodiment to effectively detect scattered X-rays.


Dual-Axis Rotating Beam



FIG. 5A illustrates another embodiment of a hand-held portable X-ray based scanning system 500, also referred to as an imaging system or device, for use in screening objects such as, but not limited to, baggage, containers/boxes, and other similar items for threat materials, items or people concealed therein. In embodiments, components of system 500, such as—a housing 505, an upper surface 510, a base, a handle 512, a front surface 514, a rear surface, a first side 518, a second side, a first cuboid 525, a central longitudinal axis 530, and a second cuboid (or trapezoidal prism) 535—are configured similar to corresponding components described above in context of FIG. 1A. These components, and associated variations, are not described here to avoid repetition.


Referring now to FIGS. 5A and 5B, housing 505 comprises an X-ray tube 540 (shown separated out from housing 505 in FIG. 5B) whose anode 541, also referred to as a target, emits a spatially localized X-ray beam 545a through an opening 542, also referred to as an aperture. A shield 543, formed of an X-ray absorptive material, such as tungsten, steel, lead or uranium, is disposed to surround and enclose anode 541 to absorb stray radiation emitted from anode 541. Further, the anode is surrounded by a highly absorbing block or material 593 (typically tungsten, steel and/or lead) through which opening 542 is defined. In an embodiment, opening 542 is a cone beam collimator slot and defines the overall area for X-ray emission, emitted from anode 541 in the form of beam 545a, with the moving collimator parts described below. In some embodiments, opening 542 is shaped so that X-ray beam 545a emanates as a cone beam. Also, in an embodiment, the head portion of X-ray tube 540, comprising opening 542, is shaped in a substantially spherical form. A cathode and heater filament assembly (not shown) may be configured, similar to embodiments described in above relation to the pencil beam embodiment.


An embodiment of collimator assembly 570 comprises a collimator 572, also referred to as a limiting element, partially surrounded by a shaped support or cradle element 574. In various embodiments, support or cradle 574 has a substantially semi-circular, or ‘C’ shape. In an embodiment, collimator 572 is a circular disk having a first radius. In one embodiment, where cradle 574 is substantially semi-circular shaped, it has a second radius, greater than the first radius, so that cradle 574 partially encompasses collimator 572. In accordance with an embodiment collimator 572 and cradle 574 are positioned between openings 543 and 544 such that a movement of collimator assembly 570 defines, shapes or forms X-ray beam 545a into pencil shaped X-ray beam 545b.


Referring now to FIGS. 5A through 5E, in one embodiment, the respective centers of collimator 572 and cradle 574 are substantially coaxial with central longitudinal axis 530 of housing 505. Collimator 572 has a transmission pattern in the form of a through opening 573 at a point between the center and the circumference of element 572. Collimator 572 is rotatable, about central longitudinal axis 530, through a bearing 582 supported by shaped cradle 574. Cradle 574 is fixed to pivoting mounts that allow cradle 572 to be oscillated about a vertical axis 532. In accordance with an aspect of the present specification, a motor 585 rotates or spins collimator 572, at a speed, about central longitudinal axis 530 while the supporting element or cradle 574 vibrates or oscillates, from side to side, about vertical axis 532 thereby causing the rotating or spinning collimator 572 to also vibrate or oscillate. In various embodiments, collimator 572 rotates at a speed ranging between 100 to 5000 RPM. In one embodiment, collimator 572 speed is 2000 RPM.


Rotating collimator 572 defines pencil beam 545b that sweeps a trajectory in a substantially vertical plane where the X-ray focal spot is in the plane of collimator 572 and on longitudinal axis 530 of bearing 582. The vibratory or oscillatory movement of cradle 574 and therefore that of collimator 572 causes pencil beam 545b to sweep over the substantially vertical plane moving from left to right and back again. The combined effect of the rotatory or spinning and oscillatory or vibratory movement of the collimator assembly 570 is one where pencil beam 545b moves in a raster pattern over a two dimensional area of the object under inspection. FIG. 5E shows X-ray tube 540 positioned within the moving collimator assembly 570 so that the substantially spherical shaped head portion 590 of X-ray tube 540, comprising opening 542, and rotating collimator 572 (supported by cradle 574) enable tight radiation collimation as X-ray beam 545b is scanned. The substantially spherical shaped head portion 590 of X-ray tube 540 allows the rotating and rocking or oscillating collimator 572 to efficiently move around head 590 with minimum radiation leakage.


A plurality of X-ray backscatter detectors 550 are configured and operated similar to detectors 150 already described in context of FIGS. 1A and 1B. Similarly, energy of the X-rays and signal quality can be maintained in a manner described earlier in context of the pencil beam embodiments.


In one embodiment, detectors 550 are scintillator based detector arrays with light guide readout to photomultiplier tubes.


During operation, as shown in FIG. 5F, shaped X-ray beam 545b interacts with an object 560 under inspection to produce scattered X-rays 546. As shown, object 560 conceals therein, an item or material 561. Scattered X-rays 546 are then detected by detectors 550 to produce scan data signal whose intensity is related to the effective atomic number (Z) near to the surface of object 560. Any one or a combination of the collimation systems disclosed above may be combined with this embodiment.


The position of the collimators is used to accurately correct images. Referring to FIG. 6A, a plurality of sensors 640 (corresponding to at least one of the detectors or detector systems mentioned in the embodiments above) is used to acquire data and communicate that data to a data acquisition system (DAQ) 610. DAQ 610, in turn, controls motor drivers responsible for creating collimator motion. Such motors include an azimuth motor 675 and a collimator motor 670. Rotary encoders 680 monitor the absolute position of the collimators and supply that information to DAQ 610 which, in turn, uses it to correct an acquired image based upon such position data.


As shown in FIG. 6B, in another embodiment, scan data 605 produced by plurality of detectors 645 (corresponding to at least one of the detectors or detector systems mentioned in the embodiments above) is accumulated into DAQ 610 wherein scan data 605 is summed within appropriate or optimal sampling time slots, time bins, or time periods. It should be appreciated that the shorter the sampling time period the noisier is the collected scan data but the more accurate or focused it is in terms of spatial location. In various embodiments scan data 605 sampling time slots, time bins, or time periods vary between 0.01 ms and 100 ms. In one embodiment, scan data 605 sampling time slot or time period is of 1 ms duration. A processing element 650, such as a microprocessor or a digital signal processor (DSP), is in data communication with DAQ 610 to perform a plurality of analyses or calculations using at least scan data 605. In one embodiment, scan data 605 is analyzed by comparing a mean scan signal level calculated over one or more temporal sampling periods with a background reference level. The bigger the difference between the sampled signal and the background level, the more substantial is the scattering object.


In accordance with an embodiment where a fan beam is utilized, the analysis is computed behind each of the plurality of collimator vanes 255 (FIGS. 2A, 2B), independently, in order to enable spatial localization and detection of even small anomalies. In further embodiments, to improve signal-to-noise ratio, the intensity of detected scatter signal 605 is estimated over all detectors 645 (corresponding to at least one of the detectors or detector systems mentioned in the embodiments above) by calculating a weighted sum of the pixel based and total signal data analysis.


In accordance with an aspect of the present specification, for each of the embodiments (illustrated in FIGS. 6A and 6B) disclosed above, the detected scatter scan data 605 is utilized to generate an alarm or feedback for the operator. In various embodiments the alarm or feedback is in the form of an audible tone and/or a scan image of the object under inspection. Accordingly, detected scatter scan data 605 is converted, using a speaker 615, into an audible tone or alarm, the pitch or frequency of which, in one embodiment, is directly proportional to the scatter signal. For example, speaker 615 emits a background tone at about 100 Hz with an average signal of 1000 detected scatter X-rays producing a frequency of about 400 Hz. Thus, a scattering object which generates a signal of 500 detected scatter X-rays would produce a tone at about 250 Hz. It will be appreciated by one of ordinary skill in the art that alternative mapping between detected scatter signal and audible tone or alarm can be envisioned, such as one which provides an exponential increase in tone, pitch or frequency to provide greater contrast for low scattering objects than for high scattering ones.


The probability of an X-ray photon interacting with the object under inspection depends strongly on the atomic number of the object—that is, the higher the atomic number the higher the probability of interaction. Similarly, the probability of absorbing a Compton scattered X-ray also depends strongly on the atomic number of the object under inspection. Therefore, it is known by those skilled in the art that the Compton backscatter signal is highest for low atomic number materials such as organic materials and people and is smallest for high atomic number materials such as steel and lead.


Additionally or alternatively, the scan image of the object under inspection is displayed on at least one display 620. A visual feedback, such as the scan image, is advantageous to enable the operator to notice subtle differences between one scattering object and another since the human visual system has a natural ability at identifying shapes and associating these shapes with specific threats (such as a gun or a knife). Referring to FIG. 6B, in order to form the scan image, an embodiment of the present specification includes a 3D gyroscope 625 and/or a 3D accelerometer 630 within the respective housings. 3D gyroscope 625 is used to track a first data stream indicative of an absolute position or pointing direction of the X-ray beam or hand-held device in 3D space, while 3D accelerometer 630 tracks a second data stream indicative of rapid relative movements of the X-ray beam in 3D space. In accordance with an embodiment, the first and second data streams are input into and combined by processing element 650 to generate position or coordinates 640 of the X-ray beam at all times during scanning operation, even in response to rapid movement of the beam or hand-held device (in embodiments described above) by the operator.


According to an aspect of the present specification, each position or coordinate of the X-ray beam in 3D space has associated plurality of active pixels that correspond to the particular spatial location, on the object under inspection, where the X-ray beam is interacting. These active pixels are located within a matrix of other potentially active pixels which together constitute an image. In a practical scenario, it is reasonable to assume that the operator will sweep the X-ray beam over the object more than once causing multiple scan frames to contribute to a pixel in the image. Therefore, in order to ensure a quantitative image, the brightness or scan data of each pixel is corrected by the total X-ray beam dwell time at that pixel location. This dwell time is calculated over all periods that the X-ray beam is present over each active pixel.


The number of X-rays reaching the object under inspection is defined by the X-ray beam collimator aperture and beam divergence. The area of the object under inspection that is covered by the X-ray beam is then determined by the distance of the X-ray source from the object under inspection—that is, the larger the distance the larger the area of the object covered by the X-ray beam. The number of scattered X-rays that return to the detector is inversely proportional to the distance between the object under inspection and the detector array. Thus, in one operating condition, the hand-held device of the present specification as described in various embodiments above is held close to the object under inspection, so that the area of the object irradiated by the X-ray beam is small and the fraction of the scattered signal collected by the detector is high.



FIG. 7 is a flow chart illustrating a plurality of exemplary steps of a method of scanning an object using an X-ray beam projected by the hand-held portable device of the present specification. At 705, an operator first sweeps the X-ray beam onto the object using a coarse scanning pattern during which a change in audible tone is used as the primary feedback to identify anomalies with reference to the object. The coarse scanning pattern, in one embodiment, refers to a fairly quick scanning or sweeping movement of the X-ray beam over the surface of the object, referred to as the general scanning area, where the coarse scanning pattern is defined as having a first density of X-ray coverage over the general scanning area. If no anomaly is identified, at 710, then the scan of the object is stopped, at 712, and a new scan session for another object can begin, if required. However, if an anomaly is identified, at 710, the operator then proceeds to make fine scanning patterns or relatively slower movements of the X-ray beam around the anomalous area, at 715, where the fine scanning pattern is defined as having a second density of X-ray coverage over the anomalous area. It should be appreciated that the anomalous area is smaller than, but positioned within, the general scanning area. It should also be appreciated that the second density (associated with the fine scanning pattern) is greater than the first density (associated with the coarse scanning pattern).


On initiating the fine sweep scanning of the object, the followings tasks are performed: at 716, data is received from a 3D gyroscope representing a direction of pointing of the X-ray beam projected onto the object; at 717 a plurality of active pixels corresponding to the direction of the X-ray beam are calculated; at 718, a dwell time of the X-ray beam at each of the active pixels is calculated; and at 719, a scan image after correcting the scan data signal is generated, at each of the active pixels, using the dwell time. At 720, data from a 3D accelerometer is obtained to check if there is a movement of the X-ray beam relative to the direction of the X-ray beam obtained at 716. If there is no movement of the X-ray beam detected, at 723, then the steps 717 to 720 are repeated (till a movement of the X-ray beam is detected).


However, if a movement of the X-ray beam is detected, at 723, then the following tasks are performed: at 725, data is received from the 3D gyroscope representing a new direction of the X-ray beam due to the movement of the X-ray beam; at 726, a plurality of active new pixels corresponding to the new direction of the X-ray beam are calculated; at 727, a dwell time of the X-ray beam at each of the active new pixels is calculated; and at 728, an updated scan image is generated after applying the dwell time correction to the scan data signal at each active pixel.


At 730, data from the 3D accelerometer is obtained again to check if there is a continued movement of the X-ray beam. If it is determined at 733 that the X-ray beam is still moving or being swept over the object, then steps 725 to 730 are repeated (till the X-ray beam sweeping movement stops). However, in case there is no detected movement of the projected X-ray beam at 733, then at 735 a check is performed to determine whether the scanning has to be stopped (and therefore, move to 740) or another scanning session or event should begin from 705 onwards. The scan image generated at 719 and/or 728 is visually analyzed by the operator to determine further features of the anomaly and declare the anomaly as benign or threat.


In various embodiments of the present specification, the hand-held device of the present specification, such as those in embodiments described above, includes a laser-beam range finder or any other suitable optical sensor beam, known to persons of ordinary skill in the art, is used to propagate an optical, visible light or laser beam along the central path of the X-ray beam (for example, by deflecting a laser beam using a thin gold coated Mylar film reflector in the X-ray beam path). The directed optical or laser beam is used to calculate the distance of the hand-held device from the object under inspection so that the surface of the object can be reconstructed in three-dimensional (3D) space (using the measured distance to the surface of the object taken in combination with the gyroscope and/or accelerometer data) in order to create an X-ray image that wraps around the three-dimensional surface of the object under inspection. Such a three-dimensional view can help the image interpreter or operator to better identify or estimate the exact location of the anomaly or threat object, area or region.


The above examples are merely illustrative of the many applications of the system of present specification. Although only a few embodiments of the present invention have been described herein, it should be understood that the present invention might be embodied in many other specific forms without departing from the spirit or scope of the invention. Therefore, the present examples and embodiments are to be considered as illustrative and not restrictive, and the invention may be modified within the scope of the appended claims.

Claims
  • 1. A method of scanning an object using a hand-held imaging device comprising: obtaining the hand-held imaging device, wherein the hand-held imaging device comprises a housing, at least one sensor positioned in the housing and configured to generate a first set of data representative of a position or a movement of the hand-held imaging device relative to the object, an X-ray source positioned within the housing and configured to generate an X-ray beam, detectors configured to generate scan data corresponding to energy scattered from the object, a display coupled to the housing, and a processing system comprising at least one processor positioned within the housing in communication with the at least one sensor, the detectors, and the display, wherein the processing system is configured to receive the first set of data and the scan data, correct the scan data using the first set of data, and generate an image based on the corrected data;causing the X-ray source to emit the X-ray beam;moving the hand-held imaging device relative to the object; andcausing the image to be displayed on the display.
  • 2. The method of claim 1, further comprising a collimator assembly positioned within the housing and configured to shape the X-ray beam from the X-ray source into a shaped X-ray beam.
  • 3. The method of claim 2, wherein the collimator assembly comprises a first collimator and a second collimator and wherein at least one the first collimator or the second collimator is adapted to shape the X-ray beam into an X-ray pencil beam.
  • 4. The method of claim 3, wherein the first collimator is a rotating collimator.
  • 5. The method of claim 4, wherein the second collimator is a rotating collimator.
  • 6. The method of claim 3, wherein at least one of the first collimator or the second collimator comprises a circular disc defining a radius and wherein the disk has a slit extending radially from a point proximate to a center of the disk to a point proximate to an edge of the disk.
  • 7. The method of claim 2, further comprising X-ray absorptive material positioned around the X-ray source.
  • 8. The method of claim 7, wherein the X-ray absorptive material comprises at least one of tungsten or uranium.
  • 9. The method of claim 7, wherein the X-ray absorptive material defines an opening and wherein a portion of the collimator assembly comprises said opening.
  • 10. The method of claim 2, wherein the collimator assembly comprises a first collimator proximate to an opening of the X-ray source and a second collimator positioned between the X-ray source and a front surface of the housing.
  • 11. The method of claim 10, wherein the second collimator is a rotating collimator and is configured to shape the X-ray beam.
  • 12. The method of claim 1, wherein the first set of data comprises a dwell time at a particular location.
  • 13. The method of claim 1, wherein the first set of data comprises a speed of the hand-held imaging device relative to the object.
  • 14. The method of claim 1, wherein the first set of data comprises a time that is based on a movement speed of the hand-held imaging device relative to the object.
  • 15. The method of claim 14, wherein the movement speed is approximately 0.2 meters per second.
  • 16. The method of claim 1, wherein the at least one sensor comprises at least one of an accelerometer or a gyroscope.
  • 17. The method of claim 1, wherein the X-ray source is adapted to operate at a fixed voltage.
  • 18. The method of claim 17, wherein the voltage is above 70 kilovolt (kV).
  • 19. The method of claim 17, wherein the voltage is above 90 kilovolt (kV).
  • 20. The method of claim 17, wherein the voltage is above 95 kilovolt (kV).
  • 21. The method of claim 1, further comprising one or more rechargeable batteries positioned in the housing, wherein the one or more rechargeable batteries are adapted to supply energy to one or more of the X-ray source, the detectors, the processing system, and/or the display.
  • 22. The method of claim 1, further comprising defining the first set of data by a sampling frequency.
  • 23. The method of claim 1, further comprising real-time presenting the image on the display in response to operator control.
  • 24. The method of claim 1, wherein the processing system further comprises a digital signal processor (DSP).
  • 25. The method of claim 24, further comprising using the DSP to determine a mean scan signal level over one or more temporal sampling periods based on the scan data.
  • 26. The method of claim 1, wherein the scan data is representative of an atomic number of a material concealed within or behind at least a portion of the object and wherein said material comprises at least one of narcotics, explosives, or currency.
  • 27. The method of claim 1, wherein the X-ray beam comprises a pencil beam and wherein the hand-held imaging device is adapted to project the pencil beam in a raster pattern over a two dimensional area of the object.
CROSS-REFERENCE

The present application is a continuation application of U.S. patent application Ser. No. 16/199,531, entitled “Hand-Held Portable Backscatter Inspections System” and filed on Nov. 26, 2018, which is a continuation application of U.S. patent application Ser. No. 15/074,787, of the same title, filed on Mar. 18, 2016, and issued as U.S. Pat. No. 10,168,445 on Jan. 1, 2019, which relies on U.S. Patent Provisional Application No. 62/136,299, entitled “Handheld Portable Backscatter Inspection System” and filed on Mar. 20, 2015, for priority. U.S. patent application Ser. No. 15/074,787 also relies on U.S. Patent Provisional Application No. 62/136,305, entitled “Handheld Portable Backscatter Inspection System” and filed on Mar. 20, 2015, for priority. U.S. patent application Ser. No. 15/074,787 also relies on U.S. Patent Provisional Application No. 62/136,315, entitled “Handheld Portable Backscatter Inspection System” and filed on Mar. 20, 2015, for priority. U.S. patent application Ser. No. 15/074,787 also relies on U.S. Patent Provisional Application No. 62/136,322, entitled “Handheld Portable Backscatter Inspection System” and filed on Mar. 20, 2015, for priority. U.S. patent application Ser. No. 15/074,787 also relies on U.S. Patent Provisional Application No. 62/136,362, entitled “Handheld Portable Backscatter Inspection System” and filed on Mar. 20, 2015, for priority. All of the above-mentioned applications are herein incorporated by reference in their entirety.

US Referenced Citations (527)
Number Name Date Kind
663072 Coy Dec 1900 A
2831123 Daly Apr 1958 A
2972430 Johnson Feb 1961 A
3766387 Heffan Oct 1973 A
3780291 Stein Dec 1973 A
3784837 Holmstrom Jan 1974 A
3961186 Leunbach Jun 1976 A
3971948 Pfeiler Jul 1976 A
4031401 Jacob Jun 1977 A
4045672 Watanabe Aug 1977 A
4047035 Dennhoven Sep 1977 A
4064440 Roder Dec 1977 A
4139771 Dennhoven Feb 1979 A
4180737 Kingsley Dec 1979 A
4200800 Swift Apr 1980 A
4210811 Dennhoven Jul 1980 A
4216499 Dennhoven Aug 1980 A
4242583 Annis Dec 1980 A
4259582 Albert Mar 1981 A
4260898 Annis Apr 1981 A
4267446 Brown May 1981 A
4315146 Rudin Feb 1982 A
4342914 Bjorkholm Aug 1982 A
4366382 Kotowski Dec 1982 A
4380817 Harding Apr 1983 A
4420182 Kaneshiro Dec 1983 A
4430568 Yoshida Feb 1984 A
4472822 Swift Sep 1984 A
4494001 Peck Jan 1985 A
4497062 Mistretta Jan 1985 A
4503332 Annis Mar 1985 A
4511799 Bjorkholm Apr 1985 A
4525854 Molbert Jun 1985 A
4566113 Doenges Jan 1986 A
4599740 Cable Jul 1986 A
4620099 Schoenig Oct 1986 A
4641330 Herwig Feb 1987 A
4646339 Rice Feb 1987 A
4692937 Sashin Sep 1987 A
4718075 Horn Jan 1988 A
4736401 Donges Apr 1988 A
4788436 Koechner Nov 1988 A
4788704 Donges Nov 1988 A
4799247 Annis Jan 1989 A
4809312 Annis Feb 1989 A
4825454 Annis Apr 1989 A
4839913 Annis Jun 1989 A
4864142 Gomberg Sep 1989 A
4870670 Geus Sep 1989 A
4884289 Glockmann Nov 1989 A
4979202 Siczek Dec 1990 A
4991189 Boomgaarden Feb 1991 A
5022062 Annis Jun 1991 A
5056129 Steinmeyer Oct 1991 A
5065418 Bermbach Nov 1991 A
5068883 DeHaan Nov 1991 A
5077771 Skillicorn Dec 1991 A
5091924 Bermbach Feb 1992 A
5098640 Gozani Mar 1992 A
5103099 Bourdinaud Apr 1992 A
5179581 Annis Jan 1993 A
5181234 Smith Jan 1993 A
5182764 Peschmann Jan 1993 A
5224144 Annis Jun 1993 A
5237598 Albert Aug 1993 A
5247561 Kotowski Sep 1993 A
5253283 Annis Oct 1993 A
5281820 Groh Jan 1994 A
5302817 Yokota Apr 1994 A
5313511 Annis May 1994 A
5319547 Krug Jun 1994 A
5338927 De Groot Aug 1994 A
5343046 Smith Aug 1994 A
5367552 Peschmann Nov 1994 A
5376795 Hasegawa Dec 1994 A
5379334 Zimmer Jan 1995 A
5391878 Petroff Feb 1995 A
5394454 Harding Feb 1995 A
5420959 Walker May 1995 A
5430787 Norton Jul 1995 A
5446288 Tumer Aug 1995 A
5493596 Annis Feb 1996 A
5524133 Neale Jun 1996 A
5548123 Perez-Mendez Aug 1996 A
5550380 Sugawara Aug 1996 A
5600144 Worstell Feb 1997 A
5600303 Husseiny Feb 1997 A
5600700 Krug Feb 1997 A
5629515 Maekawa May 1997 A
5629523 Ngo May 1997 A
5638420 Armistead Jun 1997 A
5642393 Krug Jun 1997 A
5642394 Rothschild Jun 1997 A
5665969 Beusch Sep 1997 A
5666393 Annis Sep 1997 A
5687210 Maitrejean Nov 1997 A
5692028 Geus Nov 1997 A
5692029 Husseiny Nov 1997 A
5696806 Grodzins Dec 1997 A
5734166 Czirr Mar 1998 A
5751837 Watanabe May 1998 A
5763886 Schulte Jun 1998 A
5764683 Swift Jun 1998 A
5768334 Maitrejean Jun 1998 A
5783829 Sealock Jul 1998 A
5784507 Holm-Kennedy Jul 1998 A
5787145 Geus Jul 1998 A
5805660 Perion Sep 1998 A
5838759 Armistead Nov 1998 A
5856673 Ikegami Jan 1999 A
5866907 Drukier Feb 1999 A
5903623 Swift May 1999 A
5910973 Grodzins Jun 1999 A
5930326 Rothschild Jul 1999 A
5936240 Dudar Aug 1999 A
5940468 Huang Aug 1999 A
5968425 Bross Oct 1999 A
5974111 Krug Oct 1999 A
6018562 Willson Jan 2000 A
6031890 Bermbach Feb 2000 A
6055111 Nomura Apr 2000 A
6058158 Eiler May 2000 A
6067344 Grodzins May 2000 A
6078052 Difilippo Jun 2000 A
6081580 Grodzins Jun 2000 A
6094472 Smith Jul 2000 A
6151381 Grodzins Nov 2000 A
6188747 Geus Feb 2001 B1
6192101 Grodzins Feb 2001 B1
6192104 Adams Feb 2001 B1
6195413 Geus Feb 2001 B1
6198795 Naumann Mar 2001 B1
6203846 Ellingson Mar 2001 B1
6212251 Tomura Apr 2001 B1
6218943 Ellenbogen Apr 2001 B1
6236709 Perry May 2001 B1
6249567 Rothschild Jun 2001 B1
6252929 Swift Jun 2001 B1
6256369 Lai Jul 2001 B1
6278115 Annis Aug 2001 B1
6282260 Grodzins Aug 2001 B1
6292533 Swift Sep 2001 B1
6301326 Bjorkholm Oct 2001 B2
6320933 Grodzins Nov 2001 B1
6333502 Sumita Dec 2001 B1
6356620 Rothschild Mar 2002 B1
6421420 Grodzins Jul 2002 B1
6424695 Grodzins Jul 2002 B1
6434219 Rothschild Aug 2002 B1
6435715 Betz Aug 2002 B1
6442233 Grodzins Aug 2002 B1
6445765 Frank Sep 2002 B1
6453003 Springer Sep 2002 B1
6453007 Adams Sep 2002 B2
6456684 Mun Sep 2002 B1
6459761 Grodzins Oct 2002 B1
6459764 Chalmers Oct 2002 B1
6473487 Le Oct 2002 B1
RE37899 Grodzins Nov 2002 E
6483894 Hartick Nov 2002 B2
6507025 Verbinski Jan 2003 B1
6532276 Hartick Mar 2003 B1
6542574 Grodzins Apr 2003 B2
6542578 Ries Apr 2003 B2
6542580 Carver Apr 2003 B1
6543599 Jasinetzky Apr 2003 B2
6546072 Chalmers Apr 2003 B1
6552346 Verbinski Apr 2003 B2
6556653 Hussein Apr 2003 B2
6563903 Kang May 2003 B2
6567496 Sychev May 2003 B1
6580778 Meder Jun 2003 B2
6584170 Aust Jun 2003 B2
6597760 Beneke Jul 2003 B2
6606516 Levine Aug 2003 B2
6621888 Grodzins Sep 2003 B2
6636581 Sorenson Oct 2003 B2
6637266 Froom Oct 2003 B1
6645656 Chen Nov 2003 B1
6645657 Huang Nov 2003 B2
6653588 Gillard-Hickman Nov 2003 B1
6658087 Chalmers Dec 2003 B2
6663280 Doenges Dec 2003 B2
6665373 Kotowski Dec 2003 B1
6665433 Roder Dec 2003 B2
6687326 Bechwati Feb 2004 B1
6747705 Peters Jun 2004 B2
6763635 Lowman Jul 2004 B1
6785357 Bernardi Aug 2004 B2
6812426 Kotowski Nov 2004 B1
6816571 Bijjani Nov 2004 B2
6837422 Meder Jan 2005 B1
6839403 Kotowski Jan 2005 B1
6843599 Le Jan 2005 B2
6859607 Sugihara Feb 2005 B2
6876719 Ozaki Apr 2005 B2
6879657 Hoffman Apr 2005 B2
6909770 Schramm Jun 2005 B2
6920197 Kang Jul 2005 B2
6922457 Nagata Jul 2005 B2
6965662 Eppler Nov 2005 B2
7010094 Grodzins Mar 2006 B2
7039159 Muenchau May 2006 B2
7067079 Bross Jun 2006 B2
7072440 Mario Jul 2006 B2
7099434 Adams Aug 2006 B2
7103137 Seppi Sep 2006 B2
7110493 Kotowski Sep 2006 B1
7115875 Worstell Oct 2006 B1
RE39396 Swift Nov 2006 E
7162005 Bjorkholm Jan 2007 B2
7190758 Hagiwara Mar 2007 B2
7203276 Arsenault Apr 2007 B2
7207713 Lowman Apr 2007 B2
7215737 Li May 2007 B2
7217929 Hirai May 2007 B2
7218704 Adams May 2007 B1
7233645 Feda Jun 2007 B2
7253727 Jenkins Aug 2007 B2
7308076 Studer Dec 2007 B2
7322745 Agrawal Jan 2008 B2
7326933 Katagiri Feb 2008 B2
7333587 De Feb 2008 B2
7333588 Mistretta Feb 2008 B2
7366282 Peschmann Apr 2008 B2
7369463 Van Dullemen May 2008 B1
7369643 Kotowski May 2008 B2
7379530 Hoff May 2008 B2
7400701 Cason Jul 2008 B1
7403588 Bruder Jul 2008 B2
7409033 Zhu Aug 2008 B1
7409042 Bertozzi Aug 2008 B2
7417440 Peschmann Aug 2008 B2
7486768 Allman Feb 2009 B2
7496178 Turner Feb 2009 B2
7505556 Chalmers Mar 2009 B2
7505562 Dinca Mar 2009 B2
7508910 Safai Mar 2009 B2
7517149 Agrawal Apr 2009 B2
7519148 Kotowski Apr 2009 B2
7538325 Mishin May 2009 B2
7551715 Rothschild Jun 2009 B2
7551718 Rothschild Jun 2009 B2
7555099 Rothschild Jun 2009 B2
7579845 Peschmann Aug 2009 B2
7583779 Tkaczyk Sep 2009 B2
7593506 Cason Sep 2009 B2
7593510 Rothschild Sep 2009 B2
7630472 Tsuyuki Dec 2009 B2
7672422 Seppi Mar 2010 B2
7711090 Schweizer May 2010 B2
7720195 Allman May 2010 B2
7742557 Brunner Jun 2010 B2
7742568 Smith Jun 2010 B2
7783004 Kotowski Aug 2010 B2
7783005 Kaval Aug 2010 B2
7796733 Hughes Sep 2010 B2
7796734 Mastronardi Sep 2010 B2
7809109 Mastronardi Oct 2010 B2
7817776 Agrawal Oct 2010 B2
7848480 Nakanishi Dec 2010 B2
7856079 Nielsen Dec 2010 B2
7856081 Peschmann Dec 2010 B2
7864920 Rothschild Jan 2011 B2
7876880 Kotowski Jan 2011 B2
7924979 Rothschild Apr 2011 B2
7963695 Kotowski Jun 2011 B2
7995705 Allman Aug 2011 B2
7995707 Rothschild Aug 2011 B2
8000436 Seppi Aug 2011 B2
8045781 Nakanishi Oct 2011 B2
8054938 Kaval Nov 2011 B2
8094774 Noshi Jan 2012 B2
8135110 Morton Mar 2012 B2
8135112 Hughes Mar 2012 B2
8138770 Peschmann Mar 2012 B2
8148693 Ryge Apr 2012 B2
8194822 Rothschild Jun 2012 B2
8199996 Hughes Jun 2012 B2
8275091 Morton Sep 2012 B2
8275092 Zhang Sep 2012 B1
8300763 Shedlock Oct 2012 B2
8325871 Grodzins Dec 2012 B2
8331535 Morton Dec 2012 B2
8345819 Mastronardi Jan 2013 B2
8389942 Morton Mar 2013 B2
8401147 Ryge Mar 2013 B2
8428217 Peschmann Apr 2013 B2
8433036 Morton Apr 2013 B2
8439565 Mastronardi May 2013 B2
8442186 Rothschild May 2013 B2
8451974 Morton May 2013 B2
8457274 Arodzero Jun 2013 B2
8483356 Bendahan Jul 2013 B2
8503605 Morton Aug 2013 B2
8503606 Rothschild Aug 2013 B2
8532823 McElroy Sep 2013 B2
8576982 Gray Nov 2013 B2
8582720 Morton Nov 2013 B2
8605859 Mastronardi Dec 2013 B2
8638904 Gray Jan 2014 B2
8668386 Morton Mar 2014 B2
8690427 Mastronardi Apr 2014 B2
8731137 Arroyo May 2014 B2
8735833 Morto May 2014 B2
8750452 Kaval Jun 2014 B2
8750454 Gozani Jun 2014 B2
8774357 Morton Jul 2014 B2
8774362 Hughes Jul 2014 B2
8798232 Bendahan Aug 2014 B2
8804899 Morton Aug 2014 B2
8824632 Mastronardi Sep 2014 B2
8831176 Morto Sep 2014 B2
8842808 Rothschild Sep 2014 B2
8861684 Al-Kofahi Oct 2014 B2
8884236 Rothschild Nov 2014 B2
8885794 Morton Nov 2014 B2
8903045 Schubert Dec 2014 B2
8903046 Morton Dec 2014 B2
8908831 Bendahan Dec 2014 B2
8923481 Schubert Dec 2014 B2
8929509 Morton Jan 2015 B2
8958526 Morton Feb 2015 B2
8971487 Mastronardi Mar 2015 B2
8993970 Morton Mar 2015 B2
8995619 Gray Mar 2015 B2
9014339 Grodzins Apr 2015 B2
9020100 Mastronardi Apr 2015 B2
9020103 Grodzins Apr 2015 B2
9042511 Peschmann May 2015 B2
9052271 Grodzins Jun 2015 B2
9052403 Morton Jun 2015 B2
9057679 Morton Jun 2015 B2
9069101 Arroyo, Jr. Jun 2015 B2
9099279 Rommel Aug 2015 B2
9117564 Rommel Aug 2015 B2
9121958 Morton Sep 2015 B2
9128198 Morton Sep 2015 B2
9146201 Schubert Sep 2015 B2
9158030 Morton Oct 2015 B2
9182516 Gray Nov 2015 B2
9183647 Morton Nov 2015 B2
9207195 Gozani Dec 2015 B2
9208988 Morton Dec 2015 B2
9223050 Kaval Dec 2015 B2
9251915 Lai Feb 2016 B2
9257208 Rommel Feb 2016 B2
9268058 Peschmann Feb 2016 B2
9285325 Gray Mar 2016 B2
9285488 Arodzero Mar 2016 B2
9291582 Grodzins Mar 2016 B2
9291741 Gray Mar 2016 B2
9306673 Macrae Apr 2016 B1
9316760 Bendahan Apr 2016 B2
9417060 Schubert Aug 2016 B1
9465135 Morton Oct 2016 B2
9466456 Rommel Oct 2016 B2
9535019 Rothschild Jan 2017 B1
9541510 Arodzero Jan 2017 B2
9562866 Morton Feb 2017 B2
9576766 Morton Feb 2017 B2
9606245 Czarnecki Mar 2017 B1
9606259 Morton Mar 2017 B2
9632205 Morton Apr 2017 B2
9658343 Arodzero May 2017 B2
9791590 Morton Oct 2017 B2
9823201 Morton Nov 2017 B2
9841386 Grodzins Dec 2017 B2
9915752 Peschmann Mar 2018 B2
9958569 Morton May 2018 B2
10134254 Jarvi Nov 2018 B2
10168445 Morton Jan 2019 B2
10209372 Arodzero Feb 2019 B2
10228487 Mastronardi Mar 2019 B2
10266999 Rothschild Apr 2019 B2
10295483 Morton May 2019 B2
10408967 Morton Sep 2019 B2
10670740 Couture Jun 2020 B2
10724192 Rothschild Jul 2020 B2
10762998 Rothschild Sep 2020 B2
10770195 Rothschild Sep 2020 B2
10794843 Rothschild Oct 2020 B2
10830911 Couture Nov 2020 B2
10976465 Morton Apr 2021 B2
11143783 Morton Oct 2021 B2
20010016028 Adams Aug 2001 A1
20010046275 Hussein Nov 2001 A1
20020082492 Grzeszczuk Jun 2002 A1
20020085674 Price Jul 2002 A1
20020117625 Pandelisev Aug 2002 A1
20020121604 Katagiri Sep 2002 A1
20030002628 Wilson Jan 2003 A1
20030223549 Winsor Dec 2003 A1
20040004482 Bouabdo Jan 2004 A1
20040057554 Bjorkholm Mar 2004 A1
20040086078 Adams May 2004 A1
20040104347 Bross Jun 2004 A1
20040109653 Kerr Jun 2004 A1
20040136493 Konno Jul 2004 A1
20040140431 Schmand Jul 2004 A1
20040141584 Bernardi Jul 2004 A1
20040218714 Faust Nov 2004 A1
20040251415 Verbinski Dec 2004 A1
20040256565 Adams Dec 2004 A1
20050018814 Kerschner Jan 2005 A1
20050053199 Miles Mar 2005 A1
20050073740 Phillips Apr 2005 A1
20050078793 Ikeda Apr 2005 A1
20050100124 Hsieh May 2005 A1
20050135560 Dafni Jun 2005 A1
20050185757 Kresse Aug 2005 A1
20050190878 De Man Sep 2005 A1
20050226371 Kautzer Oct 2005 A1
20050236577 Katagiri Oct 2005 A1
20060078091 Lasiuk Apr 2006 A1
20060251211 Grodzins Nov 2006 A1
20070009088 Edic Jan 2007 A1
20070019781 Haras Jan 2007 A1
20070029493 Kniss Feb 2007 A1
20070098142 Rothschild May 2007 A1
20070206726 Lu Sep 2007 A1
20070222981 Ponsardin Sep 2007 A1
20070235655 Rhiger Oct 2007 A1
20070237294 Hoff Oct 2007 A1
20070258562 Dinca Nov 2007 A1
20070280417 Kang Dec 2007 A1
20080002806 Nishide Jan 2008 A1
20080037707 Rothschild Feb 2008 A1
20080043913 Annis Feb 2008 A1
20080099692 Poreira May 2008 A1
20080152081 Cason Jun 2008 A1
20080197279 Kang Aug 2008 A1
20080219804 Chattey Sep 2008 A1
20080273652 Arnold Nov 2008 A1
20090067575 Seppi Mar 2009 A1
20090086907 Smith Apr 2009 A1
20090103686 Rothschild Apr 2009 A1
20090116617 Mastronardi May 2009 A1
20090188379 Hiza Jul 2009 A1
20090230295 Waring Sep 2009 A1
20090230925 Nathan Sep 2009 A1
20090257555 Chalmers Oct 2009 A1
20090268871 Rothschild Oct 2009 A1
20090274270 Kotowski Nov 2009 A1
20090309034 Yoshida Dec 2009 A1
20100061509 Raymond Mar 2010 A1
20100069721 Webler Mar 2010 A1
20100072398 Fruehauf Mar 2010 A1
20100108859 Andressen May 2010 A1
20100270462 Nelson Oct 2010 A1
20100276602 Clothier Nov 2010 A1
20100314546 Ronda Dec 2010 A1
20110079726 Kusner Apr 2011 A1
20110110490 Samant May 2011 A1
20110204243 Bendahan Aug 2011 A1
20110206179 Bendahan Aug 2011 A1
20110215222 Eminoglu Sep 2011 A1
20110309253 Rothschild Dec 2011 A1
20110309257 Menge Dec 2011 A1
20120033791 Mastronardi Feb 2012 A1
20120061575 Dunleavy Mar 2012 A1
20120076257 Star-Lack Mar 2012 A1
20120104265 Workman May 2012 A1
20120147987 Calderbank Jun 2012 A1
20120148020 Arroyo, Jr. Jun 2012 A1
20120199753 Chuang Aug 2012 A1
20120241628 Hesser Sep 2012 A1
20120280132 Nakamura Nov 2012 A1
20120298864 Morishita Nov 2012 A1
20130039463 Mastronardi Feb 2013 A1
20130156156 Roe Jun 2013 A1
20130195248 Rothschild Aug 2013 A1
20130202089 Schubert Aug 2013 A1
20130208857 Arodzero Aug 2013 A1
20130315368 Turner Nov 2013 A1
20140105367 Horvarth Apr 2014 A1
20140133631 Wood May 2014 A1
20140182373 Sbihli Jul 2014 A1
20150016794 Mori Jan 2015 A1
20150055751 Funk Feb 2015 A1
20150060673 Zimdars Mar 2015 A1
20150168589 Morton Jun 2015 A1
20160025888 Peschmann Jan 2016 A1
20160025889 Morton Jan 2016 A1
20160033426 Georgeson Feb 2016 A1
20160106384 Park Apr 2016 A1
20160170044 Arodzero Jun 2016 A1
20160170077 Morton Jun 2016 A1
20160223706 Franco Aug 2016 A1
20170023695 Zhang Jan 2017 A1
20170045630 Simon Feb 2017 A1
20170059739 Mastronardi Mar 2017 A1
20170184516 Chen Jun 2017 A1
20170245819 Rothschild Aug 2017 A1
20170299526 Morton Oct 2017 A1
20170299764 Morton Oct 2017 A1
20170315242 Arodzero Nov 2017 A1
20170358380 Rothschild Dec 2017 A1
20180038969 McCollough Feb 2018 A1
20180038988 Morton Feb 2018 A1
20180128935 Morton May 2018 A1
20180136340 Nelson May 2018 A1
20180252841 Grodzins Sep 2018 A1
20180284316 Morton Oct 2018 A1
20180286624 Rommel Oct 2018 A1
20180294066 Rothschild Oct 2018 A1
20180313770 Morton Nov 2018 A1
20180328861 Grodzins Nov 2018 A1
20190139385 Jarvi May 2019 A1
20190293810 Couture Sep 2019 A1
20190346382 Rothschild Nov 2019 A1
20190383953 Arodzero Dec 2019 A1
20190391280 Couture Dec 2019 A1
20200025955 Gozani Jan 2020 A1
20200033274 Couture Jan 2020 A1
20200073008 Parikh Mar 2020 A1
20200103357 Morton Apr 2020 A1
20200103547 Morton Apr 2020 A1
20200158908 Morton May 2020 A1
20200191991 Morton Jun 2020 A1
20200233100 Rothschild Jul 2020 A1
20200326291 Rothschild Oct 2020 A1
20200326436 Couture Oct 2020 A1
20200355631 Yu Nov 2020 A1
20200355632 Morton Nov 2020 A1
20210018650 Morton Jan 2021 A1
20210132239 Couture May 2021 A1
Foreign Referenced Citations (95)
Number Date Country
1270318 Oct 2000 CN
1493176 Apr 2004 CN
1745296 Mar 2006 CN
101142497 Mar 2008 CN
101166469 Apr 2008 CN
101578534 Nov 2009 CN
102519988 Jun 2012 CN
104204854 Dec 2014 CN
107193034 Sep 2017 CN
107209282 Sep 2017 CN
2639631 Mar 1978 DE
4017100 Dec 1990 DE
102013102749 Oct 2013 DE
113291 Jul 1984 EP
0261984 Mar 1988 EP
0813692 Dec 1997 EP
0864884 Sep 1998 EP
0971215 Jan 2000 EP
1168249 Jan 2002 EP
1135700 Mar 2005 EP
1254384 Jan 2008 EP
2054741 May 2009 EP
1733213 Feb 2010 EP
2049888 May 2014 EP
3271709 Jan 2018 EP
2492159 Apr 1982 FR
1505498 Mar 1978 GB
2084829 Apr 1982 GB
2150526 Jul 1985 GB
2277013 Oct 1994 GB
2400480 Oct 2004 GB
2482024 Jan 2012 GB
58103678 Jun 1983 JP
62147349 Jul 1987 JP
S63299100 Dec 1988 JP
10232284 Feb 1997 JP
H09318757 Dec 1997 JP
H10185842 Jul 1998 JP
H10232284 Sep 1998 JP
2000515629 Nov 2000 JP
2002071816 Mar 2002 JP
2004045250 Feb 2004 JP
2006505805 Feb 2006 JP
2013205122 Oct 2013 JP
3195776 Feb 2015 JP
9701089 Jan 1997 WO
1997001089 Jan 1997 WO
9802763 Jan 1998 WO
1998003889 Jan 1998 WO
9805946 Feb 1998 WO
1998020366 May 1998 WO
9913323 Mar 1999 WO
1999039189 Aug 1999 WO
2000033060 Jun 2000 WO
2000037928 Jun 2000 WO
0159485 Aug 2001 WO
0173415 Oct 2001 WO
02091023 Nov 2002 WO
03075037 Sep 2003 WO
2004010127 Jan 2004 WO
2004043740 May 2004 WO
2005079437 Sep 2005 WO
2005098400 Oct 2005 WO
2005103759 Nov 2005 WO
2006111323 Oct 2006 WO
2006137932 Dec 2006 WO
2007051092 May 2007 WO
2008021807 Feb 2008 WO
2008024825 Feb 2008 WO
2008063695 May 2008 WO
2008105782 Sep 2008 WO
2009027667 Mar 2009 WO
2009067394 May 2009 WO
2010129926 Nov 2010 WO
2011008718 Jan 2011 WO
2011011583 Jan 2011 WO
2011014445 Feb 2011 WO
2011053972 May 2011 WO
2011149566 Dec 2011 WO
2011163108 Dec 2011 WO
2012058207 May 2012 WO
2012109307 Aug 2012 WO
2012142453 Oct 2012 WO
2012142456 Oct 2012 WO
2012174265 Dec 2012 WO
2013112819 Aug 2013 WO
2013116058 Aug 2013 WO
2013116549 Aug 2013 WO
2013122763 Aug 2013 WO
2014058495 Apr 2014 WO
2016003547 Jan 2016 WO
2016081881 May 2016 WO
2018064434 Apr 2018 WO
2019217596 Nov 2019 WO
2020041161 Feb 2020 WO
Non-Patent Literature Citations (104)
Entry
International Search Report for PCT/US2016/023240, dated Jul. 12, 2016.
Nittoh et al., “Discriminated neutron and X-ray radiography using multi-color scintillation detector,” Nuclear Instruments and Methods in Physics Research A, vol. 428, pp. 583-588 (1999).
Novikov, “A method for monitoring of Gd concentration in Gd-loaded scintillators,” Nuclear Instruments and Methods in Physics Research A, vol. 366, pp. 413-414 (1995).
International Search Report for PCT/US17/54211, dated Jan. 18, 2018.
Osswald et al. “Injection Molding Handbook”, p. 394, Chemical Industry Press, Mar. 31, 2005.
Yoshiaki et al. “Development of ultra-high sensitivity bioluminescent enzyme immunoassay for prostate-specific antigen (PSA) using firefly luciferas”, Abstract, Luminescence, vol. 16, Issue 4, Jul. 31, 2001.
International Search Report for PCT/US01/09784, dated Jan. 28, 2002.
International Search Report for PCT/US02/13595, dated Aug. 6, 2002.
International Search Report for PCT/US03/35232, dated Nov. 8, 2004.
International Search Report for PCT/US03/05958, dated Jun. 27, 2003.
International Search Report for PCT/US2005/011382, dated Oct. 21, 2005.
International Seach Report for PCT/US2008/083741, dated Oct. 30, 2009.
International Search Report for PCT/US2007/066936, dated Sep. 30, 2008.
International Search Report for PCT/US2006/060158, dated Jul. 5, 2007.
International Search Report for PCT/US2007/076497, dated Jul. 28, 2008.
International Search Report for PCT/US2007/075323, dated Feb. 5, 2008.
International Search Report for PCT/US2010/043201, dated Oct. 29, 2010.
International Search Report for PCT/US2012/024248, dated Jul. 9, 2012.
International Search Report for PCT/US11/23143, dated Nov. 25, 2011.
International Search Report for PCT/US2012/033581, dated Oct. 31, 2012.
International Search Report for PCT/US2011/041033, dated Feb. 17, 2012.
International Search Report for PCT/US2012/033585, dated Nov. 29, 2012.
International Search Report for PCT/US2013/022715, dated May 15, 2013.
International Search Report for PCT/US2015/031115, dated Jul. 29, 2015.
Rose, Kathryn, “NuMI Off-Axis Experiment” Datasheet (online). University of Oxford & Rutherford Appleton Laboratory, 2003. <URL: https://slideplayer.com/slide/8765673/>.
International Search Report for PCT/US2019/027252, dated Aug. 2, 2019.
Williams et al.:“PET Detector Using Waveshifting Optical Fibers and Microchannel Plate PMT with Delay Line Readout”, IEEE Transactions on Nuclear Science, IEEE Service Center, New York, NY, US, vol. 45, No. 2, Apr. 1, 1998 (Apr. 1, 1998), pp. 195-205, XP011087844, ISSN: 0018-9499, DOI: 10.1109/23.664171.
Beznosko et al., “FNAL-NICADD Extruded Scintillator,” FERMILAB-CONF-04-216-E, pp. 1-4 (Sep. 2004).
Case et al., “Wavelength-shifting fiber readout of LaC13 and LaBr3 scintillators,” Proc. of SPIE, vol. 5898, UV, X-Ray, and Gamma-Ray Space Instrumentation for Astronomy XIV, pp. 58980K-1-58980K-8 (2005).
Gundiah, “Scintillation properties of Eu.sup.2+-activated barium fluoroiodide,” Lawrence Berkeley National Laboratory, pp. 1-10 (Feb. 2011).
Hutchinson et al., “Optical Readout for Imaging Neutron Scintillation Detectors,” Engineering Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee, 6 pages. (Nov. 2002).
Keizer, “The optimal cosmic ray detector for High-Schools,” 21 pages (2011).
Maekawa et al., “Thin Beta-ray Detectors using Plastic Scintillator Combined with Wavelength-shifting Fibers for Surface Contamination Monitoring,” J. Nucl. Sci. Technol., vol. 35, No. 12, pp. 886-894 (Dec. 1998).
Moiseev et al., “High-efficiency plastic scintillator detector with wavelength-shifting fiber readout for the GLAST Large Area Telescope,” Nucl. Instrum. Meth. Phys. Res. A, vol. 583, pp. 372-381 (2007).
Pla-Dalmau et al., “Extruded Plastic Scintillator for MINERvA,” FERMILAB-CONF-05-506-E, pp. 1298-1300 (2005).
Yoshimura et al., “Plastic scintillator produced by the injection-molding technique,” Nucl. Instr. Meth. Phys. Res. A, vol. 406, pp. 435-441 (1998).
Jae Yul Ahn, Authorized officer Korean Intellectual Property Office, International Search Report—Application No. PCT/US2013/024585, dated Jun. 2, 2013, along with Written Opinion of the International Searching Authority.
Nishikido et al. “X-ray detector made of plastic scintillators and WLS fiber for real-time dose distribution monitoring in interventional radiology,” IEEE Nuclear Science Symposium and Medical Imaging Conference Reco, pp. 1272-1274 (2012).
International Search Report for PCT/US2019/027242, dated Jul. 17, 2019.
International Search Report for PCT/US2013/024585, dated Jun. 2, 2013.
https://en.wikipedia.org/wiki/ISM_band#Common_non-ISM_uses., downloaded from Internet Nov. 23, 2020.
International Search Report for PCT/US2013/023125, dated May 15, 2013.
International Search Report for PCT/US99/29185, dated Sep. 27, 2000.
Chou, C, “Fourier coded-aperture imaging in nuclear medicine”, IEEE Proc. Sci. Meas. Technol., vol. 141. No. 3, May 1994, pp. 179-184.
Mertz, L.N., et al., “Rotational aperture synthesis for x rays”, Journal. Optical Society of America, vol. 3, Dec. 1986, pp. 2167-2170.
International Bureau of WIPO, International Preliminary Report on Patentability, PCT/US2005/011382, dated Oct. 19, 2006, 7 pages.
International Search Report and Written Opinion for PCT/US2010/041757, dated Oct. 12, 2010.
European Patent Office, International Search Report, International Application No. PCT/US99/28266, dated Sep. 6, 2000, 3 pages.
Written Opinion of the International Searching Authority, PCT/US2007/066936, dated Sep. 30, 2008, 7 pages.
International Search Report, PCT/US1999/028035, dated Sep. 15, 2000, 6 pages.
International Search Report, PCT/US1998/18642, dated Jul. 7, 1999, 4 pages.
International Search Report, PCT/US2007/066936; dated: Sep. 30, 2008, 5 pages.
European Patent Office, International Search Report and Written Opinion of the International Searching Authority, PCT/US2005/011382, dated Oct. 21, 2005.
Non-Final Office Action for U.S. Appl. No. 11/737,317, filed Mar. 25, 2008.
Applicant Response to Non-Final Office Action for U.S. Appl. No. 11/737,317, filed Apr. 30, 2008.
Notice of Allowance for U.S. Appl. No. 11/737,317, filed Sep. 9, 2008.
Information Disclosure Statement for U.S. Appl. No. 11/737,317, Nov. 6, 2008.
Notice of Allowance for U.S. Appl. No. 11/737,317, filed Nov. 20, 2008.
Non-Final Office Action for U.S. Appl. No. 11/097,092, filed May 15, 2006.
Applicant Response to Non-Final Office Action for U.S. Appl. No. 11/097,092, filed Aug. 31, 2006.
Non-Final Office Action for U.S. Appl. No. 11/097,092, filed Nov. 22, 2006.
Applicant Response to Non-Final Office Action for U.S. Appl. No. 11/097,092, filed Mar. 13, 2007.
Final Office Action for U.S. Appl. No. 11/097,092, filed Mar. 21, 2007.
Applicant Response to Final Office Action for U.S. Appl. No. 11/097,092, filed Jun. 18, 2007.
Advisory Action Before the Filing of an Appeal Brief for U.S. Appl. No. 11/097,092, filed Jun. 21, 2007.
Applicant Response to Final Office Action and Advisory Action for U.S. Appl. No. 11/097,092, filed Jul. 3, 2007.
Non-Final Office Action for U.S. Appl. No. 11/097,092, filed Aug. 20, 2007.
Applicant Response to Non-Final Office Action for U.S. Appl. No. 11/097,092, filed Nov. 2, 2007.
Notice of Allowance for U.S. Appl. No. 11/097,092, filed Mar. 24, 2008.
Certificate of Correction for U.S. Pat. No. 7,400,701, Jul. 15, 2008.
Notice of Allowance for U.S. Appl. No. 12/841,401, filed Jun. 26, 2012.
International Search Report for PCT/US20/61866, dated Feb. 11, 2021.
Roderick D. Swift, Roy P. Lindquist, “Medium energy x-ray examination of commercial trucks”, Proc. SPIE 2276, Cargo Inspection Technologies, (Oct. 6, 1994); doi: 10.1117/12.189174.
Zhang et al., “A multi-beam x-ray imaging system based on carbon nanotube field emitters”, Proceedings of SPIE vol. 6142, 614204, (2006), doi: 10.1117/12.654006.
Declaration of Richard Lanza, Ph.D. , Case No. IPR2022-00028; U.S. Pat. No. 7,505,562, Oct. 28, 2021.
Cheng et al., “Dynamic radiography using a carbonnanotube-based field emission x-ray source,” Review of Scientific Instruments, vol. 75, No. 10. Oct. 2004.
Zhang et al., “Stationary scanning x-ray source based on carbon nanotube field emitters”, Applied Physics Letters 86, 184104 (2005).
Zhang et al., “A nanotube-based field emission x-ray source for microcomputed tomography ”, Review of Scientific Instruments 76, 094301 (2005).
U.S. Appl. No. 60/737,471, filed Mar. 31, 2006.
U.S. Appl. No. 60/787,810, filed Apr. 1, 2005.
AS& E's Opposition to Viken's Motion for Rule 11 Sanctions, Dkt. 38, Case 1:20-cv-11883 (Dist. Of Mass.), Feb. 26, 2021.
Viken's Memorandum of Law In Support of Defendant's Motion for Rule 11 Sanctions, Dkt. 30, Case 1:20-cv-11883 (Dist. Of Mass.), Feb. 8, 2021.
Motion Hearing Transcript, dated Aug. 16, 2021, Case 1:20-cv-11883 (Dist. Of Mass.).
Waiver of the Service of Summons, Oct. 20, 2020; Dkt. 6, Case 1:20-cv-11883, (Dist. Of Mass.).
Evans, R. D., The Atomic Nucleus, Ch. 23-25, & Appendix A, TATA McGraw-Hill, Bombay, New Delhi (1955).
Knoll, G. F., Radiation Detection and Measurements, Ch. 2, 4, 8, & 9, Third Edition, John Wiley & Sons, Inc. New York (2000).
Johns, H., & Cunningham J. R., “The Production and Properties of X Rays,” Chapter 2, The Physics of Radiology, Charles C. Thomas Publisher, Springfield, IL, 4th Ed. (1983).
American Science and Engineering, Inc. 2002 Annual Report.
American Science & Engineering, Inc. v. Viken Detection Corp., U.S.D.C. (D. Mass.) Case No. 1:20-cv-11883-LTS, Joint Proposed Scheduling Order (Doc. 63), filed Oct. 12, 2021.
Viken Detection Corporation v. AS&E, Case No. IPR2022-00028, Petition for Inter Partes Review of U.S. Pat. No. 7,505,562, Oct. 28, 2021.
Declaration of Richard C. Lanza, Ph.D.,, Case No. IPR2021-01585; U.S. Pat. No. 7,400,701, Sep. 29, 2021.
Tateno, Y., & Tanaka, H., “Low-Dosage X-Ray Imaging System Employing Flying Spot X-Ray Microbeam (Dynamic Scanner)1,” Radiation Physics, 121(1):189-195 (1976).
Vike Detection Corporation v. AS&E, Case No. IPR2021-01585, Petition for Inter Partes Review of U.S. Pat. No. 7,400,701, Sep. 30, 2021.
Declaration of Richard C. Lanza, Ph.D., Case No. IPR2022-00027, U.S. Pat. No. 8,300,763, Oct. 20, 2021.
U.S. Appl. No. 61/228,335 (priority document for 763 Patent), filed Jul. 24, 2009.
Chapter 10, Ghilani, Adjustment Computations: Spatial Data Analysis, Sixth Edition, 2017 John Wiley & Sons, Inc. (“Weights Of Observations”).
Chambers Dictionary of Science and Tech. (1999) (definition of “weighting observation”).
Tateno, Y., & Tanaka, H., “Low-Dosage X-ray Imaging System Employing Flying Spot X-ray Microbeam (Dynamic Scanner),” Radiation Physics, 121(1):189-195 (1976).
U.S. Appl. No. 61/423,582 (“Gray '582”), filed Dec. 15, 2010.
Viken Detection Corporation v. AS&E, Petition for Inter Partes Review, Case No. IPR2022-00027, U.S. Pat. No. 8,300,763, Oct. 20, 2021.
AS&E v. Viken, Defendant Viken Detection Corp.'s Preliminary Patent Related DisclosuresCase No. 1:20-cv-11833-LTS, United States District Court for the District of Massachusetts, Jan. 7, 2022.
Z Portal for Trucks & Cargo, Multi-View, Multi-Technology, Cargo and Vehicle Screening System, 2022 downloaded from the following URL: https://www.rapiscan-ase.com/products/portal/z-portal-for-trucks-cargoscreening.
Defense Dept, contracts for X-ray tech, Apr. 7, 2009 downloaded from the following URL https://www.upi.com/Defense-News/2009/04/07/Defense-Dept-contracts-for-X-ray-tech/61051239114877/.
AS&E pulls in $4.4M deal from U.S. agency, Apr. 27, 2009, downloaded from the following URL https://www.bizjournals.com/boston/blog/mass-high-tech/2009/04/ase-pulls-in-44m-deal-from-us-agency.html.
Related Publications (1)
Number Date Country
20210349233 A1 Nov 2021 US
Provisional Applications (5)
Number Date Country
62136305 Mar 2015 US
62136299 Mar 2015 US
62136362 Mar 2015 US
62136315 Mar 2015 US
62136322 Mar 2015 US
Continuations (2)
Number Date Country
Parent 16199531 Nov 2018 US
Child 17126342 US
Parent 15074787 Mar 2016 US
Child 16199531 US