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US20110216945A1 - Automated target shape detection for vehicle muon tomography - Google Patents

Automated target shape detection for vehicle muon tomography Download PDF

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US20110216945A1
US20110216945A1 US13/108,978 US201113108978A US2011216945A1 US 20110216945 A1 US20110216945 A1 US 20110216945A1 US 201113108978 A US201113108978 A US 201113108978A US 2011216945 A1 US2011216945 A1 US 2011216945A1
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Holger M. Jaenisch
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Decision Sciences International Corp
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01VGEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
    • G01V5/00Prospecting or detecting by the use of ionising radiation, e.g. of natural or induced radioactivity
    • G01V5/20Detecting prohibited goods, e.g. weapons, explosives, hazardous substances, contraband or smuggled objects
    • GPHYSICS
    • G06COMPUTING OR CALCULATING; COUNTING
    • G06VIMAGE OR VIDEO RECOGNITION OR UNDERSTANDING
    • G06V10/00Arrangements for image or video recognition or understanding
    • G06V10/40Extraction of image or video features
    • G06V10/44Local feature extraction by analysis of parts of the pattern, e.g. by detecting edges, contours, loops, corners, strokes or intersections; Connectivity analysis, e.g. of connected components
    • G06V10/443Local feature extraction by analysis of parts of the pattern, e.g. by detecting edges, contours, loops, corners, strokes or intersections; Connectivity analysis, e.g. of connected components by matching or filtering
    • GPHYSICS
    • G06COMPUTING OR CALCULATING; COUNTING
    • G06VIMAGE OR VIDEO RECOGNITION OR UNDERSTANDING
    • G06V10/00Arrangements for image or video recognition or understanding
    • G06V10/40Extraction of image or video features
    • G06V10/44Local feature extraction by analysis of parts of the pattern, e.g. by detecting edges, contours, loops, corners, strokes or intersections; Connectivity analysis, e.g. of connected components
    • G06V10/457Local feature extraction by analysis of parts of the pattern, e.g. by detecting edges, contours, loops, corners, strokes or intersections; Connectivity analysis, e.g. of connected components by analysing connectivity, e.g. edge linking, connected component analysis or slices
    • GPHYSICS
    • G06COMPUTING OR CALCULATING; COUNTING
    • G06VIMAGE OR VIDEO RECOGNITION OR UNDERSTANDING
    • G06V20/00Scenes; Scene-specific elements
    • G06V20/50Context or environment of the image
    • G06V20/52Surveillance or monitoring of activities, e.g. for recognising suspicious objects
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N9/00Investigating density or specific gravity of materials; Analysing materials by determining density or specific gravity
    • G01N9/24Investigating density or specific gravity of materials; Analysing materials by determining density or specific gravity by observing the transmission of wave or particle radiation through the material
    • GPHYSICS
    • G06COMPUTING OR CALCULATING; COUNTING
    • G06VIMAGE OR VIDEO RECOGNITION OR UNDERSTANDING
    • G06V2201/00Indexing scheme relating to image or video recognition or understanding
    • G06V2201/05Recognition of patterns representing particular kinds of hidden objects, e.g. weapons, explosives, drugs

Definitions

  • This application relates to techniques, apparatus and systems for vehicle muon tomography imaging.
  • Muon tomography is an imaging technique that produces an image of an object such as a vehicle or its contents based on detection of the scattering of cosmic ray produced muons as they pass through the object. Muons scattered by an object can be detected and the detected signals can be processed to provide specific density and three-dimensional imaging of materials.
  • Muons penetrate through the atmosphere and into the ground at the rate of approximately 1 per square centimeter per minute. Muons can be thought of as much larger cousins of the electrons that are an essential part of ordinary matter. Energetic muons interact strongly enough with matter by ionization to be easily detected, and can penetrate large thicknesses without significant impairment.
  • Physicists at the Los Alamos National Laboratory have developed techniques for detecting scattering of cosmic ray produced muons to produce tomographic images of an object exposed to the cosmic ray muons. See, e.g., Priedhorsky et al., “Detection of high-Z objects using multiple scattering of cosmic ray muons”, Proceedings of SPIE Press, Vol. 5199A-39 (March, 2003).
  • Coulomb scattering of the charges of subatomic particles perturb its trajectory. The total deflection depends on several material properties, but the dominant parameters are the atomic number, Z, of the nuclei and the material density.
  • the LANL techniques are based on precise reconstruction of individual muon tracks and are capable of detecting and visually representing potential threat objects in vehicles or transportable containers in order to alert responsible authorities, thereby allowing them to preemptively interdict the movement of such material to prevent any damage and destruction.
  • a vehicle muon tomography system can be constructed based on the LANL techniques to provide hazard detection at various locations including ports and checkpoints. For example, such systems can provide the Department of Homeland Security (DHS) with an effective solution to the critical need for timely vehicle and cargo inspection nationwide.
  • DHS Department of Homeland Security
  • This specification describes techniques, apparatus and systems for vehicle muon tomography imaging using autonomous processing of 3-dimensional (3D) muon tomography vehicle images based on Data Modeling techniques and various applications including analyzing vehicle voxel data such as muon vehicle images to detect potential threat objects within a vehicle or transportable container and then to further discriminate the identified potential threat objects by shape.
  • a computer-automated method for processing muon vehicle imaging data of a vehicle inspection region within a vehicle muon tomography imaging system includes processing muon vehicle imaging data obtained from the vehicle inspection region to obtain a histogram of the muon vehicle imaging data at different positions in the vehicle inspection region; separating the muon vehicle imaging data into bins based on the histogram; removing a subset of the muon vehicle imaging data in a mode bin that has higher frequencies of occurrence than remaining muon vehicle imaging data from the muon vehicle imaging data to retain the remaining muon vehicle imaging data for further processing; determining an optimal number of bins for separating the remaining muon vehicle imaging data into data bins; processing the remaining muon vehicle imaging data to obtain a histogram of the remaining muon vehicle imaging data at different positions in the vehicle inspection region; separating the remaining muon vehicle imaging data into data bins at the optimal number of bins; and removing data in a mode bin that has higher frequencies of occurrence than the rest of the remaining muon vehicle imaging data to retain remaining mu
  • This method also includes using a background recognizer Data Model for identifying background vehicle structure from the target detection data; applying the background recognizer Data Model to process the remaining muon vehicle imaging data to produce an image of the vehicle inspection region by removing background structure; using a target identification Data Model for identifying a target object from the target detection data; applying the target identification Data Model to process data of the image produced after applying the background recognizer Data Model to produce an image of the target object; and processing the image of the target object to determine a location and a shape of the target object in the vehicle inspection region.
  • a computer system for processing muon vehicle imaging data of a vehicle inspection region within a muon tomography vehicle imaging system includes means for processing muon vehicle imaging data obtained from the vehicle inspection region to obtain a histogram of the muon vehicle imaging data at different positions in the vehicle inspection region; means for separating the muon vehicle imaging data into bins based on the histogram; means for removing a subset of the muon vehicle imaging data in a mode bin that has higher frequencies of occurrence than remaining muon vehicle imaging data from the muon vehicle imaging data to retain the remaining muon vehicle imaging data for further processing; means for determining an optimal number of bins for separating the remaining muon vehicle imaging data into data bins; means for processing the remaining muon vehicle imaging data to obtain a histogram of the remaining muon vehicle imaging data at different positions in the vehicle inspection region; means for separating the remaining muon vehicle imaging data into data bins at the optimal number of bins; and means for removing data in a mode bin that has higher frequencies of occurrence than the rest of the
  • This system also includes means for using a background recognizer Data Model for identifying background structure from the target detection data; means for applying the background recognizer Data Model to process the target detection data to produce an image of the vehicle inspection region by removing identified background structure; means for using a target identification Data Model for identifying a target object from the target detection data; means for applying the target identification Data Model to process data of the image produced after applying the background recognizer Data Model to produce an image of the target object; and means for processing the image of the target object to determine a location and a shape of the target object in the vehicle inspection region.
  • a muon tomography vehicle imaging system in another aspect, is described to include a first set of muon detectors located on a first side of a vehicle inspection region holding a vehicle for inspection, the muon detectors measuring incident muons; a second set of muon detectors located on a second side of the vehicle inspection region opposite to the first side to measure outgoing muons exiting the vehicle inspection region; and a muon tomography control module that receives detector outputs from the first and the second set of muon detectors and processes the detector outputs to produce a 3-dimensional image of the vehicle inspection region.
  • the muon tomography control module includes a suspect object detection module for processing muon vehicle imaging data of the 3-dimensional image.
  • the suspect object detection module includes means for applying Data Models to process the muon vehicle imaging data to isolate one or more target objects from other objects in the vehicle inspection region; means for applying primitive shape recognition to cross-section slices of an image of a volume containing data points of the one or more target objects to identify predetermined primitive shapes; and means for processing identified primitive shapes to construct a 3-dimensional image of each target object.
  • a computer-automated method for processing muon vehicle imaging data from a muon tomography vehicle imaging system includes applying Data Models to process muon tomography vehicle image data to isolate one or more target objects from other objects in a volume under inspection by the muon tomography vehicle imaging system; applying primitive shape recognition to cross-section slices of an image of the volume containing data points of the one or more target objects to identify predetermined primitive shapes; and processing identified primitive shapes to construct a 3-dimensional image of each target object.
  • a computer-implemented method for using natural cosmic muons as a radiation source to obtain muon tomographic images of a vehicle under inspection includes obtaining a cosmic muon tomography vehicle image of a vehicle under inspection; processing vehicle voxel data of each obtained muon vehicle image to compute histogram of the vehicle voxel data of the obtained muon vehicle image; applying statistical processing based on the histogram to the vehicle voxel data to generate a Data Model to monitor one or more changes in the obtained muon vehicle image indicative of presence of a target object in the obtained muon vehicle image; and determining a shape of the target object.
  • a threat object can be identified by autonomous processing without human intervention.
  • Suitable Data Modeling based on statistical process can provide efficient and robust data processing and provide autonomous identification of the shape of a threat object.
  • the present Data Modeling allows for relatively short muon vehicle imaging exposure times in capturing the muon vehicle imaging data without compromising the data processing accuracy and thus allows for high-speed detection.
  • FIG. 1 illustrates an example of a muon tomography vehicle imaging system for inspecting a vehicle for other objects.
  • FIGS. 2A , 2 B and 2 C show examples of muon tomography vehicle images obtained from a LANL-built system with imaging exposure times of 15 seconds, 30 seconds and 60 seconds, respectively.
  • FIG. 3 shows an example of a muon tomography vehicle imaging system implementing autonomous processing of 3D muon tomography vehicle images based on Data Modeling.
  • FIG. 4 shows an example of operation steps performed by the suspect object detection module in FIG. 3 .
  • FIG. 5 shows an exemplary process that implements the processing in FIG. 4 , where the Cartesian coordinates X, Y and Z are defined in FIG. 1 .
  • FIG. 6 shows examples of front view and top view projections of values for the characteristic data.
  • FIGS. 7A , 7 B, 7 C and 7 D show an example for data processing based on the Vehicle Assembly Recognizer Target Identification in FIG. 5 .
  • FIGS. 8A , 8 B and 8 C show Hamming distance curves for a square, circle, and rectangle primitive shapes in the processing in FIG. 5 .
  • FIG. 9 shows an example for data processing to indicate the corresponding primitive shapes for the process in FIG. 5 .
  • Muons contribute roughly a tenth of the natural dose of daily ionizing radiation at the earth's surface and such radiation exposure is a natural and unavoidable feature of our environment.
  • Muon tomography takes advantage of this universal presence and the penetrating characteristics of the muons to reveal the position and size of various materials without causing any harm to personnel or requiring additional intervention by inspectors to correctly identify potential threats.
  • efforts to conceal weapons or other dangerous materials by encasing them in a massive lead container would be just as revealing, since the muon deflection patterns would indicate the presence of shielding material where it didn't belong.
  • FIG. 1 illustrates an example of a muon tomography vehicle imaging system for inspecting a vehicle for other objects.
  • This system for detecting muons includes a vehicle inspection region or volume 130 for placing a vehicle to be inspected.
  • muon detectors 111 , 112 , 121 and 122 are provided to detect the incident muons from the atmosphere at the top of the region 130 and outgoing muons at the bottom of the region 130 .
  • Such muon detectors can be drift tubes that are filled with a gas which can be ionized by muons and are configured to collect and correlate the amount of deflection of each muon that passes through and the vehicle or container being inspected.
  • Multiple drift tubes can be used to form detector arrays to accurately determine a muon's path and, by analyzing the amount of deflection and the pattern of the scattering which results, a visual three-dimensional image of the variety of materials can be generated.
  • the muon detectors 111 , 112 , 121 and 122 include a first set of position-sensitive muon detectors 111 and 112 located on the top side of the vehicle inspection region 130 to measure positions and angles of incident muons, a second set of position sensitive muon detectors 121 and 122 located on the bottom side of the vehicle inspection region 130 opposite to the top side to measure positions and angles of outgoing muons exiting the vehicle inspection region.
  • a muon tomography signal processing unit which may include, e.g., a microprocessor, is provided to receive data of measured signals of the incoming muons from the first set of position sensitive muon detectors 111 and 112 and measured signals of the outgoing muons from the second set of position sensitive muon detectors 121 and 122 .
  • the muon trajectories are more strongly affected by special nuclear material (SNM) and materials that make good gamma ray shielding (such as lead and tungsten) than by the materials that make up more ordinary objects (such as water, plastic, aluminum, and steel).
  • SNM nuclear material
  • materials that make good gamma ray shielding such as lead and tungsten
  • Each muon carries information about the objects that it has penetrated, and by measuring the scattering of multiple muons, one can probe the properties of these objects. In particular, one can detect high-Z objects amongst more typical low-Z and medium-Z matter.
  • FIG. 1 shows a truck that carries a cargo 133 and a shielded crate 134 that conceals a high Z object.
  • the incident cosmic muons 101 are scattered by the truck and everything in the truck.
  • the degrees of scattering of the muons vary with the object or objects in the paths of the muons.
  • the muon rays 141 shown in FIG. 1 represent low scattering muon paths in which truck components or objects have low Z numbers.
  • the truck's engine 131 tends to have higher Z than other vehicle components and thus causes mild scattering of muons as represented by the muon rays 142 .
  • the cargo 133 carried by the truck may also cause mild scattering of muons.
  • the high Z object in the shielded crate 134 cause large scattering 143 of the muons.
  • the muon tomography signal processing unit for the system in FIG. 1 is configured to analyze scattering behaviors of muons, caused by scattering of the muons in the materials within the vehicle inspection region 130 , based on the measured incoming and outgoing positions and angles of muons, to obtain a tomographic profile or the spatial distribution of scattering centers within the vehicle inspection region 130 .
  • the obtained tomographic profile or the spatial distribution of scattering centers can be used to reveal the presence or absence of one or more objects in the vehicle inspection region such as materials with high atomic numbers Z including nuclear materials or devices.
  • the image of a high Z object is part of the generated muon tomography vehicle image and is mixed with images of other objects in the generated muon tomography vehicle image.
  • One technical challenge is to fully autonomously process the muon tomography vehicle images based on computer data processing to identify a threat object in a generated muon tomography vehicle image.
  • FIGS. 2A , 2 B and 2 C show examples of muon tomography vehicle images obtained from the LANL Large Muon Tracker system with imaging exposure times of 15 seconds, 30 seconds and 60 seconds, respectively.
  • FIG. 2A illustrates how in as little as 15 seconds various materials and components, e.g., the engine block, transmission drive train and wheels, can be distinguished—they have been color-coded to provide a visual identification.
  • Techniques, apparatus and systems for muon tomography vehicle imaging can use autonomous processing of 3D muon tomography vehicle images based on discrete and analytical Data Modeling techniques comprising Entropyology or random-field-information science. These Data Modeling techniques were previously developed by Holger M. Jaenisch. These techniques may be used to analyze voxel data such as muon vehicle images to detect potential threat objects and then to further discriminate the identified potential threat objects by shape. Data Modeling uses the smallest amount of entropic information to functionally model empirical dynamics and can take the form of a group of real numbers, a single equation, or a network of equations. A Data Model can also be a variable of another function.
  • a hierarchy of functional models (equations whose variables are themselves equations) can be built up to combine any group or subset of previously derived models.
  • Data Modeling finds a mathematical expression that provides a good model between given finite sample values of the independent variables and the associated values of the dependent variables of the process.
  • the predictive mathematical expression modeling the given sample of data is called a Data Model. This process involves finding both the structural form of the Data Model and the numeric coefficients for the Data Model.
  • the present techniques use Data Modeling methods and can be implemented in ways that minimize long exposure requirements previously reported in the literature and allow for muon vehicle imaging in the gray medium exposure length zone, which is traditionally difficult to automate. Therefore, high-speed and efficient autonomous threat detection can be achieved.
  • FIG. 3 shows an example of a muon tomography vehicle imaging system 300 implementing autonomous processing of 3D muon tomography vehicle images based on Data Modeling.
  • the detector design in this system 300 is based on the design in FIG. 1 and may also be implemented by other muon detector configurations.
  • Input detector readout circuit 310 is connected to the detectors 111 and 112 to receive and pre-process the detector outputs and feeds the pre-processed detector outputs to a muon tomography processing module 330 .
  • Output detector readout circuit 320 is connected to the detectors 121 and 122 to receive and pre-process the detector outputs and also feeds the pre-processed detector outputs to the muon tomography processing module 330 .
  • the muon tomography processing module 330 can include one or more computers or computer processors and has a muon tomography vehicle imaging processing module 331 and a suspect object detection module 332 .
  • the muon tomography vehicle imaging processing module 331 is configured to process the detector outputs from the detectors 111 , 112 , 121 and 122 to generate 3D muon tomography vehicle images of the vehicle inspection region 130 . Examples of such images are shown in FIGS. 2A , 2 B and 2 C.
  • the suspect object detection module 332 receives the voxel data of the 3D muon tomography vehicle images output by the muon tomography vehicle imaging processing module 331 and is programmed to autonomously process 3D muon tomography vehicle images based on Data Modeling. The following sections describe details of operations of the suspect object detection module 332 .
  • the suspect object detection module 332 is configured to include various processing modules and routes to provide a computer-automated method for processing muon vehicle imaging data based on Data Modeling.
  • FIG. 4 shows an example of operation steps performed by the suspect object detection module 332 .
  • the suspect object detection module 332 applies Data Models to process muon tomography vehicle image data from the muon tomography vehicle imaging processing module 331 to isolate one or more target objects from other objects in the vehicle inspection region 130 (step 410 ) and subsequently applies primitive shape recognition to cross-section slices of an image of the volume 130 containing data points of the one or more target objects to identify predetermined primitive shapes (step 420 ).
  • the suspect object detection module 332 processes the identified primitive shapes to construct a 3-dimensional image of each target object.
  • the processing in step 410 can include several processing steps.
  • a background recognizer Data Model for identifying vehicle structures is applied to process the remaining muon vehicle imaging data to produce an image of the volume by removing the identified background structure.
  • a target identification Data Model for identifying the one or more target objects is applied to process data of the image produced after applying the background recognizer Data Model to produce an image of the one or more target objects.
  • the above processing can be performed based on the vehicle voxel data from the muon tomography vehicle imaging processing module 331 and can be achieved without relying on prior samples or data on some pre-selected known threat objects.
  • FIG. 5 shows an exemplary process that implements the processing in FIG. 4 .
  • the Cartesian coordinates X, Y and Z are defined in FIG. 1 .
  • the numerals in FIG. 5 correspond the following processing steps performed by the suspect object detection module 332 :
  • Target Medium Z Identification Decision equation Data Model Apply Target Medium Z Identification Decision equation Data Model to the data after removal of data associated with identified vehicle components.
  • 2D primitive shape recognizer Data Models such as a square shape recognizer Data Model, a rectangle shape recognizer Data Model, and a circle shape recognizer Data Model.
  • step 1 bulk filtering of the vehicle shell is performed by calculating a histogram using 3 bins in step 2.
  • the mode bin one most frequently occurring, or the one with the largest number of points
  • step 2 is removed in step 2
  • step 3 the remainder of the (x,y,z) locations projected onto the XZ plane in step 3.
  • the values in the XZ plane are then projected onto the X-axis of the resulting data sequence graph in step 4, which is characterized by statistics in step 5 and used with a predictive bin estimating equation to determine optimal number of bins in step 6.
  • FIG. 6 shows examples of front view and top view projections of values for the training data.
  • a histogram for the remaining data produced by the step 2 is calculated using the optimal number of bins and the data in the new Mode bin is once again deleted (step 7).
  • the remaining points are processed through the Vehicle Assembly Recognizer Decision equation (using x, y, and z locations along with value) in step 8, and the vehicle components identified are removed in step 9.
  • the remaining points are processed through the Target Identification Decision equation (also using x, y, and z location along with value at each point) in 10. Steps 8 and 10 isolate the candidate target which is extracted in step 11.
  • FIGS. 7A , 7 B, 7 C and 7 D show an example for the above processing based on the Vehicle Assembly Recognizer Decision equation Target Identification Decision equation.
  • FIG. 7A shows the projection of van data onto the XZ plane.
  • FIG. 7B shows the XZ projection of data remaining after histogram.
  • FIG. 7C shows the data after using Vehicle Assembly and Target Identification Data Models, respectively. The points remaining in FIG. 7C are for the potential target.
  • FIG. 7D shows a graph of covariance ellipses for each cross-section neighborhood extracted and processed.
  • the above described vehicle assembly recognizer Data Model is a specific example of a background recognizer Data Model that identifies and recognizes background structure in the muon tomography data images.
  • 2-D primitive shape detection and 3-D overall shape detection are performed.
  • This process begins by extracting all planes, i.e., XY, XZ, and YZ slices that contain one or more of the points. These planes or slices are processed without replacement to extract all 32 ⁇ 32 pixel neighborhoods that contain at least one point.
  • the shape of each neighborhood is characterized by applying the Shape Characterizer in step 13.
  • the resulting sequence is then characterized using descriptive moments and cumulants in step 14 for input into the Shape Recognizers in steps 15, 16, and 17.
  • the number of pixel values in the neighborhood that change between iterations is calculated and stored as a data sequence known as the Hamming distance curves as shown in FIGS. 8A , 8 B and 8 C for the Square, Circle, and Rectangle Shapes.
  • the Hamming sequence is then characterized using statistics. The statistics drive each of the Square, Circle, and Rectangle Shape Recognizers, respectively.
  • the ratio of neighborhoods flagged as square, circle, or rectangle to the total number of extracted neighborhoods is determined.
  • FIG. 9 shows an example for this data processing to indicate the corresponding primitive shapes. If a neighborhood does not flag as any of the 3 primitive shapes, it is labeled as unrecognized.
  • the Volumetric Shape Recognizer in step 18 uses the ratio of squares, circles, and rectangles flagged to total number of neighborhoods as input to determine the overall shape. Possible classifications of volumetric shape are shell, cylindrical object, elongated box, spherical, and unrecognized (possibly multiple objects).
  • the centroid and covariance are calculated and shown as ellipses, along with the centroid and covariance of the composite in step 19.
  • the following specific processing routines can be used to implement the 19 operations shown in FIG. 5 .
  • the disclosed and other embodiments and the functional operations described in this specification can be implemented in digital electronic circuitry, or in computer software, firmware, or hardware, including the structures disclosed in this specification and their structural equivalents, or in combinations of one or more of them.
  • the disclosed and other embodiments can be implemented as one or more computer program products, i.e., one or more modules of computer program instructions encoded on a computer readable medium for execution by, or to control the operation of, data processing apparatus.
  • the computer readable medium can be a machine-readable storage device, a machine-readable storage substrate, a memory device, a composition of matter effecting a machine-readable propagated signal, or a combination of one or more them.
  • data processing apparatus encompasses all apparatus, devices, and machines for processing data, including by way of example a programmable processor, a computer, or multiple processors or computers.
  • the apparatus can include, in addition to hardware, code that creates an execution environment for the computer program in question, e.g., code that constitutes processor firmware, a protocol stack, a database management system, an operating system, or a combination of one or more of them.
  • a propagated signal is an artificially generated signal, e.g., a machine-generated electrical, optical, or electromagnetic signal, that is generated to encode information for transmission to suitable receiver apparatus.
  • a computer program (also known as a program, software, software application, script, or code) can be written in any form of programming language, including compiled or interpreted languages, and it can be deployed in any form, including as a stand-alone program or as a module, component, subroutine, or other unit suitable for use in a computing environment.
  • a computer program does not necessarily correspond to a file in a file system.
  • a program can be stored in a portion of a file that holds other programs or data (e.g., one or more scripts stored in a markup language document), in a single file dedicated to the program in question, or in multiple coordinated files (e.g., files that store one or more modules, sub-programs, or portions of code).
  • a computer program can be deployed to be executed on one computer or on multiple computers that are located at one site or distributed across multiple sites and interconnected by a communication network.
  • the processes and logic flows described in this specification can be performed by one or more programmable processors executing one or more computer programs to perform functions by operating on input data and generating output.
  • the processes and logic flows can also be performed by, and apparatus can also be implemented as, special purpose logic circuitry, e.g., an FPGA (field programmable gate array) or an ASIC (application-specific integrated circuit).
  • processors suitable for the execution of a computer program include, by way of example, both general and special purpose microprocessors, and any one or more processors of any kind of digital computer.
  • a processor will receive instructions and data from a read-only memory or a random access memory or both.
  • the essential elements of a computer are a processor for performing instructions and one or more memory devices for storing instructions and data.
  • a computer will also include, or be operatively coupled to receive data from or transfer data to, or both, one or more mass storage devices for storing data, e.g., magnetic, magneto-optical disks, or optical disks.
  • mass storage devices for storing data, e.g., magnetic, magneto-optical disks, or optical disks.
  • a computer need not have such devices.
  • Computer readable media suitable for storing computer program instructions and data include all forms of non-volatile memory, media and memory devices, including by way of example semiconductor memory devices, e.g., EPROM, EEPROM, and flash memory devices; magnetic disks, e.g., internal hard disks or removable disks; magneto-optical disks; and CD-ROM and DVD-ROM disks.
  • semiconductor memory devices e.g., EPROM, EEPROM, and flash memory devices
  • magnetic disks e.g., internal hard disks or removable disks
  • magneto-optical disks e.g., CD-ROM and DVD-ROM disks.
  • the processor and the memory can be supplemented by, or incorporated in, special purpose logic circuitry.
  • the disclosed embodiments can be implemented in a computing system that includes a back-end component, e.g., as a data server, or that includes a middleware component, e.g., an application server, or that includes a front-end component, e.g., a client computer having a graphical user interface or a Web browser through which a user can interact with an implementation of what is disclosed here, or any combination of one or more such back-end, middleware, or front-end components.
  • the components of the system can be interconnected by any form or medium of digital data communication, e.g., a communication network. Examples of communication networks include a local area network (“LAN”) and a wide area network (“WAN”), e.g., the Internet.
  • LAN local area network
  • WAN wide area network
  • a computer system for implementing the disclosed embodiments can include client computers (clients) and server computers (servers).
  • clients client computers
  • server computers server computers
  • a client and a server are generally remote from each other and typically interact through a communication network.
  • the relationship of client and server can arise by virtue of computer programs running on the respective computers and having a client-server relationship to each other.

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Abstract

Techniques, apparatus and systems for muon tomography vehicle imaging use autonomous processing of 3-dimensional muon tomography vehicle images based on Data Modeling techniques and various applications including analyzing vehicle voxel data such as muon vehicle images to detect potential threat objects and then to further discriminate the identified potential threat objects by shape.

Description

    CROSS REFERENCE TO RELATED APPLICATIONS
  • This patent application is a continuation of U.S. patent application Ser. No. 12/099,072, filed Apr. 7, 2008, which claims benefit of U.S. Provisional Patent Application No. 60/922,199, filed Apr. 5, 2007. The entire contents of the before-mentioned patent applications are incorporated by reference as part of the disclosure of this application.
  • BACKGROUND
  • This application relates to techniques, apparatus and systems for vehicle muon tomography imaging.
  • Muon tomography is an imaging technique that produces an image of an object such as a vehicle or its contents based on detection of the scattering of cosmic ray produced muons as they pass through the object. Muons scattered by an object can be detected and the detected signals can be processed to provide specific density and three-dimensional imaging of materials.
  • The collision of natural cosmic rays with atoms in the earth's upper atmosphere creates unstable particles, such as pions and kaons, which decay to muons. Muons penetrate through the atmosphere and into the ground at the rate of approximately 1 per square centimeter per minute. Muons can be thought of as much larger cousins of the electrons that are an essential part of ordinary matter. Energetic muons interact strongly enough with matter by ionization to be easily detected, and can penetrate large thicknesses without significant impairment.
  • Physicists at the Los Alamos National Laboratory (LANL) have developed techniques for detecting scattering of cosmic ray produced muons to produce tomographic images of an object exposed to the cosmic ray muons. See, e.g., Priedhorsky et al., “Detection of high-Z objects using multiple scattering of cosmic ray muons”, Proceedings of SPIE Press, Vol. 5199A-39 (August, 2003). As a muon moves through material, Coulomb scattering of the charges of subatomic particles perturb its trajectory. The total deflection depends on several material properties, but the dominant parameters are the atomic number, Z, of the nuclei and the material density. The LANL techniques are based on precise reconstruction of individual muon tracks and are capable of detecting and visually representing potential threat objects in vehicles or transportable containers in order to alert responsible authorities, thereby allowing them to preemptively interdict the movement of such material to prevent any damage and destruction. A vehicle muon tomography system can be constructed based on the LANL techniques to provide hazard detection at various locations including ports and checkpoints. For example, such systems can provide the Department of Homeland Security (DHS) with an effective solution to the critical need for timely vehicle and cargo inspection nationwide.
  • Various aspects of muon tomography imaging techniques are described in literature. See, e.g., Jenneson, “Large vessel imaging using cosmic-ray muons”, Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, Volume 525, Issues 1-2, Pages 346-351, Proceedings of the International Conference on Imaging Techniques in Subatomic Physics, Astrophysics, Medicine, Biology and Industry (June, 2004); and “Muon imager searches for smuggled nuclear material”, OE magazine, SPIE (September, 2003).
  • SUMMARY
  • This specification describes techniques, apparatus and systems for vehicle muon tomography imaging using autonomous processing of 3-dimensional (3D) muon tomography vehicle images based on Data Modeling techniques and various applications including analyzing vehicle voxel data such as muon vehicle images to detect potential threat objects within a vehicle or transportable container and then to further discriminate the identified potential threat objects by shape.
  • In one aspect, a computer-automated method for processing muon vehicle imaging data of a vehicle inspection region within a vehicle muon tomography imaging system is described. This method includes processing muon vehicle imaging data obtained from the vehicle inspection region to obtain a histogram of the muon vehicle imaging data at different positions in the vehicle inspection region; separating the muon vehicle imaging data into bins based on the histogram; removing a subset of the muon vehicle imaging data in a mode bin that has higher frequencies of occurrence than remaining muon vehicle imaging data from the muon vehicle imaging data to retain the remaining muon vehicle imaging data for further processing; determining an optimal number of bins for separating the remaining muon vehicle imaging data into data bins; processing the remaining muon vehicle imaging data to obtain a histogram of the remaining muon vehicle imaging data at different positions in the vehicle inspection region; separating the remaining muon vehicle imaging data into data bins at the optimal number of bins; and removing data in a mode bin that has higher frequencies of occurrence than the rest of the remaining muon vehicle imaging data to retain remaining muon vehicle imaging data as target detection data for further processing. This method also includes using a background recognizer Data Model for identifying background vehicle structure from the target detection data; applying the background recognizer Data Model to process the remaining muon vehicle imaging data to produce an image of the vehicle inspection region by removing background structure; using a target identification Data Model for identifying a target object from the target detection data; applying the target identification Data Model to process data of the image produced after applying the background recognizer Data Model to produce an image of the target object; and processing the image of the target object to determine a location and a shape of the target object in the vehicle inspection region.
  • In another aspect, a computer system for processing muon vehicle imaging data of a vehicle inspection region within a muon tomography vehicle imaging system is described. This system includes means for processing muon vehicle imaging data obtained from the vehicle inspection region to obtain a histogram of the muon vehicle imaging data at different positions in the vehicle inspection region; means for separating the muon vehicle imaging data into bins based on the histogram; means for removing a subset of the muon vehicle imaging data in a mode bin that has higher frequencies of occurrence than remaining muon vehicle imaging data from the muon vehicle imaging data to retain the remaining muon vehicle imaging data for further processing; means for determining an optimal number of bins for separating the remaining muon vehicle imaging data into data bins; means for processing the remaining muon vehicle imaging data to obtain a histogram of the remaining muon vehicle imaging data at different positions in the vehicle inspection region; means for separating the remaining muon vehicle imaging data into data bins at the optimal number of bins; and means for removing data in a mode bin that has higher frequencies of occurrence than the rest of the remaining muon vehicle imaging data to retain remaining muon vehicle imaging data as target detection data for further processing. This system also includes means for using a background recognizer Data Model for identifying background structure from the target detection data; means for applying the background recognizer Data Model to process the target detection data to produce an image of the vehicle inspection region by removing identified background structure; means for using a target identification Data Model for identifying a target object from the target detection data; means for applying the target identification Data Model to process data of the image produced after applying the background recognizer Data Model to produce an image of the target object; and means for processing the image of the target object to determine a location and a shape of the target object in the vehicle inspection region.
  • In another aspect, a muon tomography vehicle imaging system is described to include a first set of muon detectors located on a first side of a vehicle inspection region holding a vehicle for inspection, the muon detectors measuring incident muons; a second set of muon detectors located on a second side of the vehicle inspection region opposite to the first side to measure outgoing muons exiting the vehicle inspection region; and a muon tomography control module that receives detector outputs from the first and the second set of muon detectors and processes the detector outputs to produce a 3-dimensional image of the vehicle inspection region. The muon tomography control module includes a suspect object detection module for processing muon vehicle imaging data of the 3-dimensional image. The suspect object detection module includes means for applying Data Models to process the muon vehicle imaging data to isolate one or more target objects from other objects in the vehicle inspection region; means for applying primitive shape recognition to cross-section slices of an image of a volume containing data points of the one or more target objects to identify predetermined primitive shapes; and means for processing identified primitive shapes to construct a 3-dimensional image of each target object.
  • In another aspect, a computer-automated method for processing muon vehicle imaging data from a muon tomography vehicle imaging system is described to include applying Data Models to process muon tomography vehicle image data to isolate one or more target objects from other objects in a volume under inspection by the muon tomography vehicle imaging system; applying primitive shape recognition to cross-section slices of an image of the volume containing data points of the one or more target objects to identify predetermined primitive shapes; and processing identified primitive shapes to construct a 3-dimensional image of each target object.
  • In yet another aspect, a computer-implemented method for using natural cosmic muons as a radiation source to obtain muon tomographic images of a vehicle under inspection is described to include obtaining a cosmic muon tomography vehicle image of a vehicle under inspection; processing vehicle voxel data of each obtained muon vehicle image to compute histogram of the vehicle voxel data of the obtained muon vehicle image; applying statistical processing based on the histogram to the vehicle voxel data to generate a Data Model to monitor one or more changes in the obtained muon vehicle image indicative of presence of a target object in the obtained muon vehicle image; and determining a shape of the target object.
  • Particular embodiments described in this specification can be implemented to realize one or more of advantages. For example, a threat object can be identified by autonomous processing without human intervention. Suitable Data Modeling based on statistical process can provide efficient and robust data processing and provide autonomous identification of the shape of a threat object. As another example, the present Data Modeling allows for relatively short muon vehicle imaging exposure times in capturing the muon vehicle imaging data without compromising the data processing accuracy and thus allows for high-speed detection.
  • The details of one or more embodiments of the invention are set forth in the accompanying drawings and the description below. Other features, aspects, and advantages of the invention will become apparent from the description, the drawings, and the claims.
  • BRIEF DESCRIPTION OF THE DRAWINGS
  • FIG. 1 illustrates an example of a muon tomography vehicle imaging system for inspecting a vehicle for other objects.
  • FIGS. 2A, 2B and 2C show examples of muon tomography vehicle images obtained from a LANL-built system with imaging exposure times of 15 seconds, 30 seconds and 60 seconds, respectively.
  • FIG. 3 shows an example of a muon tomography vehicle imaging system implementing autonomous processing of 3D muon tomography vehicle images based on Data Modeling.
  • FIG. 4 shows an example of operation steps performed by the suspect object detection module in FIG. 3.
  • FIG. 5 shows an exemplary process that implements the processing in FIG. 4, where the Cartesian coordinates X, Y and Z are defined in FIG. 1.
  • FIG. 6 shows examples of front view and top view projections of values for the characteristic data.
  • FIGS. 7A, 7B, 7C and 7D show an example for data processing based on the Vehicle Assembly Recognizer Target Identification in FIG. 5.
  • FIGS. 8A, 8B and 8C show Hamming distance curves for a square, circle, and rectangle primitive shapes in the processing in FIG. 5.
  • FIG. 9 shows an example for data processing to indicate the corresponding primitive shapes for the process in FIG. 5.
  • Like reference numbers and designations in the various drawings indicate like elements.
  • DETAILED DESCRIPTION
  • Muons contribute roughly a tenth of the natural dose of daily ionizing radiation at the earth's surface and such radiation exposure is a natural and unavoidable feature of our environment. Muon tomography takes advantage of this universal presence and the penetrating characteristics of the muons to reveal the position and size of various materials without causing any harm to personnel or requiring additional intervention by inspectors to correctly identify potential threats. Moreover, efforts to conceal weapons or other dangerous materials by encasing them in a massive lead container would be just as revealing, since the muon deflection patterns would indicate the presence of shielding material where it didn't belong.
  • FIG. 1 illustrates an example of a muon tomography vehicle imaging system for inspecting a vehicle for other objects. This system for detecting muons includes a vehicle inspection region or volume 130 for placing a vehicle to be inspected. On the top and bottom sides of this vehicle inspection region 130, muon detectors 111, 112, 121 and 122 are provided to detect the incident muons from the atmosphere at the top of the region 130 and outgoing muons at the bottom of the region 130. Such muon detectors can be drift tubes that are filled with a gas which can be ionized by muons and are configured to collect and correlate the amount of deflection of each muon that passes through and the vehicle or container being inspected. Multiple drift tubes can be used to form detector arrays to accurately determine a muon's path and, by analyzing the amount of deflection and the pattern of the scattering which results, a visual three-dimensional image of the variety of materials can be generated.
  • More specifically, the muon detectors 111, 112, 121 and 122 include a first set of position- sensitive muon detectors 111 and 112 located on the top side of the vehicle inspection region 130 to measure positions and angles of incident muons, a second set of position sensitive muon detectors 121 and 122 located on the bottom side of the vehicle inspection region 130 opposite to the top side to measure positions and angles of outgoing muons exiting the vehicle inspection region. A muon tomography signal processing unit, which may include, e.g., a microprocessor, is provided to receive data of measured signals of the incoming muons from the first set of position sensitive muon detectors 111 and 112 and measured signals of the outgoing muons from the second set of position sensitive muon detectors 121 and 122.
  • The muon trajectories are more strongly affected by special nuclear material (SNM) and materials that make good gamma ray shielding (such as lead and tungsten) than by the materials that make up more ordinary objects (such as water, plastic, aluminum, and steel). Each muon carries information about the objects that it has penetrated, and by measuring the scattering of multiple muons, one can probe the properties of these objects. In particular, one can detect high-Z objects amongst more typical low-Z and medium-Z matter. The example in FIG. 1 shows a truck that carries a cargo 133 and a shielded crate 134 that conceals a high Z object. The incident cosmic muons 101 are scattered by the truck and everything in the truck. The degrees of scattering of the muons vary with the object or objects in the paths of the muons. For example, the muon rays 141 shown in FIG. 1 represent low scattering muon paths in which truck components or objects have low Z numbers. The truck's engine 131 tends to have higher Z than other vehicle components and thus causes mild scattering of muons as represented by the muon rays 142. The cargo 133 carried by the truck may also cause mild scattering of muons. The high Z object in the shielded crate 134 cause large scattering 143 of the muons.
  • The muon tomography signal processing unit for the system in FIG. 1 is configured to analyze scattering behaviors of muons, caused by scattering of the muons in the materials within the vehicle inspection region 130, based on the measured incoming and outgoing positions and angles of muons, to obtain a tomographic profile or the spatial distribution of scattering centers within the vehicle inspection region 130. The obtained tomographic profile or the spatial distribution of scattering centers can be used to reveal the presence or absence of one or more objects in the vehicle inspection region such as materials with high atomic numbers Z including nuclear materials or devices.
  • Notably, the image of a high Z object, such as the example enclosed in the shielded crate 134 in FIG. 1, is part of the generated muon tomography vehicle image and is mixed with images of other objects in the generated muon tomography vehicle image. One technical challenge is to fully autonomously process the muon tomography vehicle images based on computer data processing to identify a threat object in a generated muon tomography vehicle image.
  • It is generally believed that longer muon vehicle imaging exposure times can improve the image quality and detection accuracy in identifying a threat object in the obtained muon tomography vehicle images. However, contrary to this general belief, longer exposure times are not necessarily better for automatic target detection, because more false positives occur. FIGS. 2A, 2B and 2C show examples of muon tomography vehicle images obtained from the LANL Large Muon Tracker system with imaging exposure times of 15 seconds, 30 seconds and 60 seconds, respectively. FIG. 2A illustrates how in as little as 15 seconds various materials and components, e.g., the engine block, transmission drive train and wheels, can be distinguished—they have been color-coded to provide a visual identification. The appearance of the small item shown in red above the rear axle and marked in a dashed line circle indicates a suspect high-Z object which can be a potential nuclear mass. However, in the image obtained with a longer exposure time of 30 seconds in FIG. 2B, the image of the suspect high-Z object is not readily visible. Therefore, muon tomography using appropriate drift tubes and advanced algorithms such as entropy based methods enables the timely inspection of all cargo entering the U.S., the monitoring of trucks and other vehicles passing through critical infrastructure points, and the detection of specific explosive components used in terrorist weapons around the world.
  • Techniques, apparatus and systems for muon tomography vehicle imaging can use autonomous processing of 3D muon tomography vehicle images based on discrete and analytical Data Modeling techniques comprising Entropyology or random-field-information science. These Data Modeling techniques were previously developed by Holger M. Jaenisch. These techniques may be used to analyze voxel data such as muon vehicle images to detect potential threat objects and then to further discriminate the identified potential threat objects by shape. Data Modeling uses the smallest amount of entropic information to functionally model empirical dynamics and can take the form of a group of real numbers, a single equation, or a network of equations. A Data Model can also be a variable of another function. A hierarchy of functional models (equations whose variables are themselves equations) can be built up to combine any group or subset of previously derived models. Data Modeling finds a mathematical expression that provides a good model between given finite sample values of the independent variables and the associated values of the dependent variables of the process. The predictive mathematical expression modeling the given sample of data is called a Data Model. This process involves finding both the structural form of the Data Model and the numeric coefficients for the Data Model.
  • The present techniques use Data Modeling methods and can be implemented in ways that minimize long exposure requirements previously reported in the literature and allow for muon vehicle imaging in the gray medium exposure length zone, which is traditionally difficult to automate. Therefore, high-speed and efficient autonomous threat detection can be achieved.
  • FIG. 3 shows an example of a muon tomography vehicle imaging system 300 implementing autonomous processing of 3D muon tomography vehicle images based on Data Modeling. The detector design in this system 300 is based on the design in FIG. 1 and may also be implemented by other muon detector configurations. Input detector readout circuit 310 is connected to the detectors 111 and 112 to receive and pre-process the detector outputs and feeds the pre-processed detector outputs to a muon tomography processing module 330. Output detector readout circuit 320 is connected to the detectors 121 and 122 to receive and pre-process the detector outputs and also feeds the pre-processed detector outputs to the muon tomography processing module 330.
  • The muon tomography processing module 330 can include one or more computers or computer processors and has a muon tomography vehicle imaging processing module 331 and a suspect object detection module 332. The muon tomography vehicle imaging processing module 331 is configured to process the detector outputs from the detectors 111, 112, 121 and 122 to generate 3D muon tomography vehicle images of the vehicle inspection region 130. Examples of such images are shown in FIGS. 2A, 2B and 2C. The suspect object detection module 332 receives the voxel data of the 3D muon tomography vehicle images output by the muon tomography vehicle imaging processing module 331 and is programmed to autonomously process 3D muon tomography vehicle images based on Data Modeling. The following sections describe details of operations of the suspect object detection module 332.
  • The suspect object detection module 332 is configured to include various processing modules and routes to provide a computer-automated method for processing muon vehicle imaging data based on Data Modeling. FIG. 4 shows an example of operation steps performed by the suspect object detection module 332. As illustrated, the suspect object detection module 332 applies Data Models to process muon tomography vehicle image data from the muon tomography vehicle imaging processing module 331 to isolate one or more target objects from other objects in the vehicle inspection region 130 (step 410) and subsequently applies primitive shape recognition to cross-section slices of an image of the volume 130 containing data points of the one or more target objects to identify predetermined primitive shapes (step 420). Next, the suspect object detection module 332 processes the identified primitive shapes to construct a 3-dimensional image of each target object.
  • The processing in step 410 can include several processing steps. First, the muon vehicle imaging data obtained from the volume 130 is processed to obtain a histogram of the muon vehicle imaging data at different positions in the volume 130 and the muon vehicle imaging data is separated into bins based on the histogram. Second, a subset of the muon vehicle imaging data in a mode bin that has higher frequencies of occurrence than remaining muon vehicle imaging data is removed from the muon vehicle imaging data to retain the remaining muon vehicle imaging data for further processing. Third, a background recognizer Data Model for identifying vehicle structures is applied to process the remaining muon vehicle imaging data to produce an image of the volume by removing the identified background structure. Subsequently, a target identification Data Model for identifying the one or more target objects is applied to process data of the image produced after applying the background recognizer Data Model to produce an image of the one or more target objects. The above processing can be performed based on the vehicle voxel data from the muon tomography vehicle imaging processing module 331 and can be achieved without relying on prior samples or data on some pre-selected known threat objects.
  • FIG. 5 shows an exemplary process that implements the processing in FIG. 4. The Cartesian coordinates X, Y and Z are defined in FIG. 1. The numerals in FIG. 5 correspond the following processing steps performed by the suspect object detection module 332:
  • 1. Receive vehicle voxel data from the muon tomography processing module 330.
  • 2. Compute the histogram of the received vehicle voxel data and separate the histogram data into three bins. Delete data in the Mode bin which is the bin that has most frequently occurring data points or has the largest number of points. After deletion of the Mode bin, the remaining muon vehicle imaging data is used in two processing paths: (1) determination of the optimal number of bins to separate the remaining muon vehicle imaging data carried in subsequent processing steps 3-6, and (2) further processing the remaining muon vehicle imaging data to detect threat objects in subsequent processing steps 7-19.
  • 3. Project the remaining data onto XZ plane. One of various techniques for this process is described in Jaenisch, H., Handley, J., “Data Modeling for Defense Planning”, Society for Computer Simulation (Huntsville Simulation Conference 2003), Huntsville, Ala. (October, 2003).
  • 4. Project remaining voxel rays onto the X axis.
  • 5. Calculate moments and cumulants.
  • 6. Determine optimal number of bins using predictive equation Data Model based on the calculated moments and cumulants. Examples of processing techniques for performing this step are described in Jaenisch, H. M. and Handley, J. W., “Data Modeling for Radar Applications”, Proceedings of IEEE Radar Conference 2003; Jaenisch, H., “Enabling Unattended Data Logging and Publication by Data Model Change Detection and Environmental Awareness”, SPIE Defense and Security Symposium, Orlando, Fla., April 2006; Jaenisch, H., Handley, J., Jaenisch, K., Hicklen, M., “Enabling Human HUMS with Data Modeling”, SPIE Defense and Security Symposium, Orlando, Fla., April 2006; Pooley, J., Murray, S., Jaenisch, H., Handley, J., “Fault Detection via Complex Hybrid Signature Analysis”, JANNAF 39th Combustion, 27th Airbreathing Propulsion, 21st Propulsion Systems Hazards, and 3rd Modeling and Simulation Subcommittees Joint Meeting, Colorado Springs, Colo., (Dec. 1-5, 2003); and Jaenisch, H., Handley, J., Hicklen, M., Vineyard, D., Ramage, M., Colthart, J., “Muon vehicle imaging and Data Modeling”, Proceedings of SPIE, Defense and Security Symposium, Orlando, Fla., April 2007, Vol. 6538, No. 85.
  • 7. Compute the histogram of the remaining data produced by the step 2 and separate the remaining data into the optimal number of bins. Once again, delete the data in the Mode bin and retain the remaining data as the target detection data for further processing.
  • 8. Apply Vehicle Assembly Recognizer Decision equation Data Model to the remaining data produced in the step 7 to identify Z values associated with vehicle components.
  • 9. Remove vehicle components.
  • 10. Apply Target Medium Z Identification Decision equation Data Model to the data after removal of data associated with identified vehicle components.
  • 11. Extract a candidate target and determine if the target exists and location of the target.
  • 12. Extract cross-section slices.
  • 13. Apply a shape characterizer Data Model to each extracted cross-section slice.
  • 14. Calculate moments and cumulants of each cross-section slice.
  • 15-17. Apply 2D primitive shape recognizer Data Models, such as a square shape recognizer Data Model, a rectangle shape recognizer Data Model, and a circle shape recognizer Data Model.
  • 18. Perform 3D primitive shape recognition (Volumetric) using Volumetric Shape Recognizer Data Model.
  • 19. Calculate centroids and covariances. Examples of processing techniques for performing this step are described in Jaenisch et al., “A Simple Algorithm For Sensor Fusion Using Spatial Voting (Unsupervised Object Grouping)”, Proceedings of SPIE, Defense and Security Symposium 2008, Orlando, Fla., March 2008, Vol. 6968, No. 68.
  • Once data is loaded in step 1, bulk filtering of the vehicle shell is performed by calculating a histogram using 3 bins in step 2. The mode bin (one most frequently occurring, or the one with the largest number of points) is removed in step 2, and the remainder of the (x,y,z) locations projected onto the XZ plane in step 3. The values in the XZ plane are then projected onto the X-axis of the resulting data sequence graph in step 4, which is characterized by statistics in step 5 and used with a predictive bin estimating equation to determine optimal number of bins in step 6. FIG. 6 shows examples of front view and top view projections of values for the training data.
  • After the optimal number of bins is determined at step 6, a histogram for the remaining data produced by the step 2 is calculated using the optimal number of bins and the data in the new Mode bin is once again deleted (step 7). The remaining points are processed through the Vehicle Assembly Recognizer Decision equation (using x, y, and z locations along with value) in step 8, and the vehicle components identified are removed in step 9. The remaining points are processed through the Target Identification Decision equation (also using x, y, and z location along with value at each point) in 10. Steps 8 and 10 isolate the candidate target which is extracted in step 11.
  • FIGS. 7A, 7B, 7C and 7D show an example for the above processing based on the Vehicle Assembly Recognizer Decision equation Target Identification Decision equation. FIG. 7A shows the projection of van data onto the XZ plane. FIG. 7B shows the XZ projection of data remaining after histogram. FIG. 7C shows the data after using Vehicle Assembly and Target Identification Data Models, respectively. The points remaining in FIG. 7C are for the potential target. FIG. 7D shows a graph of covariance ellipses for each cross-section neighborhood extracted and processed.
  • The above described vehicle assembly recognizer Data Model is a specific example of a background recognizer Data Model that identifies and recognizes background structure in the muon tomography data images.
  • Beginning next in step 12, 2-D primitive shape detection and 3-D overall shape detection are performed. This process begins by extracting all planes, i.e., XY, XZ, and YZ slices that contain one or more of the points. These planes or slices are processed without replacement to extract all 32×32 pixel neighborhoods that contain at least one point. The shape of each neighborhood is characterized by applying the Shape Characterizer in step 13. The resulting sequence is then characterized using descriptive moments and cumulants in step 14 for input into the Shape Recognizers in steps 15, 16, and 17. In this regard, the number of pixel values in the neighborhood that change between iterations is calculated and stored as a data sequence known as the Hamming distance curves as shown in FIGS. 8A, 8B and 8C for the Square, Circle, and Rectangle Shapes. The Hamming sequence is then characterized using statistics. The statistics drive each of the Square, Circle, and Rectangle Shape Recognizers, respectively.
  • Upon completion of processing all of the neighborhoods, the ratio of neighborhoods flagged as square, circle, or rectangle to the total number of extracted neighborhoods is determined. FIG. 9 shows an example for this data processing to indicate the corresponding primitive shapes. If a neighborhood does not flag as any of the 3 primitive shapes, it is labeled as unrecognized. Subsequently, the Volumetric Shape Recognizer in step 18 uses the ratio of squares, circles, and rectangles flagged to total number of neighborhoods as input to determine the overall shape. Possible classifications of volumetric shape are shell, cylindrical object, elongated box, spherical, and unrecognized (possibly multiple objects). For each neighborhood extracted initially, the centroid and covariance are calculated and shown as ellipses, along with the centroid and covariance of the composite in step 19.
  • In one exemplary implementation of the process in FIG. 5, the following specific processing routines can be used to implement the 19 operations shown in FIG. 5.
  • 1. Start with Vehicle voxel data
  • write(6,*)‘Input File Name => ’
    read(5,*)pt1
    open(1,file=pt1,status=‘unknown’)
    read(1,*)ix,iy,iz
    allocate (YY1(0:ix*iy*iz−1,0:3))
    write(6,*)‘Axis lengths ’,ix,iy,iz
    m=0
    do k=0,iz−1
    do j=0,iy−1
    do i=0,ix−1
    YY1(m,0)=i
    YY1(m,1)=j
    YY1(m,2)=k
    read(1,*)YY1(m,3)
    m=m+1
    enddo
    enddo
    enddo
    close(1)
  • 2. Histogram data into 3 bins, delete Mode
  • call calchist(YY1,m,3,zzz,n)
    subroutine calchist(Y,m,nbin,E,p)
    implicit none
    integer nbin,m,i,j,maxbin,maxbval,n,p
    real minD, maxD, rngD, minbinD
    real maxbinD, meanA, stdevA
    real histt(0:nbin−1)
    real D(0:m−1),E(0:m−1,0:3)
    real Y(0:m−1,0:3),A(0:m−1)
    minD=Y(0,3)
    maxD=Y(0,3)
    do i=0, m−1
    D(i)=Y(i,3)
    if(D(i).gt.maxD)maxD=D(i)
    if(D(i).lt.minD)minD=D(i)
    enddo
    rngD=maxD−minD
    do i=0,nbin−1
    histt(i)=0
    enddo
    do i=0,m−1
    do j=0,nbin−1
    if(D(i).ge.(minD+j*rngD/nbin) .and. D(i).lt.
    + (minD+(j+1)*rngD/nbin))histt(j)=histt(j)+1
    enddo
    enddo
    maxbin=0
    maxbval=histt(0)
    do j=1,nbin−1
    if(histt(j).ge.maxbval) then
    maxbin=j
    maxbval=histt(j)
    endif
    enddo
    minbinD=minD+maxbin*rngD/nbin
    maxbinD=minD+(maxbin+1)*rngD/nbin
    A(0)=0
    n=0
    p=0
    do i=0,m−1
    if(D(i).ge.minbinD .and. D(i).le.maxbinD) then
    A(n)=D(i)
    n=n+1
    else
    do j=0,3
    E(p,j)=Y(i,j)
    enddo
    p=p+1
    endif
    enddo
    call mean(A,n,meanA)
    call stdev(A,n,stdevA)
    do i=0,p−1
    E(i,3)=(E(i,3)−meanA)/stdevA
    enddo
    return
    end
  • 3. Project remaining data onto XZ plane
  • subroutine extractplanes(X,Y,Z,A,ix,iy,iz,B,n1,n2,n3,n)
    implicit none
    integer ix,iy,iz,n1,n2,n3,i,j,k,n
    integer X(0:n−1),Y(0:n−1),Z(0:n−1),A(0:ix−1,0:iy−1,0:iz−1)
    integer B(0:n1+n2+n3−1, 0:ix−1, 0:ix−1)
    write(6,*)n1,n2,n3
    do i=0,n1−1
    do j=0,iy−1
    do k=0,iz−1
    B(i,j,k)=A(X(i),j,k)
    enddo
    enddo
    enddo
    do i=0,n2−1
    do j=0,ix−1
    do k=0,iz−1
    B(n1+i,j,k)=A(j,Y(i),k)
    enddo
    enddo
    enddo
    do i=0,n3−1
    do j=0,ix−1
    do k=0,iy−1
    B(n1+n2+i,j,k)=A(j,k,Z(i))
    enddo
    enddo
    enddo
    return
    end
  • 4. Project remaining voxel rays onto X axis (included in code for step 3)
  • 5. Calculate Moments and Cumulants.
  • subroutine mean(A,n,meanA)
    implicit none
    integer n,i
    real A(0:n−1)
    real meanA
    meanA=0.0
    do i=0,n−1
    meanA=meanA+A(i)/n
    enddo
    return
    end
    subroutine stdev(A,n,stdevA)
    implicit none
    integer n,i
    real A(0:n−1)
    real stdevA,meanA,s,pp
    stdevA=0.0
    meanA=0.0
    do i=0,n−1
    meanA=meanA+A(i)/n
    enddo
    do i=0,n−1
    s=A(i)−meanA
    pp=s*s
    stdevA=stdevA+pp
    enddo
    stdevA=sqrt(stdevA/(n−1))
    return
    end
    subroutine skewness(A,n,ystat)
    implicit none
    integer n
    real A(0:n−1)
    integer i
    real ystat,ymean,ystdev
    call mean(A,n,ymean)
    call stdev(A,n,ystdev)
    ystat=0
    do i=0,n−1
    ystat=ystat+(1/n)*((A(i)−ymean)/ystdev)**3
    enddo
    return
    end
    subroutine kurtosis(A,n,ystat)
    implicit none
    integer n
    real A(0:n−1)
    integer i
    real ystat,ymean,ystdev
    call mean(A,n,ymean)
    call stdev(A,n,ystdev)
    ystat=0
    do i=0,n−1
    ystat=ystat+(1/n)*((A(i)−ymean)/ystdev)**4
    enddo
    ystat=ystat−3
    return
    end
  • 6. Determine optimal number of bins using predictive equation Data Model
  • cls
    on error resume next
    input “stdev => ”, stdev
    avg0=0
    dev0=1
    stdev = (stdev − avg0) / dev0
    input “skew => ”, skew
    avg1=0
    dev1=1
    skew = (skew − avg1) / dev1
    input “kurt => ”, kurt
    avg2=0
    dev2=1
    kurt = (kurt − avg2) / dev2
    t1 = 3996.8959
    t1=t1 + −2034.3165*stdev
    t1=t1 + −7531.7086*skew
    t1=t1 + 1462.2043*kurt
    t1=t1 + 406.1663*stdev*stdev
    t1=t1 + 4485.9879*skew*skew
    t1=t1 + 144.8136*kurt*kurt
    t1=t1 + 2368.6092*stdev*skew
    t1=t1 + −433.4313*stdev*kurt
    t1=t1 + −1658.6568*skew*kurt
    t1=t1 + 210.6329*stdev*skew*kurt
    t1=t1 + −17.9517*stdev*stdev*stdev
    t1=t1 + −883.0253*skew*skew*skew
    t1=t1 + 4.7155*kurt*kurt*kurt
    t1=t1 + −261.7948*skew*stdev*stdev
    t1=t1 + −612.5371*stdev*skew*skew
    t1=t1 + −16.8366*stdev*kurt*kurt
    t1=t1 + 46.8615*kurt*stdev*stdev
    t1=t1 + 477.7376*kurt*skew*skew
    t1=t1 + −83.0172*skew*kurt*kurt
    t2 = −962.0357
    t2=t2 + 934.7015*stdev
    t2=t2 + 602.9623*skew
    t2=t2 + −333.8504*stdev*stdev
    t2=t2 + −133.4822*skew*skew
    t2=t2 + −349.8407*stdev*skew
    t2=t2 + 44.3898*stdev*stdev*stdev
    t2=t2 + 9.9078*skew*skew*skew
    t2=t2 + 52.4919*skew*stdev*stdev
    t2=t2 + 38.1055*stdev*skew*skew
    t3 = −251.5042
    t3=t3 + 402.1001*stdev
    t3=t3 + 33.9866*kurt
    t3=t3 + −212.6009*stdev*stdev
    t3=t3 + −1.804*kurt*kurt
    t3=t3 + −31.4003*stdev*kurt
    t3=t3 + 37.3747*stdev*stdev*stdev
    t3=t3 + 0.031*kurt*kurt*kurt
    t3=t3 + 7.362*kurt*stdev*stdev
    t3=t3 + 0.8384*stdev*kurt*kurt
    t4 = −150.1537
    t4=t4 + −31.6181*t1
    t4=t4 + 287.8003*stdev
    t4=t4 + 57.6673*t2
    t4=t4 + −0.773*t1*t1
    t4=t4 + −190.0648*stdev*stdev
    t4=t4 + −11.2456*t2*t2
    t4=t4 + −0.1633*t1*stdev
    t4=t4 + 9.6926*t1*t2
    t4=t4 + −21.4703*stdev*t2
    t4=t4 + 2.656*t1*stdev*t2
    t4=t4 + −0.077*t1*t1*t1
    t4=t4 + 41.7226*stdev*stdev*stdev
    t4=t4 + 0.9628*t2*t2*t2
    t4=t4 + −1.5302*stdev*t1*t1
    t4=t4 + 2.237*t1*stdev*stdev
    t4=t4 + −1.4072*t1*t2*t2
    t4=t4 + 0.5811*t2*t1*t1
    t4=t4 + 2.7992*t2*stdev*stdev
    t4=t4 + −0.1588*stdev*t2*t2
    t5 = −22.5943
    t5=t5 + −18.4502*t1
    t5=t5 + 35.9303*t2
    t5=t5 + −6.8155*t3
    t5=t5 + −2.2486*t1*t1
    t5=t5 + 51.4807*t2*t2
    t5=t5 + 24.0612*t3*t3
    t5=t5 + −29.7499*t1*t2
    t5=t5 + 39.3189*t1*t3
    t5=t5 + −84.1592*t2*t3
    t5=t5 + 21.6412*t1*t2*t3
    t5=t5 + 0.0136*t1*t1*t1
    t5=t5 + 5.3467*t2*t2*t2
    t5=t5 + 0.4352*t3*t3*t3
    t5=t5 + 2.353*t2*t1*t1
    t5=t5 + −11.1333*t1*t2*t2
    t5=t5 + −11.3915*t1*t3*t3
    t5=t5 + −2.089*t3*t1*t1
    t5=t5 + −11.921*t3*t2*t2
    t5=t5 + 6.8004*t2*t3*t3
    t6 = −35.6965
    t6=t6 + −34.3335*t1
    t6=t6 + 8.3038*stdev
    t6=t6 + 50.8947*t3
    t6=t6 + −0.4694*t1*t1
    t6=t6 + −3.7115*stdev*stdev
    t6=t6 + −9.7482*t3*t3
    t6=t6 + 9.4526*t1*stdev
    t6=t6 + 8.0349*t1*t3
    t6=t6 + −10.3683*stdev*t3
    t6=t6 + −0.6248*t1*stdev*t3
    t6=t6 + 0.033*t1*t1*t1
    t6=t6 + 4.454l*stdev*stdev*stdev
    t6=t6 + 0.5147*t3*t3*t3
    t6=t6 + −0.2535*stdev*t1*t1
    t6=t6 + 0.6433*t1*stdev*stdev
    t6=t6 + −0.5219*t1*t3*t3
    t6=t6 + 0.0365*t3*t1*t1
    t6=t6 + −3.4256*t3*stdev*stdev
    t6=t6 + 1.502*stdev*t3*t3
    t7 = 3.821
    t7=t7 + −2.6472*t4
    t7=t7 + 4.7821*t5
    t7=t7 + −2.8123*t6
    t7=t7 + −2.8771*t4*t4
    t7=t7 + −5.9143*t5*t5
    t7=t7 + 0.8615*t6*t6
    t7=t7 + 8.755*t4*t5
    t7=t7 + −2.6803*t4*t6
    t7=t7 + 2.0996*t5*t6
    t7=t7 + 1.951*t4*t5*t6
    t7=t7 + 1.674*t4*t4*t4
    t7=t7 + 0.1775*t5*t5*t5
    t7=t7 + −0.4787*t6*t6*t6
    t7=t7 + −3.9432*t5*t4*t4
    t7=t7 + 2.5218*t4*t5*t5
    t7=t7 + 0.1642*t4*t6*t6
    t7=t7 + −0.8945*t6*t4*t4
    t7=t7 + −2.3395*t6*t5*t5
    t7=t7 + 1.1562*t5*t6*t6
    t8 = −2.2118
    t8=t8 + 3.9246*t4
    t8=t8 + 29.6485*stdev
    t8=t8 + −4.3768*t5
    t8=t8 + −5.1916*t4*t4
    t8=t8 + −24.7618*stdev*stdev
    t8=t8 + −6.6462*t5*t5
    t8=t8 + −18.2263*t4*stdev
    t8=t8 + 12.1779*t4*t5
    t8=t8 + 15.0158*stdev*t5
    t8=t8 + −2.1248*t4*stdev*t5
    t8=t8 + 0.895*t4*t4*t4
    t8=t8 + 5.6838*stdev*stdev*stdev
    t8=t8 + −0.4061*t5*t5*t5
    t8=t8 + 1.0503*stdev*t4*t4
    t8=t8 + 7.1515*t4*stdev*stdev
    t8=t8 + 1.7875*t4*t5*t5
    t8=t8 + −2.293*t5*t4*t4
    t8=t8 + −5.6934*t5*stdev*stdev
    t8=t8 + 1.1406*stdev*t5*t5
    nbins = 251.4737
    nbins=nbins + 49.4576*t7
    nbins=nbins + −422.8133*stdev
    nbins=nbins + −79.0417*t8
    nbins=nbins + 2.6774*t7*t7
    nbins=nbins + 224.8445*stdev*stdev
    nbins=nbins + 10.196*t8*t8
    nbins=nbins + −33.2568*t7*stdev
    nbins=nbins + −11.5861*t7*t8
    nbins=nbins + 67.0927*stdev*t8
    nbins=nbins + 7.0562*t7*stdev*t8
    nbins=nbins + 0.5882*t7*t7*t7
    nbins=nbins + −38.7188*stdev*stdev*stdev
    nbins=nbins + −0.8134*t8*t8*t8
    nbins=nbins + −2.2341*stdev*t7*t7
    nbins=nbins + 4.2043*t7*stdev*stdev
    nbins=nbins + 2.0341*t7*t8*t8
    nbins=nbins + −1.823*t8*t7*t7
    nbins=nbins + −12.6836*t8*stdev*stdev
    nbins=nbins + −5.6006*stdev*t8*t8
    nbins = int(nbins)
    print “nbins = ”,format$(nbins,“0.000000”)
    end
  • 7. Bin Data using optimal number of bins and Delete Mode
  • call calchist(YY1,m,nbins,zzz,n)
    subroutine calchist(Y,m,nbin,E,p)
    implicit none
    integer nbin,m,i,j,maxbin,maxbval,n,p
    real minD,maxD,rngD,minbinD,maxbinD,meanA,stdevA
    real histt(0:nbin−1)
    real D(0:m−1),E(0:m−1,0:3),Y(0:m−1,0:3),A(0:m−1)
    minD=Y(0,3)
    maxD=Y(0,3)
    do i=0, m−1
    D(i)=Y(i,3)
    if(D(i).gt.maxD)maxD=D(i)
    if(D(i).lt.minD)minD=D(i)
    enddo
    rngD=maxD−minD
    do i=0,nbin−1
    histt(i)=0
    enddo
    do i=0,m−1
    do j=0,nbin−1
    if(D(i).ge.(minD+j*rngD/nbin) .and. D(i).lt.
    + (minD+(j+1)*rngD/nbin))histt(j)=histt(j)+1
    enddo
    enddo
    maxbin=0
    maxbval=histt(0)
    do j=1,nbin−1
    if(histt(j).ge.maxbval) then
    maxbin=j
    maxbval=histt(j)
    endif
    enddo
    minbinD=minD+maxbin*rngD/nbin
    maxbinD=minD+(maxbin+1)*rngD/nbin
    A(0)=0
    n=0
    p=0
    do i=0,m−1
    if(D(i).ge.minbinD .and. D(i).le.maxbinD) then
    A(n)=D(i)
    n=n+1
    else
    do j=0,3
    E(p,j)=Y(i,j)
    enddo
    p=p+1
    endif
    enddo
    call mean(A,n,meanA)
    call stdev(A,n,stdevA)
    do i=0,p−1
    E(i,3)=(E(i,3)−meanA)/stdevA
    enddo
    return
    end
  • 8. Apply Vehicle Assembly Recognizer Decision equation Data Model
  • cls
     on error resume next
     input “xloc => ”, xloc
     avg0=28.8234
     dev0=16.2348
     xloc = (xloc − avg0) / dev0
     input “yloc => ”, yloc
     avg1=24.7133
     dev1=5.1657
     yloc = (yloc − avg1) / dev1
     input “zloc => ”, zloc
     avg2=15.1265
     dev2=4.2319
     zloc = (zloc − avg2) / dev2
     input “zval => ”, zval
     avg3=28.9563
     dev3=12.9545
     zval = (zval − avg3) / dev3
     t1 = 0.1
     t1=t1 + −0.1508*xloc
     t1=t1 + −0.1539*yloc
     t1=t1 + 1.1732*zloc
     t1=t1 + −0.0228*xloc*xloc
     t1=t1 + 0.0079*yloc*yloc
     t1=t1 + −0.0833*zloc*zloc
     t1=t1 + −0.1833*xloc*yloc
     t1=t1 + −0.1095*xloc*zloc
     t1=t1 + 0.0294*yloc*zloc
     t1=t1 + −0.0265*xloc*yloc*zloc
     t1=t1 + 0.0165*xloc*xloc*xloc
     t1=t1 + 0.0046*yloc*yloc*yloc
     t1=t1 + −0.1393*zloc*zloc*zloc
     t1=t1 + 0.0516*yloc*xloc*xloc
     t1=t1 + −0.0016*xloc*yloc*yloc
     t1=t1 + 0.0422*xloc*zloc*zloc
     t1=t1 + 0.0464*zloc*xloc*xloc
     t1=t1 + −0.0008*zloc*yloc*yloc
     t1=t1 + 0.0074*yloc*zloc*zloc
     t2 = 0.1147
     t2=t2 + 0.0036*yloc
     t2=t2 + 1.2614*zloc
     t2=t2 + 0.0105*zval
     t2=t2 + 0.0363*yloc*yloc
     t2=t2 + −0.0721*zloc*zloc
     t2=t2 + −0.0023*zval*zval
     t2=t2 + 0.0742*yloc*zloc
     t2=t2 + 0.0309*yloc*zval
     t2=t2 + −0.0188*zloc*zval
     t2=t2 + 0.0129*yloc*zloc*zval
     t2=t2 + 0.0088*yloc*yloc*yloc
     t2=t2 + −0.159*zloc*zloc*zloc
     t2=t2 + 0.0004*zval*zval*zval
     t2=t2 + 0.0237*zloc*yloc*yloc
     t2=t2 + 0.0145*yloc*zloc*zloc
     t2=t2 + −0.0056*yloc*zval*zval
     t2=t2 + 0.0007*zval*yloc*yloc
     t2=t2 + −0.0143*zval*zloc*zloc
     t2=t2 + 0.0071*zloc*zval*zval
     vehicreg = −0.0902
     vehicreg=vehicreg + 1.1065*t1
     vehicreg=vehicreg + −1.4047*zloc
     vehicreg=vehicreg + 1.267*t2
     vehicreg=vehicreg + −0.1239*t1*t1
     vehicreg=vehicreg + −0.3097*zloc*zloc
     vehicreg=vehicreg + −1.7494*t2*t2
     vehicreg=vehicreg + −0.6863*t1*zloc
     vehicreg=vehicreg + 1.35*t1*t2
     vehicreg=vehicreg + 1.5229*zloc*t2
     vehicreg=vehicreg + −0.4454*t1*zloc*t2
     vehicreg=vehicreg + −2.1904*t1*t1*t1
     vehicreg=vehicreg + 0.3772*zloc*zloc*zloc
     vehicreg=vehicreg + 3.0995*t2*t2*t2
     vehicreg=vehicreg + 0.6835*zloc*t1*t1
     vehicreg=vehicreg + −0.0339*t1*zloc*zloc
     vehicreg=vehicreg + −7.117*t1*t2*t2
     vehicreg=vehicreg + 6.3359*t2*t1*t1
     vehicreg=vehicreg + −0.2997*t2*zloc*zloc
     vehicreg=vehicreg + −0.4166*zloc*t2*t2
     vehicreg= vehicreg*0.8427 + 2.1317
     print “vehicreg = ”, format$(vehicreg,“0.000000”)
     end
  • 9. Remove Vehicle Components
  • do i=0,n−1
     zj1(i)=real(nint(zj1(i)))
     if (zj1(i).lt.0 .or. zj1(i).gt.5)then
     zj1(i)=1
     else
     zj1(i)=0
     end if
    enddo
  • 10. Apply Target Medium Z Identification Decision equation Data Model
  • cls
    on error resume next
    input “xloc => ”, xloc
    avg0=28.8234
    dev0=16.2348
    xloc = (xloc − avg0) / dev0
    input “yloc => ”, yloc
    avg1=24.7133
    dev1=5.1657
    yloc = (yloc − avg1) / dev1
    input “zloc => ”, zloc
    avg2=15.1265
    dev2=4.2319
    zloc = (zloc − avg2) / dev2
    input “zval => ”, zval
    avg3=28.9563
    dev3=12.9545
    zval = (zval − avg3) / dev3
    t1 = 0.1
    t1=t1 + −0.1508*xloc
    t1=t1 + −0.1539*yloc
    t1=t1 + 1.1732*zloc
    t1=t1 + −0.0228*xloc*xloc
    t1=t1 + 0.0079*yloc*yloc
    t1=t1 + −0.0833*zloc*zloc
    t1=t1 + −0.1833*xloc*yloc
    t1=t1 + −0.1095*xloc*zloc
    t1=t1 + 0.0294*yloc*zloc
    t1=t1 + −0.0265*xloc*yloc*zloc
    t1=t1 + 0.0165*xloc*xloc*xloc
    t1=t1 + 0.0046*yloc*yloc*yloc
    t1=t1 + −0.1393*zloc*zloc*zloc
    t1=t1 + 0.0516*yloc*xloc*xloc
    t1=t1 + −0.0016*xloc*yloc*yloc
    t1=t1 + 0.0422*xloc*zloc*zloc
    t1=t1 + 0.0464*zloc*xloc*xloc
    t1=t1 + −0.0008*zloc*yloc*yloc
    t1=t1 + 0.0074*yloc*zloc*zloc
    t2 = 0.032
    t2=t2 + −0.2285*xloc
    t2=t2 + 1.0758*zloc
    t2=t2 + 0.0218*zval
    t2=t2 + 0.0643*xloc*xloc
    t2=t2 + −0.0616*zloc*zloc
    t2=t2 + −0.0043*zval*zval
    t2=t2 + −0.2528*xloc*zloc
    t2=t2 + −0.0196*xloc*zval
    t2=t2 + −0.0048*zloc*zval
    t2=t2 + −0.0193*xloc*zloc*zval
    t2=t2 + 0.0001*xloc*xloc*xloc
    t2=t2 + −0.1435*zloc*zloc*zloc
    t2=t2 + 0.0005*zval*zval*zval
    t2=t2 + 0.0996*zloc*xloc*xloc
    t2=t2 + 0.0406*xloc*zloc*zloc
    t2=t2 + 0.0003*xloc*zval*zval
    t2=t2 + −0.001*zval*xloc*xloc
    t2=t2 + −0.0125*zval*zloc*zloc
    t2=t2 + 0.0036*zloc*zval*zval
    t3 = 0.1147
    t3=t3 + 0.0036*yloc
    t3=t3 + 1.2614*zloc
    t3=t3 + 0.0105*zval
    t3=t3 + 0.0363*yloc*yloc
    t3=t3 + −0.0721*zloc*zloc
    t3=t3 + −0.0023*zval*zval
    t3=t3 + 0.0742*yloc*zloc
    t3=t3 + 0.0309*yloc*zval
    t3=t3 + −0.0188*zloc*zval
    t3=t3 + 0.0129*yloc*zloc*zval
    t3=t3 + 0.0088*yloc*yloc*yloc
    t3=t3 + −0.159*zloc*zloc*zloc
    t3=t3 + 0.0004*zval*zval*zval
    t3=t3 + 0.0237*zloc*yloc*yloc
    t3=t3 + 0.0145*yloc*zloc*zloc
    t3=t3 + −0.0056*yloc*zval*zval
    t3=t3 + 0.0007*zval*yloc*yloc
    t3=t3 + −0.0143*zval*zloc*zloc
    t3=t3 + 0.0071*zloc*zval*zval
    t4 = −0.0902
    t4=t4 + 1.1065*t1
    t4=t4 + −1.4047*zloc
    t4=t4 + 1.267*t3
    t4=t4 + −0.1239*t1*t1
    t4=t4 + −0.3097*zloc*zloc
    t4=t4 + −1.7494*t3*t3
    t4=t4 + −0.6863*t1*zloc
    t4=t4 + 1.35*t1*t3
    t4=t4 + 1.5229*zloc*t3
    t4=t4 + −0.4454*t1*zloc*t3
    t4=t4 + −2.1904*t1*t1*t1
    t4=t4 + 0.3772*zloc*zloc*zloc
    t4=t4 + 3.0995*t3*t3*t3
    t4=t4 + 0.6835*zloc*t1*t1
    t4=t4 + −0.0339*t1*zloc*zloc
    t4=t4 + −7.117*t1*t3*t3
    t4=t4 + 6.3359*t3*t1*t1
    t4=t4 + −0.2997*t3*zloc*zloc
    t4=t4 + −0.4166*zloc*t3*t3
    t5 = 0.1215
    t5=t5 + −0.3914*t2
    t5=t5 + −0.1228*xloc
    t5=t5 + 1.4642*t3
    t5=t5 + −2.8041*t2*t2
    t5=t5 + −0.1571*xloc*xloc
    t5=t5 + −2.8051*t3*t3
    t5=t5 + −0.6428*t2*xloc
    t5=t5 + 5.2211*t2*t3
    t5=t5 + 0.0726*xloc*t3
    t5=t5 + −4.1602*t2*xloc*t3
    t5=t5 + 3.817*t2*t2*t2
    t5=t5 + 0.034*xloc*xloc*xloc
    t5=t5 + −1.3168*t3*t3*t3
    t5=t5 + 1.859*xloc*t2*t2
    t5=t5 + 0.3431*t2*xloc*xloc
    t5=t5 + 6.6148*t2*t3*t3
    t5=t5 + −9.3625*t3*t2*t2
    t5=t5 + −0.4085*t3*xloc*xloc
    t5=t5 + 1.8654*xloc*t3*t3
    t6 = 0.0032
    t6=t6 + 1.9491*t3
    t6=t6 + −0.0768*xloc
    t6=t6 + −0.9715*zloc
    t6=t6 + −0.8872*t3*t3
    t6=t6 + −0.1115*xloc*xloc
    t6=t6 + −0.4895*zloc*zloc
    t6=t6 + −0.2123*t3*xloc
    t6=t6 + 1.2271*t3*zloc
    t6=t6 + −0.119*xloc*zloc
    t6=t6 + 0.019*t3*xloc*zloc
    t6=t6 + 0.0383*t3*t3*t3
    t6=t6 + 0.0252*xloc*xloc*xloc
    t6=t6 + 0.3739*zloc*zloc*zloc
    t6=t6 + −0.2305*xloc*t3*t3
    t6=t6 + −0.0578*t3*xloc*xloc
    t6=t6 + −0.4851*t3*zloc*zloc
    t6=t6 + −0.0524*zloc*t3*t3
    t6=t6 + 0.0566*zloc*xloc*xloc
    t6=t6 + 0.0326*xloc*zloc*zloc
    t7 = −0.0003
    t7=t7 + 1.7744*t5
    t7=t7 + −0.01*zloc
    t7=t7 + −0.7502*t6
    t7=t7 + 0.2615*t5*t5
    t7=t7 + −0.2461*zloc*zloc
    t7=t7 + −0.4588*t6*t6
    t7=t7 + −0.2182*t5*zloc
    t7=t7 + −0.0551*t5*t6
    t7=t7 + 0.7274*zloc*t6
    t7=t7 + 3.2643*t5*zloc*t6
    t7=t7 + −2.9004*t5*t5*t5
    t7=t7 + 0.2584*zloc*zloc*zloc
    t7=t7 + 4.5188*t6*t6*t6
    t7=t7 + −1.9513*zloc*t5*t5
    t7=t7 + −0.0356*t5*zloc*zloc
    t7=t7 + −12.5793*t5*t6*t6
    t7=t7 + 10.8537*t6*t5*t5
    t7=t7 + −0.6884*t6*zloc*zloc
    t7=t7 + −0.7478*zloc*t6*t6
    t8 = 0.0086
    t8=t8 + 0.221*t4
    t8=t8 + −0.0715*zloc
    t8=t8 + 0.84*t5
    t8=t8 + −0.2009*t4*t4
    t8=t8 + −0.234*zloc*zloc
    t8=t8 + 0.1087*t5*t5
    t8=t8 + 0.5239*t4*zloc
    t8=t8 + −0.1962*t4*t5
    t8=t8 + −0.0019*zloc*t5
    t8=t8 + 1.0789*t4*zloc*t5
    t8=t8 + 1.6506*t4*t4*t4
    t8=t8 + 0.1764*zloc*zloc*zloc
    t8=t8 + −1.0135*t5*t5*t5
    t8=t8 + −0.0216*zloc*t4*t4
    t8=t8 + −0.4746*t4*zloc*zloc
    t8=t8 + 4.2787*t4*t5*t5
    t8=t8 + −4.8714*t5*t4*t4
    t8=t8 + 0.0866*t5*zloc*zloc
    t8=t8 + −0.8898*zloc*t5*t5
    t9 = 0.03
    t9=t9 + 0.3106*t4
    t9=t9 + 0.0331*xloc
    t9=t9 + 0.6825*t5
    t9=t9 + 0.6573*t4*t4
    t9=t9 + −0.0117*xloc*xloc
    t9=t9 + 0.4201*t5*t5
    t9=t9 + 0.3835*t4*xloc
    t9=t9 + −1.1068*t4*t5
    t9=t9 + −0.36*xloc*t5
    t9=t9 + 0.6052*t4*xloc*t5
    t9=t9 + 0.4543*t4*t4*t4
    t9=t9 + −0.0001*xloc*xloc*xloc
    t9=t9 + −0.7816*t5*t5*t5
    t9=t9 + −0.3329*xloc*t4*t4
    t9=t9 + −0.0653*t4*xloc*xloc
    t9=t9 + 2.0233*t4*t5*t5
    t9=t9 + −1.6749*t5*t4*t4
    t9=t9 + 0.0428*t5*xloc*xloc
    t9=t9 + −0.2963*xloc*t5*t5
    targid = −0.0028
    targid=targid + 0.9135*t7
    targid=targid + 0.1295*t8
    targid=targid + −0.0366*t9
    targid=targid + 0.4651*t7*t7
    targid=targid + −3.707*t8*t8
    targid=targid + 1.377*t9*t9
    targid=targid + 4.4745*t7*t8
    targid=targid + −5.0282*t7*t9
    targid=targid + 2.4147*t8*t9
    targid=targid + 69.3333*t7*t8*t9
    targid=targid + −1.2669*t7*t7*t7
    targid=targid + 31.8732*t8*t8*t8
    targid=targid + 1.0329*t9*t9*t9
    targid=targid + 1.0146*t8*t7*t7
    targid=targid + −34.6345*t7*t8*t8
    targid=targid + −39.3371*t7*t9*t9
    targid=targid + 3.2002*t9*t7*t7
    targid=targid + −65.7963*t9*t8*t8
    targid=targid + 34.5815*t8*t9*t9
    targid=targid*0.8427 + 2.1317
    print “targid = ”, format$(targid, “0.000000”)
    end
  • 11. Extract Candidate Target and determine if target exists and location
  • do i=0,n−1
     zj1(i)=real(nint(zj1(i)))
     if (zj1(i).gt.0 .and. zj1(i).lt.5)then
     zj1(i)=1
     else
     zj1(i)=0
     end if
    enddo
  • 12. Extract Cross-section slices
  • call slices(b,1,n,xp,nxp)
    call slices(b,2,n,yp,nyp)
    call slices(b,3,n,zp,nzp)
    subroutine slices(A,icol,n,B,n1)
    implicit none
    integer i,icol,n,n1
    integer A(0:n−1,0:2)
    integer B(0:n−1)
    integer z(0:n−1,0:2)
    icol=icol−1
    call csort2(A,icol,n,z)
    n1=1
    B(0)=z(0,icol)
    do i=1,n−1
     if(z(i,icol).ne.B(n−1))then
     B(n1)=z(i,icol)
     n1=n1+1
     endif
    enddo
    return
    end
  • 13. Apply Shape Characterizer
  • cls
    on error resume next
    input “S => ”, S
    avg0=0.5
    dev0=0.5
    S = (S − avg0) / dev0
    input “N => ”, N
    avg1=4
    dev1=2.2222
    N = (N − avg1) / dev1
    t1 = 0.5455
    t1=t1 + −1.4983*N
    t1=t1 + −0.404*N*N
    t1=t1 + 0.5154*N*N*N
    t2 = 0
    t2=t2 + 0.2*S
    t2=t2 + −0.2667*N
    t3 = 0
    t3=t3 + 0.2*S
    t3=t3 + 0*S*S
    t3=t3 + 0*S*S*S
    t4 = −1.3457
    t4=t4 + −1.2483*t1
    t4=t4 + 0.9904*N
    t4=t4 + 1.0176*t1*t1
    t4=t4 + 1.8455*N*N
    t4=t4 + 3.2656*t1*N
    t4=t4 + 6.9251*t1*t1*t1
    t4=t4 + −1.1587*N*N*N
    t4=t4 + 5.3817*N*t1*t1
    t4=t4 + −0.1932*t1*N*N
    t5 = −1.319
    t5=t5 + 0.1858*t1
    t5=t5 + −1.4401*t3
    t5=t5 + 1.1002*t1*t1
    t5=t5 + 12.6254*t3*t3
    t5=t5 + 1.4314*t1*t3
    t5=t5 + 0.8973*t1*t1*t1
    t5=t5 + 13.5737*t3*t3*t3
    t5=t5 + 2.8124*t3*t1*t1
    t5=t5 + −5.4825*t1*t3*t3
    t6 = −0.6995
    t6=t6 + −0.4762*t4
    t6=t6 + 0.2221*t5
    t6=t6 + −0.3014*t4*t4
    t6=t6 + 0.1565*t5*t5
    t6=t6 + 0.1268*t4*t5
    t6=t6 + 0.3597*t4*t4*t4
    t6=t6 + 0*t5*t5*t5
    t6=t6 + −0.4057*t5*t4*t4
    t6=t6 + 0.2608*t4*t5*t5
    outval = t6*0.2778 + 0.1667
    print “outval = ”, format$(outval,“0.000000”)
    end
  • 14. Calculate Moments and Cumulants
  • subroutine mean(A,n,meanA)
    implicit none
    integer n,i
    real A(0:n−1)
    real meanA
    meanA=0.0
    do i=0,n−1
     meanA=meanA+A(i)/n
    enddo
    return
    end
    subroutine stdev(A,n,stdevA)
    implicit none
    integer n,i
    real A(0:n−1)
    real stdevA,meanA,s,pp
    stdevA=0.0
    meanA=0.0
    do i=0,n−1
     meanA=meanA+A(i)/n
    enddo
    do i=0,n−1
     s=A(i)−meanA
     pp=s*s
     stdevA=stdevA+pp
    enddo
    stdevA=sqrt(stdevA/(n−1))
    return
    end
    subroutine skewness(A,n,ystat)
    implicit none
    integer n
    real A(0:n−1)
    integer i
    real ystat,ymean,ystdev
    call mean(A,n,ymean)
    call stdev(A,n,ystdev)
    ystat=0
    do i=0,n−1
     ystat=ystat+(1/n)*((A(i)−ymean)/ystdev)**3
    enddo
    return
    end
    subroutine kurtosis(A,n,ystat)
    implicit none
    integer n
    real A(0:n−1)
    integer i
    real ystat,ymean,ystdev
    call mean(A,n,ymean)
    call stdev(A,n,ystdev)
    ystat=0
    do i=0,n−1
     ystat=ystat+(1/n)*((A(i)−ymean)/ystdev)**4
    enddo
    ystat=ystat−3
    return
    end
  • 15. Apply Square Shape Recognizer Data Model
  • cls
     on error resume next
     input “stdev => ”, stdev
     avg0=0
     dev0=1
     stdev = (stdev − avg0) / dev0
     input “skew => ”, skew
     avg1=0
     dev1=1
     skew = (skew − avg1) / dev1
     input “kurt => ”, kurt
     avg2=0
     dev2=1
     kurt = (kurt − avg2) / dev2
     t1 = −8.7325
     t1=t1 + 16.1062*stdev
     t1=t1 + 7.7824*skew
     t1=t1 + −4.2487*kurt
     t1=t1 + −8.4543*stdev*stdev
     t1=t1 + −1.0114*skew*skew
     t1=t1 + −0.4265*kurt*kurt
     t1=t1 + −11.0898*stdev*skew
     t1=t1 + 5.6503*stdev*kurt
     t1=t1 + 1.4876*skew*kurt
     t1=t1 + −1.0844*stdev*skew*kurt
     t1=t1 + 1.1564*stdev*stdev*stdev
     t1=t1 + 0.0664*skew*skew*skew
     t1=t1 + −0.012*kurt*kurt*kurt
     t1=t1 + 3.9996*skew*stdev*stdev
     t1=t1 + 0.6607*stdev*skew*skew
     t1=t1 + 0.2972*stdev*kurt*kurt
     t1=t1 + −1.8273*kurt*stdev*stdev
     t1=t1 + −0.084*kurt*skew*skew
     t1=t1 + 0.0594*skew*kurt*kurt
     t2 = 0.499
     t2=t2 + −0.0445*stdev
     t2=t2 + 0.0027*skew
     t2=t2 + 0.098*stdev*stdev
     t2=t2 + −0.0018*skew*skew
     t2=t2 + −0.0262*stdev*skew
     t2=t2 + −0.0469*stdev*stdev*stdev
     t2=t2 + −0.0032*skew*skew*skew
     t2=t2 + 0.0116*skew*stdev*stdev
     t2=t2 + 0.0099*stdev*skew*skew
     squr = 1439.2517
     squr=squr + −3245.4202*t1
     squr=squr + 5.2508*kurt
     squr=squr + −4734.6232*t2
     squr=squr + 2159.0814*t1*t1
     squr=squr + −0.0368*kurt*kurt
     squr=squr + 6231.9075*t2*t2
     squr=squr + −133.4063*t1*kurt
     squr=squr + 6264.3623*t1*t2
     squr=squr + 112.4382*kurt*t2
     squr=squr + −1674.8553*t1*kurt*t2
     squr=squr + −1172.5311*t1*t1*t1
     squr=squr + 0*kurt*kurt*kurt
     squr=squr + −3869.1525*t2*t2*t2
     squr=squr + 971.6707*kurt*t1*t1
     squr=squr + −0.0339*t1*kurt*kurt
     squr=squr + −3049.0222*t1*t2*t2
     squr=squr + −809.8377*t2*t1*t1
     squr=squr + 0.1072*t2*kurt*kurt
     squr=squr + 724.1183*kurt*t2*t2
     print “squr = ”, format$(squr,“0.000000”)
     end
  • 16. Apply Rectangle Shape Recognizer
  • cls
     on error resume next
     input “stdev => ”, stdev
     avg0=0
     dev0=1
     stdev = (stdev − avg0) / dev0
     input “skew => ”, skew
     avg1=0
     dev1=1
     skew = (skew − avg1) / dev1
     input “kurt => ”, kurt
     avg2=0
     dev2=1
     kurt = (kurt − avg2) / dev2
     t1 = 0.7139
     t1=t1 + −0.4487*stdev
     t1=t1 + −0.135*skew
     t1=t1 + 0.0548*kurt
     t1=t1 + 0.306*stdev*stdev
     t1=t1 + 0.0093*skew*skew
     t1=t1 + 0.0031*kurt*kurt
     t1=t1 + 0.209*stdev*skew
     t1=t1 + −0.089*stdev*kurt
     t1=t1 + −0.0084*skew*kurt
     t1=t1 + 0.0079*stdev*skew*kurt
     t1=t1 + −0.0685*stdev*stdev*stdev
     t1=t1 + −0.004*skew*skew*skew
     t1=t1 + 0.0001*kurt*kurt*kurt
     t1=t1 + −0.0796*skew*stdev*stdev
     t1=t1 + −0.0034*stdev*skew*skew
     t1=t1 + −0.0031*stdev*kurt*kurt
     t1=t1 + 0.0343*kurt*stdev*stdev
     t1=t1 + 0.0015*kurt*skew*skew
     t1=t1 + −0.0003*skew*kurt*kurt
     t2 = 0.5173
     t2=t2 + −0.0904*stdev
     t2=t2 + 0.0113*kurt
     t2=t2 + 0.1138*stdev*stdev
     t2=t2 + 0.0011*kurt*kurt
     t2=t2 + −0.024*stdev*kurt
     t2=t2 + −0.042*stdev*stdev*stdev
     t2=t2 + 0*kurt*kurt*kurt
     t2=t2 + 0.0122*kurt*stdev*stdev
     t2=t2 + −0.0011*stdev*kurt*kurt
     t3 = −77.6056
     t3=t3 + −18069.338*t1
     t3=t3 + 1558.8694*stdev
     t3=t3 + 14563.848*t2
     t3=t3 + −16865.123*t1*t1
     t3=t3 + 0.9483*stdev*stdev
     t3=t3 + −21107.108*t2*t2
     t3=t3 + 18605.424*t1*stdev
     t3=t3 + 52937.839*t1*t2
     t3=t3 + −24846.303*stdev*t2
     t3=t3 + −22824.812*t1*stdev*t2
     t3=t3 + −7165.8933*t1*t1*t1
     t3=t3 + −0.0009*stdev*stdev*stdev
     t3=t3 + 19184.557*t2*t2*t2
     t3=t3 + −7159.3752*stdev*t1*t1
     t3=t3 + −10.8134*t1*stdev*stdev
     t3=t3 + −109868.89*t1*t2*t2
     t3=t3 + 82565.844*t2*t1*t1
     t3=t3 + 8.9252*t2*stdev*stdev
     t3=t3 + 36230.44*stdev*t2*t2
     t4 = −173.1588
     t4=t4 + −1855.8662*t1
     t4=t4 + −19.0692*kurt
     t4=t4 + 2632.1107*t2
     t4=t4 + 4080.3157*t1*t1
     t4=t4 + 0.0104*kurt*kurt
     t4=t4 + 2595.4904*t2*t2
     t4=t4 + 239.0646*t1*kurt
     t4=t4 + −7699.3372*t1*t2
     t4=t4 + −162.953*kurt*t2
     t4=t4 + 984.7128*t1*kurt*t2
     t4=t4 + −3919.6113*t1*t1*t1
     t4=t4 + 0*kurt*kurt*kurt
     t4=t4 + −2885.6103*t2*t2*t2
     t4=t4 + −731.566*kurt*t1*t1
     t4=t4 + 0.0145*t1*kurt*kurt
     t4=t4 + −3988.0655*t1*t2*t2
     t4=t4 + 11124.641*t2*t1*t1
     t4=t4 + −0.0352*t2*kurt*kurt
     t4=t4 + −329.0933*kurt*t2*t2
     t5 = 259.3714
     t5=t5 + −859.0387*t4
     t5=t5 + 40.2851*skew
     t5=t5 + −30.9792*kurt
     t5=t5 + 323.8594*t4*t4
     t5=t5 + −2.8428*skew*skew
     t5=t5 + −0.1779*kurt*kurt
     t5=t5 + −152.5373*t4*skew
     t5=t5 + 121.8502*t4*kurt
     t5=t5 + 1.3911*skew*kurt
     t5=t5 + −2.7864*t4*skew*kurt
     t5=t5 + 717.4708*t4*t4*t4
     t5=t5 + −0.0015*skew*skew*skew
     t5=t5 + 0*kurt*kurt*kurt
     t5=t5 + 143.9216*skew*t4*t4
     t5=t5 + 5.6934*t4*skew*skew
     t5=t5 + 0.3564*t4*kurt*kurt
     t5=t5 + −119.7801*kurt*t4*t4
     t5=t5 + 0.0011*kurt*skew*skew
     t5=t5 + −0.0003*skew*kurt*kurt
     rect = 180.678
     rect=rect + −231.9235*t5
     rect=rect + 27.3046*skew
     rect=rect + −9.6504*kurt
     rect=rect + −1234.8733*t5*t5
     rect=rect + −2.1871*skew*skew
     rect=rect + −0.1997*kurt*kurt
     rect=rect + −103.8636*t5*skew
     rect=rect + 36.9092*t5*kurt
     rect=rect + 1.3074*skew*kurt
     rect=rect + −2.6183*t5*skew*kurt
     rect=rect + 1956.0207*t5*t5*t5
     rect=rect + −0.0011*skew*skew*skew
     rect=rect + 0*kurt*kurt*kurt
     rect=rect + 98.4999*skew*t5*t5
     rect=rect + 4.3798*t5*skew*skew
     rect=rect + 0.4*t5*kurt*kurt
     rect=rect + −35.2138*kurt*t5*t5
     rect=rect + 0.001*kurt*skew*skew
     rect=rect + −0.0003*skew*kurt*kurt
     print “rect = ”, format$(rect,“0.000000”)
     end
  • 17. Apply Circle Shape Recognizer Data Model
  • cls
    on error resume next
    input “stdev => ”, stdev
    avg0=0
    dev0=1
    stdev = (stdev − avg0) / dev0
    input “skew => ”, skew
    avg1=0
    dev1=1
    skew = (skew − avg1) / dev1
    input “kurt => ”, kurt
    avg2=0
    dev2=1
    kurt = (kurt − avg2) / dev2
    t1 = 35.3015
    t1=t1 + −10.3986*stdev
    t1=t1 + −50.2487*skew
    t1=t1 + 6.8536*kurt
    t1=t1 + −2.5942*stdev*stdev
    t1=t1 + 22.9365*skew*skew
    t1=t1 + 0.4247*kurt*kurt
    t1=t1 + 13.5646*stdev*skew
    t1=t1 + −1.4197*stdev*kurt
    t1=t1 + −6.3791*skew*kurt
    t1=t1 + 1.0864*stdev*skew*kurt
    t1=t1 + −0.1976*stdev*stdev*stdev
    t1=t1 + −3.0322*skew*skew*skew
    t1=t1 + 0.0082*kurt*kurt*kurt
    t1=t1 + 2.2012*skew*stdev*stdev
    t1=t1 + −5.0368*stdev*skew*skew
    t1=t1 + −0.0547*stdev*kurt*kurt
    t1=t1 + −0.2888*kurt*stdev*stdev
    t1=t1 + 1.3431*kurt*skew*skew
    t1=t1 + −0.1869*skew*kurt*kurt
    t2 = 0.3476
    t2=t2 + 0.319*stdev
    t2=t2 + −0.0112*kurt
    t2=t2 + −0.2213*stdev*stdev
    t2=t2 + −0.0004*kurt*kurt
    t2=t2 + 0.0166*stdev*kurt
    t2=t2 + 0.0399*stdev*stdev*stdev
    t2=t2 + 0*kurt*kurt*kurt
    t2=t2 + −0.0019*kurt*stdev*stdev
    t2=t2 + −0.0002*stdev*kurt*kurt
    t3 = 20.2592
    t3=t3 + 102.8048*t1
    t3=t3 + −55.3313*stdev
    t3=t3 + 10.0486*kurt
    t3=t3 + −923.6519*t1*t1
    t3=t3 + 32.9265*stdev*stdev
    t3=t3 + 0.3638*kurt*kurt
    t3=t3 + 265.0418*t1*stdev
    t3=t3 + −33.2655*t1*kurt
    t3=t3 + −8.0704*stdev*kurt
    t3=t3 + 16.1045*t1*stdev*kurt
    t3=t3 + 1277.8001*t1*t1*t1
    t3=t3 + −0.0589*stdev*stdev*stdev
    t3=t3 + 0*kurt*kurt*kurt
    t3=t3 + −308.801*stdev*t1*t1
    t3=t3 + −65.6686*t1*stdev*stdev
    t3=t3 + −0.7262*t1*kurt*kurt
    t3=t3 + 26.3573*kurt*t1*t1
    t3=t3 + 0.014*kurt*stdev*stdev
    t3=t3 + −0.001*stdev*kurt*kurt
    t4 = 618.027
    t4=t4 + −4441.4235*t1
    t4=t4 + −154.6627*stdev
    t4=t4 + 188.7003*skew
    t4=t4 + 10005.74*t1*t1
    t4=t4 + 66.6965*stdev*stdev
    t4=t4 + 38.4076*skew*skew
    t4=t4 + 1112.1743*t1*stdev
    t4=t4 + −932.3528*t1*skew
    t4=t4 + −117.027*stdev*skew
    t4=t4 + 234.0486*t1*stdev*skew
    t4=t4 + −7186.6583*t1*t1*t1
    t4=t4 + −0.0295*stdev*stdev*stdev
    t4=t4 + 0.004*skew*skew*skew
    t4=t4 + −1605.2637*stdev*t1*t1
    t4=t4 + −133.4835*t1*stdev*stdev
    t4=t4 + −76.8216*t1*skew*skew
    t4=t4 + 1109.94*skew*t1*t1
    t4=t4 + 0.0506*skew*stdev*stdev
    t4=t4 + −0.0234*stdev*skew*skew
    circ = 249.5062
    circ=circ + 85.1877*t3
    circ=circ + −113.5633*stdev
    circ=circ + −1071.3463*t4
    circ=circ + 1361.5581*t3*t3
    circ=circ + −0.6902*stdev*stdev
    circ=circ + 180.1794*t4*t4
    circ=circ + 1066.7217*t3*stdev
    circ=circ + −600.4015*t3*t4
    circ=circ + −607.0379*stdev*t4
    circ=circ + −252.2958*t3*stdev*t4
    circ=circ + −374.621*t3*t3*t3
    circ=circ + 0*stdev*stdev*stdev
    circ=circ + −169.8192*t4*t4*t4
    circ=circ + −941.9394*stdev*t3*t3
    circ=circ + 1.2513*t3*stdev*stdev
    circ=circ + 4700.8014*t3*t4*t4
    circ=circ + −4086.4429*t4*t3*t3
    circ=circ + 0.1286*t4*stdev*stdev
    circ=circ + 729.1219*stdev*t4*t4
    print “circ = ”, format$(circ,“0.000000”)
    end
  • 18. Perform 3D primitive shape recognition (Volumetric) using Volumetric Shape Recognizer Data Model
  • cls
    on error resume next
    input ″sqrrat => ″, sqrrat
    avg0=0.347346
    dev0=0.257595
    sqrrat = (sqrrat − avg0) / dev0
    input ″cirrat => ″, cirrat
    avg1=0.26136
    dev1=0.299084
    cirrat = (cirrat − avg1) / dev1
    input ″recrat => ″, recrat
    avg2=0.461342
    dev2=0.286608
    recrat = (recrat − avg2) / dev2
    t1 = 2.140537
    t1=t1 + −0.554984*sqrrat
    t1=t1 + −1.486669*cirrat
    t1=t1 + −1.961653*recrat
    t1=t1 + −0.723202*sqrrat*sqrrat
    t1=t1 + −2.23146*cirrat*cirrat
    t1=t1 + −0.70339*recrat*recrat
    t1=t1 + −0.986561*sqrrat*cirrat
    t1=t1 + 0.384267*sqrrat*recrat
    t1=t1 + −1.330231*cirrat*recrat
    t1=t1 + 1.146032*sqrrat*cirrat*recrat
    t1=t1 + 0.029627*sqrrat*sqrrat*sqrrat
    t1=t1 + 0.790767*cirrat*cirrat*cirrat
    t1=t1 + −0.203694*recrat*recrat*recrat
    t1=t1 + 0.027664*cirrat*sqrrat*sqrrat
    t1=t1 + 0.767389*sqrrat*cirrat*cirrat
    t1=t1 + −0.034321*sqrrat*recrat*recrat
    t1=t1 + 0.501569*recrat*sqrrat*sqrrat
    t1=t1 + 0.319538*recrat*cirrat*cirrat
    t1=t1 + −0.819217*cirrat*recrat*recrat
    t2 = 1.377919
    t2=t2 + 0.21651*sqrrat
    t2=t2 + −15.398505*sqrrat
    t2=t2 + 18.820342*recrat
    t2=t2 + −0.410596*sqrrat*sqrrat
    t2=t2 + 30.531425*sqrrat*sqrrat
    t2=t2 + 42.929545*recrat*recrat
    t2=t2 + 0.155626*sqrrat*sqrrat
    t2=t2 + −0.038907*sqrrat*recrat
    t2=t2 + −74.056914*sqrrat*recrat
    t2=t2 + 17.119525*sqrrat*sqrrat*recrat
    t2=t2 + 0.030897*sqrrat*sqrrat*sqrrat
    t2=t2 + −44.89291*sqrrat*sqrrat*sqrrat
    t2=t2 + 78.573052*recrat*recrat*recrat
    t2=t2 + 2.52622*sqrrat*sqrrat*sqrrat
    t2=t2 + −5.885253*sqrrat*sqrrat*sqrrat
    t2=t2 + −11.905429*sqrrat*recrat*recrat
    t2=t2 + −3.06317*recrat*sqrrat*sqrrat
    t2=t2 + 166.10598*recrat*sqrrat*sqrrat
    t2=t2 + −201.10207*sqrrat*recrat*recrat
    t3 = 1.267654
    t3=t3 + 0.184478*sqrrat
    t3=t3 + −1.4849*sqrrat
    t3=t3 + 0.210468*recrat
    t3=t3 + −0.381928*sqrrat*sqrrat
    t3=t3 + −2.981706*sqrrat*sqrrat
    t3=t3 + −1.035758*recrat*recrat
    t3=t3 + −0.249815*sqrrat*sqrrat
    t3=t3 + 0.192463*sqrrat*recrat
    t3=t3 + 0.46816*sqrrat*recrat
    t3=t3 + 3.401237*sqrrat*sqrrat*recrat
    t3=t3 + 0.047071*sqrrat*sqrrat*sqrrat
    t3=t3 + 2.184666*sqrrat*sqrrat*sqrrat
    t3=t3 + −0.838692*recrat*recrat*recrat
    t3=t3 + 1.356104*sqrrat*sqrrat*sqrrat
    t3=t3 + 2.039595*sqrrat*sqrrat*sqrrat
    t3=t3 + −2.040051*sqrrat*recrat*recrat
    t3=t3 + −0.677151*recrat*sqrrat*sqrrat
    t3=t3 + 1.295684*recrat*sqrrat*sqrrat
    t3=t3 + −0.225608*sqrrat*recrat*recrat
    shape3d = 0.117942
    shape3d=shape3d + 0.526004*t1
    shape3d=shape3d + −1.047472*t2
    shape3d=shape3d + 1.8487*t3
    shape3d=shape3d + −0.320166*t1*t1
    shape3d=shape3d + −0.587216*t2*t2
    shape3d=shape3d + 3.452296*t3*t3
    shape3d=shape3d + 1.66785*t1*t2
    shape3d=shape3d + −1.0663*t1*t3
    shape3d=shape3d + −3.00491*t2*t3
    shape3d=shape3d + 3.183958*t1*t2*t3
    shape3d=shape3d + −0.033971*t1*t1*t1
    shape3d=shape3d + 2.711255*t2*t2*t2
    shape3d=shape3d + 0.580184*t3*t3*t3
    shape3d=shape3d + 2.056935*t2*t1*t1
    shape3d=shape3d + −2.41716*t1*t2*t2
    shape3d=shape3d + −0.908928*t1*t3*t3
    shape3d=shape3d + −1.840469*t3*t1*t1
    shape3d=shape3d + −7.163242*t3*t2*t2
    shape3d=shape3d + 3.809345*t2*t3*t3
    shape3d = shape3d*0.725898 + 2.565217
    print ″shape3d = ″, format$(shape3d,″0.000000″)
    if int(shape3d)=1 then shape$=”shell”
    if int(shape3d)=2 then shape$=”cylindrical”
    if int(shape3d)=3 then shape$=”box-like”
    if int(shape3d)=4 then shape$=”spherical”
    if int(shape3d)=5 then shape$=”unrecognized (possibly multiple)”
    if int(shape3d)<1 or int(shape3d)>5 then shape$=”no definite object”
    end
  • 19. Calculate centroids and covariances
  •   call calccovar(f,n,gcov)
      if(gcov(0,0).gt.sqrt(gcov1 (0,0)).or.
      +  gcov(1,1).gt.sqrt(gcov1(1,1)))shape$=”no definite object”
     nother = total_n_slices − nrectangles − ncircles − nsquares
     IF nother > nrectangles AND nother > ncircles AND nother > nsquares
    THEN shape$=”unrecognized (possibly multiple)”
      subroutine calccovar(A,n,covar1)
      implicit none
      integer n,i,m,j,k,l1,l2
      real A(0:31,0:31,0:n−1)
      real B(0:n−1,0:1)
      real covar(0:1,0:1)
      real covar1(0:1,0:1,0:n−1)
      do i=0,n−1
      m=0
      do j=0,31
       do k=0,31
       B(m,0)=j*A(j,k,i)
       B(m,1)=k*A(j,k,i)
       m=m+1
       enddo
      enddo
      call covarz(covar,B,2,m)
      do l1=0,1
       do l2=0,1
       covar1(l1,l2,i)=covar(l1,l2)
       enddo
      enddo
      enddo
      return
      end
  • The disclosed and other embodiments and the functional operations described in this specification can be implemented in digital electronic circuitry, or in computer software, firmware, or hardware, including the structures disclosed in this specification and their structural equivalents, or in combinations of one or more of them. The disclosed and other embodiments can be implemented as one or more computer program products, i.e., one or more modules of computer program instructions encoded on a computer readable medium for execution by, or to control the operation of, data processing apparatus. The computer readable medium can be a machine-readable storage device, a machine-readable storage substrate, a memory device, a composition of matter effecting a machine-readable propagated signal, or a combination of one or more them. The term “data processing apparatus” encompasses all apparatus, devices, and machines for processing data, including by way of example a programmable processor, a computer, or multiple processors or computers. The apparatus can include, in addition to hardware, code that creates an execution environment for the computer program in question, e.g., code that constitutes processor firmware, a protocol stack, a database management system, an operating system, or a combination of one or more of them. A propagated signal is an artificially generated signal, e.g., a machine-generated electrical, optical, or electromagnetic signal, that is generated to encode information for transmission to suitable receiver apparatus.
  • A computer program (also known as a program, software, software application, script, or code) can be written in any form of programming language, including compiled or interpreted languages, and it can be deployed in any form, including as a stand-alone program or as a module, component, subroutine, or other unit suitable for use in a computing environment. A computer program does not necessarily correspond to a file in a file system. A program can be stored in a portion of a file that holds other programs or data (e.g., one or more scripts stored in a markup language document), in a single file dedicated to the program in question, or in multiple coordinated files (e.g., files that store one or more modules, sub-programs, or portions of code). A computer program can be deployed to be executed on one computer or on multiple computers that are located at one site or distributed across multiple sites and interconnected by a communication network.
  • The processes and logic flows described in this specification can be performed by one or more programmable processors executing one or more computer programs to perform functions by operating on input data and generating output. The processes and logic flows can also be performed by, and apparatus can also be implemented as, special purpose logic circuitry, e.g., an FPGA (field programmable gate array) or an ASIC (application-specific integrated circuit).
  • Processors suitable for the execution of a computer program include, by way of example, both general and special purpose microprocessors, and any one or more processors of any kind of digital computer. Generally, a processor will receive instructions and data from a read-only memory or a random access memory or both. The essential elements of a computer are a processor for performing instructions and one or more memory devices for storing instructions and data. Generally, a computer will also include, or be operatively coupled to receive data from or transfer data to, or both, one or more mass storage devices for storing data, e.g., magnetic, magneto-optical disks, or optical disks. However, a computer need not have such devices. Computer readable media suitable for storing computer program instructions and data include all forms of non-volatile memory, media and memory devices, including by way of example semiconductor memory devices, e.g., EPROM, EEPROM, and flash memory devices; magnetic disks, e.g., internal hard disks or removable disks; magneto-optical disks; and CD-ROM and DVD-ROM disks. The processor and the memory can be supplemented by, or incorporated in, special purpose logic circuitry.
  • The disclosed embodiments can be implemented in a computing system that includes a back-end component, e.g., as a data server, or that includes a middleware component, e.g., an application server, or that includes a front-end component, e.g., a client computer having a graphical user interface or a Web browser through which a user can interact with an implementation of what is disclosed here, or any combination of one or more such back-end, middleware, or front-end components. The components of the system can be interconnected by any form or medium of digital data communication, e.g., a communication network. Examples of communication networks include a local area network (“LAN”) and a wide area network (“WAN”), e.g., the Internet.
  • A computer system for implementing the disclosed embodiments can include client computers (clients) and server computers (servers). A client and a server are generally remote from each other and typically interact through a communication network. The relationship of client and server can arise by virtue of computer programs running on the respective computers and having a client-server relationship to each other.
  • While this specification contains many specifics, these should not be construed as limitations on the scope of any invention or of what may be claimed, but rather as descriptions of features specific to particular embodiments. Certain features that are described in this specification in the context of separate embodiments can also be implemented in combination in a single embodiment. Conversely, various features that are described in the context of a single embodiment can also be implemented in multiple embodiments separately or in any suitable subcombination. Moreover, although features may be described above as acting in certain combinations and even initially claimed as such, one or more features from a claimed combination can in some cases be excised from the combination, and the claimed combination may be directed to a subcombination or variation of a subcombination.
  • Similarly, operations are depicted in the drawings in a particular order, and such operations should be performed in the particular order shown or in sequential order, and that all illustrated operations be performed, to achieve desirable results. In certain circumstances, multitasking and parallel processing may be advantageous. Moreover, the separation of various system components in the embodiments described above should not be understood as requiring such separation in all embodiments, and it should be understood that the described program components and systems can generally be integrated together in a single software product or packaged into multiple software products.
  • Thus, particular embodiments have been described. Other embodiments are within the scope of the following claims.

Claims (1)

1. A computer-automated method for processing muon vehicle imaging data of a vehicle under inspection located in a vehicle inspection region within a muon tomography vehicle imaging system, comprising:
processing muon vehicle imaging data obtained from the vehicle inspection region to obtain a histogram of the muon vehicle imaging data at different positions in the vehicle inspection region;
separating the muon vehicle imaging data into bins based on the histogram;
removing a subset of the muon vehicle imaging data in a mode bin that has higher frequencies of occurrence than remaining muon vehicle imaging data from the muon vehicle imaging data to retain the remaining muon vehicle imaging data for further processing;
using a vehicle assembly recognizer Data Model for identifying vehicle components from the remaining muon vehicle imaging data;
applying the vehicle assembly recognizer Data Model to process the remaining muon vehicle imaging data to produce an image of the vehicle inspection region by removing vehicle components;
using a target identification Data Model for identifying a target object from the remaining muon vehicle imaging data;
applying the target identification Data Model to process data of the image produced after applying the vehicle assembly recognizer Data Model to produce an image of the target object; and
processing the image of the target object to determine a location and a shape of the target object in the vehicle under inspection.
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US9220889B2 (en) 2008-02-11 2015-12-29 Intelect Medical, Inc. Directional electrode devices with locating features
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US9310323B2 (en) 2009-05-16 2016-04-12 Rapiscan Systems, Inc. Systems and methods for high-Z threat alarm resolution
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US9792412B2 (en) 2012-11-01 2017-10-17 Boston Scientific Neuromodulation Corporation Systems and methods for VOA model generation and use
US9355502B2 (en) * 2012-12-12 2016-05-31 Analogic Corporation Synthetic image generation by combining image of object under examination with image of target
US9557427B2 (en) 2014-01-08 2017-01-31 Rapiscan Systems, Inc. Thin gap chamber neutron detectors
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US9959388B2 (en) 2014-07-24 2018-05-01 Boston Scientific Neuromodulation Corporation Systems, devices, and methods for providing electrical stimulation therapy feedback
US10272247B2 (en) 2014-07-30 2019-04-30 Boston Scientific Neuromodulation Corporation Systems and methods for stimulation-related volume analysis, creation, and sharing with integrated surgical planning and stimulation programming
US10265528B2 (en) 2014-07-30 2019-04-23 Boston Scientific Neuromodulation Corporation Systems and methods for electrical stimulation-related patient population volume analysis and use
WO2016028929A1 (en) * 2014-08-19 2016-02-25 Decision Sciences International Corporation Calibrating modular charged particle detector arrays
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US10191180B2 (en) 2014-12-12 2019-01-29 Lingacom Ltd. Large scale gas electron multiplier and detection method
US11125904B2 (en) 2014-12-12 2021-09-21 Lingacom Ltd. Large scale gas electron multiplier with sealable opening
WO2016145105A1 (en) * 2015-03-10 2016-09-15 Decision Sciences International Corporation Sensor fusion with muon detector arrays to augment tomographic imaging using ambient cosmic rays
US10780283B2 (en) 2015-05-26 2020-09-22 Boston Scientific Neuromodulation Corporation Systems and methods for analyzing electrical stimulation and selecting or manipulating volumes of activation
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WO2017003946A1 (en) 2015-06-29 2017-01-05 Boston Scientific Neuromodulation Corporation Systems and methods for selecting stimulation parameters based on stimulation target region, effects, or side effects
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US10071249B2 (en) 2015-10-09 2018-09-11 Boston Scientific Neuromodulation Corporation System and methods for clinical effects mapping for directional stimulation leads
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WO2017223505A2 (en) 2016-06-24 2017-12-28 Boston Scientific Neuromodulation Corporation Systems and methods for visual analytics of clinical effects
WO2018044881A1 (en) 2016-09-02 2018-03-08 Boston Scientific Neuromodulation Corporation Systems and methods for visualizing and directing stimulation of neural elements
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JP6828149B2 (en) 2016-10-14 2021-02-10 ボストン サイエンティフィック ニューロモデュレイション コーポレイション Systems and methods for closed-loop determination of stimulation parameter settings for electrical stimulation systems
US10792501B2 (en) 2017-01-03 2020-10-06 Boston Scientific Neuromodulation Corporation Systems and methods for selecting MRI-compatible stimulation parameters
EP3519043B1 (en) 2017-01-10 2020-08-12 Boston Scientific Neuromodulation Corporation Systems and methods for creating stimulation programs based on user-defined areas or volumes
US10625082B2 (en) 2017-03-15 2020-04-21 Boston Scientific Neuromodulation Corporation Visualization of deep brain stimulation efficacy
US11357986B2 (en) 2017-04-03 2022-06-14 Boston Scientific Neuromodulation Corporation Systems and methods for estimating a volume of activation using a compressed database of threshold values
WO2019009664A1 (en) 2017-07-07 2019-01-10 Koh Young Technology Inc Apparatus for optimizing inspection of exterior of target object and method thereof
WO2019014224A1 (en) 2017-07-14 2019-01-17 Boston Scientific Neuromodulation Corporation Systems and methods for estimating clinical effects of electrical stimulation
US10960214B2 (en) 2017-08-15 2021-03-30 Boston Scientific Neuromodulation Corporation Systems and methods for controlling electrical stimulation using multiple stimulation fields
EP3561459B1 (en) * 2018-04-25 2021-09-15 VEGA Grieshaber KG Device and method for measuring a medium fill level or density by the help of muons
AU2019260740B2 (en) 2018-04-27 2022-05-19 Boston Scientific Neuromodulation Corporation Multi-mode electrical stimulation systems and methods of making and using
WO2019210214A1 (en) 2018-04-27 2019-10-31 Boston Scientific Neuromodulation Corporation Systems for visualizing and programming electrical stimulation
US10381205B1 (en) 2018-05-04 2019-08-13 Douglas Electrical Components, Inc. Muon drift tube and method of making same
US10854055B1 (en) * 2019-10-17 2020-12-01 The Travelers Indemnity Company Systems and methods for artificial intelligence (AI) theft prevention and recovery
EP4153980A4 (en) * 2020-06-16 2024-07-03 Atomic Energy of Canada Limited/ Énergie Atomique du Canada Limitée Muon tomography method and apparatus
WO2022232036A1 (en) 2021-04-27 2022-11-03 Boston Scientific Neuromodulation Corporation Systems and methods for automated programming of electrical stimulation
US12403313B2 (en) 2021-06-15 2025-09-02 Boston Scientific Neuromodulation Corporation Methods and systems for estimating neural activation by stimulation using a stimulation system
AU2022406888A1 (en) 2021-12-09 2024-05-16 Boston Scientific Neuromodulation Corporation Methods and systems for monitoring or assessing movement disorders or other physiological parameters using a stimulation system
EP4415809B1 (en) 2021-12-10 2026-01-28 Boston Scientific Neuromodulation Corporation Systems and methods for generating and using response maps for electrical stimulation

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20070102648A1 (en) * 2005-01-13 2007-05-10 Celight, Inc. Method and system for nuclear substance revealing using muon detection
US7897925B2 (en) * 2007-01-04 2011-03-01 Celight, Inc. System and method for high Z material detection
US7908121B2 (en) * 2006-10-27 2011-03-15 Los Alamos National Security, Llc Determination of time zero from a charged particle detector
US7945105B1 (en) * 2008-04-07 2011-05-17 Decision Sciences International Corporation Automated target shape detection for vehicle muon tomography

Family Cites Families (20)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5732158A (en) 1994-11-23 1998-03-24 Tec-Masters, Inc. Fractal dimension analyzer and forecaster
US6169476B1 (en) 1997-02-18 2001-01-02 John Patrick Flanagan Early warning system for natural and manmade disasters
US7327913B2 (en) 2001-09-26 2008-02-05 Celight, Inc. Coherent optical detector and coherent communication system and method
US6930596B2 (en) 2002-07-19 2005-08-16 Ut-Battelle System for detection of hazardous events
US7483600B2 (en) 2003-07-02 2009-01-27 Celight, Inc. Integrated coherent optical detector
US8050351B2 (en) 2003-07-02 2011-11-01 Celight, Inc. Quadrature modulator with feedback control and optical communications system using the same
US7840144B2 (en) 2003-07-02 2010-11-23 Celight, Inc. Coherent optical transceiver and coherent communication system and method for satellite communications
US8064767B2 (en) 2003-09-22 2011-11-22 Celight, Inc. Optical orthogonal frequency division multiplexed communications with coherent detection
US7502118B2 (en) 2003-09-22 2009-03-10 Celight, Inc. High sensitivity coherent photothermal interferometric system and method for chemical detection
US7426035B2 (en) 2003-09-22 2008-09-16 Celight, Inc. System and method for chemical sensing using trace gas detection
US7119676B1 (en) 2003-10-09 2006-10-10 Innovative Wireless Technologies, Inc. Method and apparatus for multi-waveform wireless sensor network
US7148803B2 (en) 2003-10-24 2006-12-12 Symbol Technologies, Inc. Radio frequency identification (RFID) based sensor networks
US8929228B2 (en) 2004-07-01 2015-01-06 Honeywell International Inc. Latency controlled redundant routing
US7531791B2 (en) 2005-02-17 2009-05-12 Advanced Applied Physics Solutions, Inc. Geological tomography using cosmic rays
KR20070118226A (en) 2005-02-17 2007-12-14 트라이엄프,오퍼레이팅애즈어조인트벤쳐바이더거버너스 오브더유니버시티오브알버타더유니버시티오브브리티시콜롬비아 칼레톤유니버시티시몬프레이저유니버시티더유니버시티 오브토론토앤드더유니버시티오브빅토리아 Geometric X-ray Tomography Using Cosmic Rays
WO2008127442A2 (en) 2007-01-04 2008-10-23 Celight, Inc. High z material detection system and method
WO2008086507A1 (en) 2007-01-10 2008-07-17 Decision Sciences Corporation Information collecting and decision making via tiered information network systems
US8143575B2 (en) 2007-01-25 2012-03-27 Celight, Inc. Detection of high Z materials using reference database
US20080212970A1 (en) 2007-02-26 2008-09-04 Celight, Inc. Non-line of sight optical communications
US8288721B2 (en) * 2007-04-23 2012-10-16 Decision Sciences International Corporation Imaging and sensing based on muon tomography

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20070102648A1 (en) * 2005-01-13 2007-05-10 Celight, Inc. Method and system for nuclear substance revealing using muon detection
US7908121B2 (en) * 2006-10-27 2011-03-15 Los Alamos National Security, Llc Determination of time zero from a charged particle detector
US7897925B2 (en) * 2007-01-04 2011-03-01 Celight, Inc. System and method for high Z material detection
US7945105B1 (en) * 2008-04-07 2011-05-17 Decision Sciences International Corporation Automated target shape detection for vehicle muon tomography

Cited By (13)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US9851311B2 (en) 2013-04-29 2017-12-26 Decision Sciences International Corporation Muon detector array stations
WO2014179238A3 (en) * 2013-04-29 2015-02-12 Decision Sciences International Corporation Muon detector array stations
US20150241593A1 (en) * 2014-02-26 2015-08-27 Decision Sciences International Corporation Discrimination of low-atomic weight materials using scattering and stopping of cosmic-ray electrons and muons
US9915626B2 (en) * 2014-02-26 2018-03-13 Decision Sciences International Corporation Discrimination of low-atomic weight materials using scattering and stopping of cosmic-ray electrons and muons
WO2015154054A1 (en) * 2014-04-04 2015-10-08 Decision Sciences International Corporation Muon tomography imaging improvement using optimized limited angle data
US9639973B2 (en) * 2014-04-04 2017-05-02 Decision Sciences International Corporation Muon tomography imaging improvement using optimized limited angle data
US20150287237A1 (en) * 2014-04-04 2015-10-08 Decision Sciences International Corporation Muon tomography imaging improvement using optimized limited angle data
US10042079B2 (en) 2014-05-07 2018-08-07 Decision Sciences International Corporation Image-based object detection and feature extraction from a reconstructed charged particle image of a volume of interest
US9841530B2 (en) 2014-08-11 2017-12-12 Decision Sciences International Corporation Material discrimination using scattering and stopping of muons and electrons
US20160104290A1 (en) * 2014-10-08 2016-04-14 Decision Sciences International Corporation Image based object locator
WO2016057532A1 (en) * 2014-10-08 2016-04-14 Decision Sciences International Corporation Image based object locator
US10115199B2 (en) * 2014-10-08 2018-10-30 Decision Sciences International Corporation Image based object locator
US10459092B2 (en) * 2016-04-25 2019-10-29 Wagner Research Center for Physics of the Hungarian Academy of Science Muographic observation instrument

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