WO2007070080A2 - Method and apparatus of detecting an object - Google Patents

Method and apparatus of detecting an object Download PDF

Info

Publication number
WO2007070080A2
WO2007070080A2 PCT/US2006/016822 US2006016822W WO2007070080A2 WO 2007070080 A2 WO2007070080 A2 WO 2007070080A2 US 2006016822 W US2006016822 W US 2006016822W WO 2007070080 A2 WO2007070080 A2 WO 2007070080A2
Authority
WO
WIPO (PCT)
Prior art keywords
container
interferometer
further including
laser
sampling
Prior art date
Application number
PCT/US2006/016822
Other languages
French (fr)
Other versions
WO2007070080A3 (en
Inventor
Robert Kurt Brandt
Mark Stephen Williamsen
Original Assignee
Brandt Innovative Technologies, Inc.
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Brandt Innovative Technologies, Inc. filed Critical Brandt Innovative Technologies, Inc.
Priority to JP2008510131A priority Critical patent/JP5306810B2/en
Priority to US11/913,414 priority patent/US8151644B2/en
Priority to CA002606848A priority patent/CA2606848A1/en
Priority to EP06752084A priority patent/EP1883824A4/en
Publication of WO2007070080A2 publication Critical patent/WO2007070080A2/en
Publication of WO2007070080A3 publication Critical patent/WO2007070080A3/en
Priority to US13/443,335 priority patent/US8555725B2/en

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01HMEASUREMENT OF MECHANICAL VIBRATIONS OR ULTRASONIC, SONIC OR INFRASONIC WAVES
    • G01H9/00Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by using radiation-sensitive means, e.g. optical means
    • G01H9/008Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by using radiation-sensitive means, e.g. optical means by using ultrasonic waves
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01HMEASUREMENT OF MECHANICAL VIBRATIONS OR ULTRASONIC, SONIC OR INFRASONIC WAVES
    • G01H9/00Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by using radiation-sensitive means, e.g. optical means
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N29/00Investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves; Visualisation of the interior of objects by transmitting ultrasonic or sonic waves through the object
    • G01N29/04Analysing solids
    • G01N29/12Analysing solids by measuring frequency or resonance of acoustic waves
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N29/00Investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves; Visualisation of the interior of objects by transmitting ultrasonic or sonic waves through the object
    • G01N29/22Details, e.g. general constructional or apparatus details
    • G01N29/24Probes
    • G01N29/2418Probes using optoacoustic interaction with the material, e.g. laser radiation, photoacoustics
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N2291/00Indexing codes associated with group G01N29/00
    • G01N2291/01Indexing codes associated with the measuring variable
    • G01N2291/014Resonance or resonant frequency
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N2291/00Indexing codes associated with group G01N29/00
    • G01N2291/26Scanned objects
    • G01N2291/269Various geometry objects
    • G01N2291/2695Bottles, containers

Definitions

  • the present invention relates in general to the field of safety, security and process control. More particularly, the present invention relates to a method and apparatus for detecting potential harmful objects in a closed container, measuring critical-to-quality parameters in a container's contents for process control and identifying defects in the container itself.
  • the performance of the PSM interferometer was experimentally demonstrated in photorefractive sillenite crystals (Bi 12 Ti0 2 o) by Kamshilin et al.
  • the performance of the PSM interferometer was experimentally demonstrated in photorefractive GaP crystals by (Kobozev et al.)
  • the present invention is directed to an inspection system with a sensor.
  • This system has the capability for stand-off, non-invasive, continuous, real-time, non- radiological, non-consumable, eye-safe inspection of closed containers made of a wide of materials that include ferrous metals, non-ferrous metals, glass, plastics and organic material. Each function is described more fully below:
  • Stand-off means the sensor preferably operates in close proximity (millimeters) or at a long distance (kilometers) with certain adjustments to the basic design.
  • the sensor preferably uses laser-based ultrasound generation and detection which has been shown to be a viable stand-off detection technology.
  • Non-invasive means the sensor preferably determines material properties of the contents of a container closed to material flow.
  • the sensor preferably uses laser-based ultrasound generation and detection which has been shown to be a viable non-invasive detection technology.
  • the senor preferably takes many consecutive measurements without intervention.
  • the sensor has a repetition rate between 1 and 10 Hz and can collect data continually from the sample as long as the sensor is aimed at the container.
  • Real-time means the results preferably are available within seconds or fractions of seconds.
  • the sensor preferably has a repetition rate between 1 and 10 Hz and can collect data continually from the sample as long as the sensor is aimed at the container.
  • Non-radiological means the sensor preferably does not require the use of materials that undergo radioactive decay to produce an energy source for the sensor.
  • the sensor preferably uses laser radiation at 1.5 um which is considered by the literature as the "eye-safe" region of the electromagnetic spectrum.
  • Non-consumable means the sensor preferably does not require chemical or biological ingredients that are consumed by the activity of sensing.
  • the entire sensor preferably consists of hardware and software, as described in the parts lists and associated figures, that does not require use of any disposable test kits, ingredients, or other consumable media.
  • Eye-safe means the sensor preferably does not emit radiation that is destructive to the human eye.
  • the sensor preferably uses laser radiation at 1.5 um which is considered by the literature as the "eye-safe" region of the electromagnetic spectrum.
  • Another aspect of the invention is to provide an apparatus that is ruggedized and reliable, thereby decreasing down time and operating costs.
  • Still another aspect of the invention is to provide an apparatus that has one or more of the characteristics discussed above but which is relatively simple to manufacture, assemble, and use using a minimum of equipment, time and resources.
  • subsystems would be purchased from other manufacturers and final assembly and integration of these subsystems would be done at a central location.
  • Still another aspect of the invention is to perform stand-off, non-invasive level inspection of beverage cans and bottles without the use of radiological materials.
  • Yet another aspect of the invention is to perform stand-off, non-invasive inspection of drums, pipes, warheads, bombs, and other closed containers for chemical and/or biological weapons.
  • Closed containers for chemical and/or biological weapons are generally made of either ferrous, non-ferrous, polymer or glass containers.
  • Another aspect of the invention is to detect defects during the creation of laminate materials.
  • Still another aspect of the invention is to detect contraband in tires of vehicles moving through border inspection stations. Another aspect of the invention is to verify contents in containers shipped into the US borders. Still another aspect of the invention is to identify flow characteristics in pipelines which is currently being done by contact-based ultrasound sensors (GE for example). Another aspect of the invention is to identify defects in pipelines.
  • GE contact-based ultrasound sensors
  • Yet another aspect is to provide quality assurance of canned and bottled food products using a continuous, real-time, noninvasive sensor.
  • Another aspect of the invention is to detect a small amount of biological material, e.g., a few drops of biological material (dairy fat, blood) in a closed container of water.
  • Still another aspect of the invention is to measure mixtures of materials inside a closed container. Another aspect of the invention is to provide a method that can be used to satisfy the above aspects of the invention. Still another aspect of the invention is to provide a method that is predictable and reproducible, thereby decreasing variance and operating costs.
  • Another aspect of the invention is to provide a method that has one or more of the characteristics discussed above but which is which is relatively simple to setup and operate using relatively low skilled workers.
  • Fig.l shows one embodiment of the present invention with a transmitted material wave and reflected material wave as they probe the material properties of the contents of the container;
  • Fig. 2 shows one embodiment of the present invention with a transmitted material wave and reflected material wave probing the material properties a contaminant of the contents of the container;
  • Fig. 3 shows one embodiment of the present invention with a transmitted material wave and reflected material wave as they probe the material defect in the container;
  • Fig. 4 shows one embodiment of the present invention with a transmitted material wave being detected on the opposite side of the container
  • Fig. 5 shows one embodiment of a hand-held, mobile package of the present invention
  • Fig. 6 shows a schematic of one system configuration of the present invention
  • Fig. 7 shows a schematic of one optical subsystem of the present invention.
  • the inventive system of the present invention includes an optical device that may be mounted on an optical "breadboard.”
  • the breadboard may be mounted on a rail to enable the distance between a sensor of the system and a target container to be varied in a controllable way.
  • the inventive system of the present invention includes all optics, electronics, and software in a single hand-held unit, see e.g., Fig. 5.
  • the preferred optical device includes an excitation laser that will be a Q-switched Nd:Yag laser pumped with a laser diode.
  • the entire laser will be preferably housed in a TO-3 case; have a Wavelength: 1.550 ⁇ m, Pulse Energy: 100 ⁇ J, Pulse Width:2 ns, Peak Power: 50 Kw, Repetition Rate: SS to 10 Hz and the supplied driver is designed to work from a 3V battery.
  • the excitation beam is preferably launched through an optional pattern generator and is directed collinear with probe and detection beams to minimize angle and distance-dependant focusing effects.
  • a filter is preferably inserted to prevent excitation beam energy -from reaching the detector. The high impulse energy and low continuous power make this embodiment ideal for mobile applications
  • a probe laser preferably consists of a CW Laser Diode (1550 nm, 13OmW).
  • the probe laser beam preferably is launched through an optional pattern generator into a beam splitter.
  • the beam splitter directs a first part of the beam towards the target (probe or transmitted material wave beam) and a second part of the beam toward a photorefractive crystal of CdTe or similar (reference beam).
  • Two-wave mixing takes place in the photorefractive crystal and the resulting signal is detected by a high-speed differential detector consisting of a polarizing beam splitter and two photodiodes.
  • a high peak power Q-switched solid-state laser is used for the excitation source.
  • this traditional approach involves high-energy optical pulse irradiation that may lead to surface damage, especially in carbon or glass fiber composites. Therefore, in another embodiment, the simple projection system is substituted with a pattern- based projection system. This enables excitation without damage but requires coded temporal signals. Arrays of patterns generated by semiconductor laser sources may also produce very broadband acoustic signals, both temporally and spatially.
  • the probe laser is a low-cost near infrared laser diode (1550 nm 130 mW).
  • the optical arrangement may also have a provision for holographic pattern generation to allow for decoding of encoded excitation laser signals.
  • laser diodes in the region of 1550 nm allows the entire system to be eye safe.
  • the system could be created at other wavelengths of light using optical component appropriate for the selected wavelength of light.
  • the system could be replaced by other radiation sources such as microwaves.
  • Semiconductor crystals are known to possess a high mobility of charge carriers resulting in fast formation of the space-charge field. Others including Delaye 1995, Ing et. al. 1996, Campagne et. al. 2001, Iida et. al. 2003, Blouin et. al. 1994, Golovan et. al. 2004, Kobozev et. al. 2001 and Kuroda et. al. 1990 have also demonstrated photorefractive-based interferometers based on semiconductor crystals.
  • the GaP crystal is a representative of a wide-band gap semiconductor, and exhibits the photorefractive effect in red and near-infrared regions of the optical spectrum.
  • Kobozev et al. carried out experiments with a GaP crystal cut in the form of a parallelepiped with edges parallel to the [UO], [001] and [110] crystallographic axes.
  • the dimensions of the sample were 3.97, 5.8 and 6.52 mm, respectively.
  • silver electrodes were evaporated on the (110) faces of the crystal.
  • the light beams propagated at small angles to the [UO] crystallographic axis.
  • the semi-insulating GaP single crystal (point symmetry group 43m) was grown at Sumitomo Metal Mining Co., Japan.
  • Shcherbin et al. and others have shown a CdTe crystal, which exhibits the largest electro-optic constant among all known semiconductors, to be suitable for photorefractive applications in the near infrared.
  • the data-acquisition system of the present inventions preferably includes a signal processor.
  • the stimulus and response signals are managed with a combination of analog and digital strategies.
  • the focus is in digital technologies, which may be reconfigured for different applications, without too much confusion.
  • Amplification is preferably done with an off the shelf pulser/receiver that has noise referred to the input of about 100 ⁇ V (pk-pk). This is within the dynamic range of 16 bit A/D converters (65536 counts from 0 to 5 Vdc gives a resolution of 76 ⁇ V). In this case, signal conditioning consists of impedance conversion/matching and band-pass filtering with no gain required. If 12 bit converters are used, then some gain will be required, as 4096 counts from 0 to 5 Vdc gives a resolution of 1.2 mV. As such, it is desirable to have computer control of the gain.
  • sample rate a "digital radio" is used to maximum gain flexibility, hi other words, a sensor connected directly to an A/D converter.
  • sample components up to 10 MHz, not less than 20 M samples/second (preferably more) are used.
  • the limiting factor is on the anti-aliasing filter provided. Actual bandwidth may be end at the knee of the filter skirt when the bottom of the skirt reaches the noise floor at 10 MHz.
  • a 96 dB/8— low pass filter provides us a 5 MHz bandwidth.
  • off the shelf converters may be used having typical binary outputs with either 12 or 16 bit resolution, hi some instances, 20 or even 24 bit converters may be used.
  • signal levels and attenuation characteristics are known, then dynamic range becomes less important.
  • sample thickness and ultrasound attenuation vary greatly, dynamic range is needed to accommodate it. Further, this is less important if a computer controls preamp gain.
  • DSP Digital Signal Processing
  • samples may be captured at that rate and then analyzed off-line at a much slower rate. And, since the repetition rate may be arbitrarily slow, off-line processing may be accomplished at this slower pace. This avoids the need to have DSP specific hardware for computation.
  • data may be captured from the digital oscilloscope, and stored to a PC. The system may then apply signal processing algorithms to the data.
  • the inventive system 1 is generally constructed in accordance with what is shown in Figs. 1-7. It may be employed in variety of environments including airports, military bases, manufacturing sites, transportation centers, construction sites, and border patrol checkpoints.
  • the construction of units typically employing the various components of this invention is well known to those skilled in the art and therefore a detailed description thereof is not necessary to fully understand the present invention
  • one embodiment of the invention preferably contains several components.
  • the system 1 has a laser source Ia connected to excitation optics 2.
  • the system creates various waves which are directed to container vessel 3 and vessel surface 4.
  • the waves including incident excitation wave 5, transmitted material wave 1, reflected material wave, incident probe wave 11, and reflected probe wave 12 are all preferable emitted from probe laser 14.
  • the waves of the laser Ia are primarily directed at the vessel bulk 6 and are used to make a determination of the container contents 9.
  • Collection optics 13 preferably work in conjunction with probe optics 15.
  • the data acquisition systems 16 collect the information received by the reflected material wave 10.
  • the inventive system 1 preferably also has control electronics 17, digital signal processing systems 18, a microprocessor 19 and a database system 20.
  • a display 21 may also be provided.
  • the object of interest 23 is probed by the various waves of the system 1 to determine the content of the container vessel 3.
  • the below graphs and tables show the results of some of the tests using one embodiment of the present invention.
  • Graph 1 Shows the measuring the phase transition in Phenolic Frictional Material Manufacture.
  • Table 1 The above shows the speed of sound for various materials (longitudinal mode propagation).
  • the transition time for a wideband ultrasound pulse can easily be measured and along with the physical dimension of the container a speed of sound may be calculated.
  • the speed of sound varies significantly, even in water, as the chemical composition is varied. If the geometry is known then the speed of sound becomes an easy way to differentiate two materials.
  • Graph 4 Amplitude of measured signal for different frequencies as a function of the number fat drops added to a container of water. We can detect about a dozen drops of fat in 355 ml of water in an aluminum container.
  • Graph 5 Comparison of Time Series Data, 3 rd Order Cumulant data and Bispectra data. Scale factors (Cumulant x-axis and y-axis are both -102.4 uS to + 102.4 uS each pixel is 0.8 us 256 points) (Bispectra- 312.5 kHz to + 312.5 kHz each point is 4.88 kHz 128 points) (Time series data 20 MSS, 6500 samples, 325 uS, ).
  • Table 2 Measured Speed of sound using laser-based ultrasound on a number of different containers and contents.
  • the analysis of the signal of the system 1 is preferably based on the following:
  • Timing of the return pulse is used to calculate speed of sound of the material in the container.
  • Spectral analysis is used to determine the frequency and attenuation response of the container and contents. This technique is used to identify various constituents or ingredients in the preparation of food products.
  • Vx in the liquid form preferably has a speed of sound similar to water and the molecular makeup of the material is likely to result in a frequency-dependent spectra that is different than water.
  • Fluctuation Enhanced Analysis [Kish, Mendel] is preferably used to investigate the non- Gaussian noise characteristics of the signals that may translate into useful information.
  • Smulko and Kish have identified a methodology that suggests the stochastic component of a chemical sensor signal contains valuable information that can be visualized not only by spectral analysis but also by methods of higher-order statistics (HOS).
  • HOS higher-order statistics
  • the analysis of HOS enables the extraction of non-conventional features that lead to significant improvements in selectivity and sensitivity.
  • Each bispectrum is plotted in gray scale pixel values, as the sum of the sine and cosine Fourier components.
  • Fig. 6 shows an example system configuration.
  • the device under test or object (71) is, for example, a 55 gal. Drum or container.
  • Beam steering optics (72) is, for example, a telephoto lens.
  • An excitation beam combiner (73) is preferably a beam splitter.
  • a probe beam combiner (74) is, for example, a beam splitter.
  • a preferred adaptive interferometer (75) is a photorefractive crystal, mirror, and polarizer.
  • a detector assembly (76) is, for example, a beam splitter differential photo-detector combination.
  • An excitation laser assembly (77) includes preferably a Q-switched YAG laser while a probe laser assembly (78) includes, for example, a diode laser.
  • a preferred excitation beam driver (79) is a current controller pulsing circuit.
  • a probe laser driver (80) is, for example, a constant current supply with diode feedback.
  • Drive electronics for adaptive interferometer (81) preferably include a bias supply for photorefractive crystal.
  • a microprocessor assembly (83) is a PC 104 minicomputer module and power management (84) includes a power supply battery charging module.
  • Thermal management (85) includes, for example, a thermoelectric cooler and controller.
  • User interface (86) is, for example, a LCD touch screen module.
  • Communications interface (87) is, for example, a Wi-Fi interface module, Ethernet interface module, USB interface module, ZigBee interface module.
  • Optical Subsystem (88) (see, e.g., Fig. 7).
  • Business intelligence subsystem (89) is, for example, an application server, data base server, application software and database software and data to provide list parameters for contents of shipping containers and software integration to software manifests of shipping container contents.
  • the container or device under test (201) is, for example, a 5/55/65 gal. drum.
  • a telephoto lens (202) is also provided.
  • the excitation laser (203), in an example 1 is a diode- pumped solid state laser housed in TO-3 case having a wavelength: 1.54 ⁇ m, Pulse Energy: 100 ⁇ j, Pulse Width:2 ns, Peak Power: 50 Kw, Repetition Rate: SS to 10 Hz.
  • a diode pumped solid-state laser having a Wavelength: 1.54 ⁇ m, Pulse Energy: 4 mJ, Pulse Width:7 ns, Repetition Rate: SS to 10 Hz.
  • the probe laser (204) is a fabry Perot laser cavity having a single transverse mode of 13OmW in wavelength range 1550 nm. InGaAs MQW. In another example, a single transverse mode of 44mW is provided in wavelength range 1550 irm.InGaAsP/InP SQW.
  • the polarizing beam splitter (206) is preferably a Narrow Band: BK7 grade A optical glass, Broadband: SF5 optical glass with a Dimension Tolerance ⁇ 0.2mm, Extinction Ratio >100:l, Flatness 1/4 @ 632.8 nm per 25mm, Surface Quality 60/40 scratches and dig, Principal Transmittance Tp>95% and Ts ⁇ l%, Principal Reflectance Rs>99% and Rp ⁇ 5%, Beam Deviation ⁇ 3 arc minutes.
  • the polarizer (207) is preferably a linear NIR polarizer nominal 50% at 1550. Alternatively, the polarizer is a linear polarizer having an extinction ratio better than 10,000:1, High transmission, Wide acceptance angle, and Low wavefront distortion.
  • the retardation plate (208) preferably has dimensions 5mm x 5mm, Material: Crystal Quartz, Substrate: BK-7, 2mm thick, Bonding: Cement, Wavelength: 1550nm, Coating: AR ⁇ 0.5%.
  • the plate is a Crystal quartz, having Dimension Tolerance +0.0, -0.2mm, Wavefront Distortion ⁇ l/8@632.8, Retardation Tolerance ⁇ l/500, Parallelism ⁇ 1 arc second, Clear aperture >80%, Surface Quality 20/10 scratches & dig, Coating RO.2% on both surfaces at central wavelength.
  • the photorefractive crystal (209), in example 1, is a CdTe, Ge crystal germainium-doped to give a dark conductivity of 10 "9 ⁇ cm "1 with dimensions 4 mm x 5 mm x 10 mm cut along [112], [111], and [HO] directions respectively having faces parallel to [110] polished, faces parallel to [111] silvered.
  • a CdTe:V, crystal vanadium-doped is provided with dimensions 3 mm x 3 mm x 5 mm cut along [112], [111], and [UO] directions respectively having the faces parallel to [110] polished, faces parallel to [111] silvered.
  • a GaAs crystal with no doping with dimensions 5 mm x 5 mm x 5 mm cut along [001], [110], and [110] directions respectively is provided that also has the faces parallel to [UO] polished.
  • the material is BK7 Grade A Optical Glass, and the Dimension Tolerance is + 0.0, - 0.2mm, Thickness Tolerance is ⁇ 0.2mm, Clear Aperture is > 80%, Parallelism is ⁇ 1 arc minute, Surface Quality is 60/40 (S/D), and Bevel(Chamfer) is 0.15 ⁇ 0.35mmx45° face width x 45° ⁇ 15° ).
  • the photodiode (211), in an example 1, is InGaAs Photodiode with a 15 MHz Bandwidth and a 1200-2600nm, 01mm Active Area, hi an example 2, it is an InGaAs Photodiode with a 1 GHz Bandwidth, and al000-1600nm, 75 urn Active Area.
  • the individual components need not be formed in the disclosed shapes, or assembled in the disclosed configuration, but could be provided in virtually any shape, and assembled in virtually any configuration.
  • the components are described herein as physically separate modules, it will be manifest that these may be integrated into the apparatus with which it is associated.
  • all the disclosed features of each disclosed embodiment can be combined with, or substituted for, the disclosed features of every other disclosed embodiment except where such features are mutually exclusive.

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • General Health & Medical Sciences (AREA)
  • Immunology (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • Pathology (AREA)
  • Health & Medical Sciences (AREA)
  • Optics & Photonics (AREA)
  • Acoustics & Sound (AREA)
  • Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)
  • Geophysics And Detection Of Objects (AREA)
  • Optical Radar Systems And Details Thereof (AREA)

Abstract

A system for stand-off, continuous, real-time, non-invasive, non-radiological, eye-safe, non-consumable characterization of an object (3) is disclosed that comprises in combination a pulsed laser emitter (2) for directing energy at the surface of the object (3), wherein ultrasonic wave (7, 10) is generated within the object to be characterized, and a remote means (13) of measuring the vibrational excitation in the object (3), whereby the object is remotely characterized.

Description

METHOD AND APPARATUS OF DETECTING AN OBJECT
STATEMENT AS TO RIGHTS TO INVENTION(S) MADE UNDER FEDERALLY-SPONSORED RESEARCH AND DEVELOPMENT
The U.S. Government has provided funding for the background research for this invention through an award by the Department of Defense
CROSS-REFERENCE TO RELATED APPLICATIONS
This application claims priority from U.S. Provisional Patent Application Serial No. 60/677,751, filed on May 4, 2005, the entity of which is expressly incorporated by reference herein in its entirety.
BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates in general to the field of safety, security and process control. More particularly, the present invention relates to a method and apparatus for detecting potential harmful objects in a closed container, measuring critical-to-quality parameters in a container's contents for process control and identifying defects in the container itself.
2. Discussion of the Related Art
As is known to those skilled in the art, the detection of potential harmful materials in a closed container continues to be a problem. This is particularly true where X-Ray radiation cannot be employed for safety or health reason, lack of sensitivity or specificity. Other techniques such as contact-based ultrasound, optical spectroscopy, gas chromatography, mass spectroscopy, bio-assay etc. also lack the ability to perform stand-off, non-invasive, continuous, real-time, non-consumable inspection of closed containers that include plastic, glass, ferrous and non-ferrous metals.
Below several publications are referenced within parentheses. The disclosures of all these publications in their entireties are hereby expressly incorporated by reference into the present application for at least the puiposes of indicating the background of the present invention and illustrating the state of the art. Various authors have reported schemes for interferometer, e.g., KamsMlin et al. introduces an interferometric technique for linear detection of small ultrasonic out-of-plane vibrations of a rough surface. (Kamshilin et al.) This technique is based on the polarization self-modulation (PSM) effect in the photorefractive crystals under an applied AC field that excludes the field screening. The performance of the PSM interferometer was experimentally demonstrated in photorefractive sillenite crystals (Bi12Ti02o) by Kamshilin et al. The performance of the PSM interferometer was experimentally demonstrated in photorefractive GaP crystals by (Kobozev et al.)
The below-referenced U.S. patents disclose embodiments that were at least in-part satisfactory for the purposes for which they were intended. The disclosures of all the below- referenced prior United States patents are hereby expressly incorporated by reference into this present application for purposes including, but not limited to, indicating the background of the present invention and illustrating the state of the art:
U.S. Pat. No. 4,455,268 discloses a "Control System for Processing Composite
Materials",
U.S. Pat. No. 4,758,803 discloses a "Marginal Oscillator for Acoustic Monitoring of Curing of Plastics",
U.S. Pat. No. 4,862,384 discloses a "Method of Using Dynamic Viscosity Using
Acoustic Transducer",
U.S. Pat. No. 5,505,090 discloses a "Method and Apparatus for Non-Destructive
Inspection of Composite Materials and Semi-Monocoque Structures",
U.S. Pat. No. 5,533,339 discloses a "Method and Apparatus for Non-Destructive
Measurement of Elastic Properties of Composite Materials", and
U.S. Pat. No. 6,029,520 discloses an "Ultrasonic Monitoring of Resin in a Press for the Production of Particle Board and Similar Materials."
However, what is needed is a cost-effective, accurate way to make measurements of things, e.g., containers, and fulfill one or more of the following inspection conditions: portable, stand-off, non-invasive, continuous, real-time, non-radiological, and non-consumable. SUMMARY AND OBJECTS OF THE INVENTION
By way of summary, the present invention is directed to an inspection system with a sensor. This system has the capability for stand-off, non-invasive, continuous, real-time, non- radiological, non-consumable, eye-safe inspection of closed containers made of a wide of materials that include ferrous metals, non-ferrous metals, glass, plastics and organic material. Each function is described more fully below:
Stand-off means the sensor preferably operates in close proximity (millimeters) or at a long distance (kilometers) with certain adjustments to the basic design. Here the sensor preferably uses laser-based ultrasound generation and detection which has been shown to be a viable stand-off detection technology.
Non-invasive means the sensor preferably determines material properties of the contents of a container closed to material flow. Here the sensor preferably uses laser-based ultrasound generation and detection which has been shown to be a viable non-invasive detection technology.
Continuous means the sensor preferably takes many consecutive measurements without intervention. Here the sensor has a repetition rate between 1 and 10 Hz and can collect data continually from the sample as long as the sensor is aimed at the container.
Real-time means the results preferably are available within seconds or fractions of seconds. Here the sensor preferably has a repetition rate between 1 and 10 Hz and can collect data continually from the sample as long as the sensor is aimed at the container.
Non-radiological means the sensor preferably does not require the use of materials that undergo radioactive decay to produce an energy source for the sensor. Here the sensor preferably uses laser radiation at 1.5 um which is considered by the literature as the "eye-safe" region of the electromagnetic spectrum.
Non-consumable means the sensor preferably does not require chemical or biological ingredients that are consumed by the activity of sensing. Here the entire sensor preferably consists of hardware and software, as described in the parts lists and associated figures, that does not require use of any disposable test kits, ingredients, or other consumable media.
Eye-safe means the sensor preferably does not emit radiation that is destructive to the human eye. Here the sensor preferably uses laser radiation at 1.5 um which is considered by the literature as the "eye-safe" region of the electromagnetic spectrum. Another aspect of the invention is to provide an apparatus that is ruggedized and reliable, thereby decreasing down time and operating costs.
Still another aspect of the invention is to provide an apparatus that has one or more of the characteristics discussed above but which is relatively simple to manufacture, assemble, and use using a minimum of equipment, time and resources. In one such a manufacturing process, subsystems would be purchased from other manufacturers and final assembly and integration of these subsystems would be done at a central location.
Another aspect of the invention is to provide a non-invasive process sensor to monitor the phase transition of the cross linking process that occurs in manufacture of polymer products. Yet another aspect of the invention is to perform a stand-off, non-invasive inspection of returnable beverage kegs for frozen beverage or non-nominal material contents.
Still another aspect of the invention is to perform stand-off, non-invasive level inspection of beverage cans and bottles without the use of radiological materials.
Yet another aspect of the invention is to perform stand-off, non-invasive inspection of drums, pipes, warheads, bombs, and other closed containers for chemical and/or biological weapons. Note: Closed containers for chemical and/or biological weapons are generally made of either ferrous, non-ferrous, polymer or glass containers.
Another aspect of the invention is to detect defects during the creation of laminate materials.
Still another aspect of the invention is to detect contraband in tires of vehicles moving through border inspection stations. Another aspect of the invention is to verify contents in containers shipped into the US borders. Still another aspect of the invention is to identify flow characteristics in pipelines which is currently being done by contact-based ultrasound sensors (GE for example). Another aspect of the invention is to identify defects in pipelines.
Yet another aspect is to provide quality assurance of canned and bottled food products using a continuous, real-time, noninvasive sensor. Another aspect of the invention is to detect a small amount of biological material, e.g., a few drops of biological material (dairy fat, blood) in a closed container of water.
Still another aspect of the invention is to measure mixtures of materials inside a closed container. Another aspect of the invention is to provide a method that can be used to satisfy the above aspects of the invention. Still another aspect of the invention is to provide a method that is predictable and reproducible, thereby decreasing variance and operating costs.
Another aspect of the invention is to provide a method that has one or more of the characteristics discussed above but which is which is relatively simple to setup and operate using relatively low skilled workers.
These, and other aspects and objects of the present invention will be better appreciated and understood when considered in conjunction with the following description and the accompanying drawings. It should be understood, however, that the following description, while indicating preferred embodiments of the present invention, is given by way of illustration and not of limitation. Many changes and modifications may be made within the scope of the present invention without departing from the spirit thereof, and the invention includes all such modifications.
BRIEF DESCRIPTION OF THE DRAWINGS
A clear conception of the advantages and features constituting the present invention, and of the construction and operation of typical mechanisms provided with the present invention, will become more readily apparent by referring to the exemplary, and therefore non-limiting, embodiments illustrated in the drawings accompanying and forming a part of this specification, wherein like reference numerals designate the same elements in the several views, and in which Figs. 1-7 illustrate various aspects of the present invention. Specifically,
Fig.l shows one embodiment of the present invention with a transmitted material wave and reflected material wave as they probe the material properties of the contents of the container;
Fig. 2 shows one embodiment of the present invention with a transmitted material wave and reflected material wave probing the material properties a contaminant of the contents of the container;
Fig. 3 shows one embodiment of the present invention with a transmitted material wave and reflected material wave as they probe the material defect in the container;
Fig. 4 shows one embodiment of the present invention with a transmitted material wave being detected on the opposite side of the container;
Fig. 5 shows one embodiment of a hand-held, mobile package of the present invention;
Fig. 6 shows a schematic of one system configuration of the present invention; and Fig. 7 shows a schematic of one optical subsystem of the present invention.
In describing the preferred embodiment of the invention that is illustrated in the drawings, specific terminology will be resorted to for the sake of clarity. However, it is not intended that the invention be limited to the specific terms so selected and it is to be understood that each specific term includes all technical equivalents, which operate in a similar manner to accomplish a similar purpose. For example, the word connected or terms similar thereto are often used. They are not limited to direct connection but include connection through other elements where such connection is recognized as being equivalent by those skilled in the art.
DESCRIPTION OF PREFERRED EMBODIMENTS
The present invention and the various features and advantageous details thereof are explained more fully with reference to the non-limiting embodiments described in detail in the following description. 1. System Overview
In one embodiment, the inventive system of the present invention includes an optical device that may be mounted on an optical "breadboard." The breadboard may be mounted on a rail to enable the distance between a sensor of the system and a target container to be varied in a controllable way.
In another embodiment the inventive system of the present invention includes all optics, electronics, and software in a single hand-held unit, see e.g., Fig. 5.
The preferred optical device includes an excitation laser that will be a Q-switched Nd:Yag laser pumped with a laser diode. The entire laser will be preferably housed in a TO-3 case; have a Wavelength: 1.550 μm, Pulse Energy: 100 μJ, Pulse Width:2 ns, Peak Power: 50 Kw, Repetition Rate: SS to 10 Hz and the supplied driver is designed to work from a 3V battery. The excitation beam is preferably launched through an optional pattern generator and is directed collinear with probe and detection beams to minimize angle and distance-dependant focusing effects. A filter is preferably inserted to prevent excitation beam energy -from reaching the detector. The high impulse energy and low continuous power make this embodiment ideal for mobile applications
A probe laser preferably consists of a CW Laser Diode (1550 nm, 13OmW). The probe laser beam preferably is launched through an optional pattern generator into a beam splitter. The beam splitter directs a first part of the beam towards the target (probe or transmitted material wave beam) and a second part of the beam toward a photorefractive crystal of CdTe or similar (reference beam). Two-wave mixing takes place in the photorefractive crystal and the resulting signal is detected by a high-speed differential detector consisting of a polarizing beam splitter and two photodiodes.
As mentioned, in one embodiment a high peak power Q-switched solid-state laser is used for the excitation source. However, this traditional approach involves high-energy optical pulse irradiation that may lead to surface damage, especially in carbon or glass fiber composites. Therefore, in another embodiment, the simple projection system is substituted with a pattern- based projection system. This enables excitation without damage but requires coded temporal signals. Arrays of patterns generated by semiconductor laser sources may also produce very broadband acoustic signals, both temporally and spatially.
In one preferred embodiment, the probe laser is a low-cost near infrared laser diode (1550 nm 130 mW). The optical arrangement may also have a provision for holographic pattern generation to allow for decoding of encoded excitation laser signals.
The use of laser diodes in the region of 1550 nm allows the entire system to be eye safe. The system could be created at other wavelengths of light using optical component appropriate for the selected wavelength of light. Of course, the system could be replaced by other radiation sources such as microwaves.
Semiconductor crystals are known to possess a high mobility of charge carriers resulting in fast formation of the space-charge field. Others including Delaye 1995, Ing et. al. 1996, Campagne et. al. 2001, Iida et. al. 2003, Blouin et. al. 1994, Golovan et. al. 2004, Kobozev et. al. 2001 and Kuroda et. al. 1990 have also demonstrated photorefractive-based interferometers based on semiconductor crystals. The GaP crystal is a representative of a wide-band gap semiconductor, and exhibits the photorefractive effect in red and near-infrared regions of the optical spectrum. In particular, two-wave mixing at red light (wavelength of 633 nm) was first observed in the GaP crystal by Kuroda et al. It was shown that the response time of the space- charge-field formation in the GaP crystal is about 5 ms at a light intensity of 100 mW cm"2. Linear sensing of speckle-pattern displacements using the PSM effect was demonstrated in a GaP crystal at the same wavelength. For practical implementation, the material has to show some potential in the near infrared because of the availability of low-cost laser diodes in this spectral region. This has been demonstrated by Kobozev et al. who has reported observations of fast response time of space-charge-field formation obtained in the photorefractive GaP crystal in the near infrared (1=807 nm). By using the PSM interferometer for the detection of small out-of- plane vibrations, Kobozev et al. found that a response time of a few milliseconds can be achieved with commercially available laser diodes.
Kobozev et al. carried out experiments with a GaP crystal cut in the form of a parallelepiped with edges parallel to the [UO], [001] and [110] crystallographic axes. The dimensions of the sample were 3.97, 5.8 and 6.52 mm, respectively. To apply external voltage, silver electrodes were evaporated on the (110) faces of the crystal. The light beams propagated at small angles to the [UO] crystallographic axis. The semi-insulating GaP single crystal (point symmetry group 43m) was grown at Sumitomo Metal Mining Co., Japan.
Kobozev et al. pointed out that the above-described laser diode had a complicated beam intensity profile, which was far from the Gaussian distribution. Nevertheless, this did not limit the performance of the PSM interferometer. Despite large losses of the scattered light, the high intensity of the reference beam provides a fast response.
Shcherbin et al. and others (Bardeleben et.al., Jarasiunas et. al.) have shown a CdTe crystal, which exhibits the largest electro-optic constant among all known semiconductors, to be suitable for photorefractive applications in the near infrared.
The data-acquisition system of the present inventions preferably includes a signal processor. The stimulus and response signals are managed with a combination of analog and digital strategies. The focus is in digital technologies, which may be reconfigured for different applications, without too much confusion.
Amplification is preferably done with an off the shelf pulser/receiver that has noise referred to the input of about 100 μV (pk-pk). This is within the dynamic range of 16 bit A/D converters (65536 counts from 0 to 5 Vdc gives a resolution of 76 μV). In this case, signal conditioning consists of impedance conversion/matching and band-pass filtering with no gain required. If 12 bit converters are used, then some gain will be required, as 4096 counts from 0 to 5 Vdc gives a resolution of 1.2 mV. As such, it is desirable to have computer control of the gain.
The three factors affecting A/D conversion are: sample rate, dynamic range, and memory depth. For sample rate, a "digital radio" is used to maximum gain flexibility, hi other words, a sensor connected directly to an A/D converter. To sample components up to 10 MHz, not less than 20 M samples/second (preferably more) are used. The limiting factor is on the anti-aliasing filter provided. Actual bandwidth may be end at the knee of the filter skirt when the bottom of the skirt reaches the noise floor at 10 MHz. A 96 dB/8— low pass filter provides us a 5 MHz bandwidth.
For dynamic range, off the shelf converters may be used having typical binary outputs with either 12 or 16 bit resolution, hi some instances, 20 or even 24 bit converters may be used. Preferably, if the signal levels and attenuation characteristics are known, then dynamic range becomes less important. On the other hand, if sample thickness and ultrasound attenuation vary greatly, dynamic range is needed to accommodate it. Further, this is less important if a computer controls preamp gain.
For memory depth, there is need to accommodate several megabytes of sample depth particularly in the design of a commercial system. An adaptive system that first seeks the return signal and then dynamically windows the process to minimize sample depth is desired.
Digital Signal Processing (DSP) done in real-time DSP at 20 Msamp/sec. Is processor sensitive. However, samples may be captured at that rate and then analyzed off-line at a much slower rate. And, since the repetition rate may be arbitrarily slow, off-line processing may be accomplished at this slower pace. This avoids the need to have DSP specific hardware for computation. In one embodiment, data may be captured from the digital oscilloscope, and stored to a PC. The system may then apply signal processing algorithms to the data.
2. Detailed Description of Preferred Embodiments
The inventive system 1 is generally constructed in accordance with what is shown in Figs. 1-7. It may be employed in variety of environments including airports, military bases, manufacturing sites, transportation centers, construction sites, and border patrol checkpoints. The construction of units typically employing the various components of this invention is well known to those skilled in the art and therefore a detailed description thereof is not necessary to fully understand the present invention
Specific embodiments of the present invention will now be further described by the following, non-limiting examples which will serve to illustrate various features of significance. The examples are intended merely. to facilitate an understanding of ways in which the present invention may be practiced and to further enable those of skill in the art to practice the present invention. Accordingly, the examples should not be construed as limiting the scope of the present invention. As shown in Figs.1-4, one embodiment of the invention preferably contains several components. The system 1 has a laser source Ia connected to excitation optics 2. The system creates various waves which are directed to container vessel 3 and vessel surface 4. The waves including incident excitation wave 5, transmitted material wave 1, reflected material wave, incident probe wave 11, and reflected probe wave 12 are all preferable emitted from probe laser 14. The waves of the laser Ia are primarily directed at the vessel bulk 6 and are used to make a determination of the container contents 9. Collection optics 13 preferably work in conjunction with probe optics 15. The data acquisition systems 16 collect the information received by the reflected material wave 10. The inventive system 1 preferably also has control electronics 17, digital signal processing systems 18, a microprocessor 19 and a database system 20. A display 21 may also be provided. The object of interest 23 is probed by the various waves of the system 1 to determine the content of the container vessel 3. The below graphs and tables show the results of some of the tests using one embodiment of the present invention.
Ultrasound Amplitude 196 C under pressure of about 10
Figure imgf000011_0001
Time (minutes)
Graph 1 : Shows the measuring the phase transition in Phenolic Frictional Material Manufacture.
Figure imgf000012_0001
Table 1: The above shows the speed of sound for various materials (longitudinal mode propagation). The transition time for a wideband ultrasound pulse can easily be measured and along with the physical dimension of the container a speed of sound may be calculated. The speed of sound varies significantly, even in water, as the chemical composition is varied. If the geometry is known then the speed of sound becomes an easy way to differentiate two materials.
Figure imgf000013_0001
Graph 2: Sound velocity for differing concentrations of various electrolyte solutions (after Dukliin et al.) is shown above.
Figure imgf000014_0001
Frequency [MHz|
Graph 3: Frequency dependence of attenuation for various electrolyte solutions (after Dukhin et al.)
Figure imgf000015_0001
Graph 4: Amplitude of measured signal for different frequencies as a function of the number fat drops added to a container of water. We can detect about a dozen drops of fat in 355 ml of water in an aluminum container.
Figure imgf000016_0001
Graph 5: Comparison of Time Series Data, 3rd Order Cumulant data and Bispectra data. Scale factors (Cumulant x-axis and y-axis are both -102.4 uS to + 102.4 uS each pixel is 0.8 us 256 points) (Bispectra- 312.5 kHz to + 312.5 kHz each point is 4.88 kHz 128 points) (Time series data 20 MSS, 6500 samples, 325 uS, ).
Figure imgf000017_0001
Graph 6: Time Domain Ultrasound for nine container/contents combinations
Figure imgf000017_0002
Table 2: Measured Speed of sound using laser-based ultrasound on a number of different containers and contents.
In one preferred embodiment, the analysis of the signal of the system 1 is preferably based on the following:
Timing of the return pulse is used to calculate speed of sound of the material in the container. Spectral analysis is used to determine the frequency and attenuation response of the container and contents. This technique is used to identify various constituents or ingredients in the preparation of food products. Vx in the liquid form preferably has a speed of sound similar to water and the molecular makeup of the material is likely to result in a frequency-dependent spectra that is different than water.
Fluctuation Enhanced Analysis [Kish, Mendel] is preferably used to investigate the non- Gaussian noise characteristics of the signals that may translate into useful information. Smulko and Kish have identified a methodology that suggests the stochastic component of a chemical sensor signal contains valuable information that can be visualized not only by spectral analysis but also by methods of higher-order statistics (HOS). The analysis of HOS enables the extraction of non-conventional features that lead to significant improvements in selectivity and sensitivity. We pay particular attention to the bispectrum that characterizes the non-Gaussian component and detects non stationary in analyzed noise. As Smulko' s results suggest that the bispectrum can be applied for material recognition, this will be tried also.
Ultrasound data for each measurement was acquired as multiple time series, which were then phase locked and averaged in software to provide a clear signal, well above the noise floor. The third order cumulant of the processed time series was obtained by the expression:
n=N
C3x (k, l) = Σ ∑ x(n)x(n + k)x{n + /) n=0
This was done over the range k = (-128...128), / = (-128...128) times a scale factor, with n running over the range (0...6500), producing the two-dimensional plots given below. A second order Fourier Transform was then performed on each cumulant to obtain the bispectrum, by the expression:
Figure imgf000018_0001
Each bispectrum is plotted in gray scale pixel values, as the sum of the sine and cosine Fourier components.
Another example of the preferred embodiment is shown in Fig. 6 which shows an example system configuration. Here the device under test or object (71) is, for example, a 55 gal. Drum or container. Beam steering optics (72) is, for example, a telephoto lens. An excitation beam combiner (73) is preferably a beam splitter. A probe beam combiner (74) is, for example, a beam splitter. A preferred adaptive interferometer (75) is a photorefractive crystal, mirror, and polarizer. A detector assembly (76) is, for example, a beam splitter differential photo-detector combination. An excitation laser assembly (77) includes preferably a Q-switched YAG laser while a probe laser assembly (78) includes, for example, a diode laser.
A preferred excitation beam driver (79) is a current controller pulsing circuit. A probe laser driver (80) is, for example, a constant current supply with diode feedback. Drive electronics for adaptive interferometer (81) preferably include a bias supply for photorefractive crystal. Detector electronics (82), for example, include a differential operational amplifier.
Preferably, a microprocessor assembly (83) is a PC 104 minicomputer module and power management (84) includes a power supply battery charging module. Thermal management (85) includes, for example, a thermoelectric cooler and controller. User interface (86) is, for example, a LCD touch screen module. Communications interface (87) is, for example, a Wi-Fi interface module, Ethernet interface module, USB interface module, ZigBee interface module. Optical Subsystem (88) (see, e.g., Fig. 7). Business intelligence subsystem (89) is, for example, an application server, data base server, application software and database software and data to provide list parameters for contents of shipping containers and software integration to software manifests of shipping container contents.
Another preferred embodiment of the optical subsystem is shown at Fig. 7. In this example, the container or device under test (201) is, for example, a 5/55/65 gal. drum. A telephoto lens (202) is also provided. The excitation laser (203), in an example 1 is a diode- pumped solid state laser housed in TO-3 case having a wavelength: 1.54 μm, Pulse Energy: 100 μj, Pulse Width:2 ns, Peak Power: 50 Kw, Repetition Rate: SS to 10 Hz. In an example 2, a diode pumped solid-state laser is provided having a Wavelength: 1.54 μm, Pulse Energy: 4 mJ, Pulse Width:7 ns, Repetition Rate: SS to 10 Hz. The probe laser (204), for example, is a fabry Perot laser cavity having a single transverse mode of 13OmW in wavelength range 1550 nm. InGaAs MQW. In another example, a single transverse mode of 44mW is provided in wavelength range 1550 irm.InGaAsP/InP SQW.
The non-polarizing beam splitter (205), in an example 1, has a BK7 grade A optical glass having a Dimension Tolerance ±0.2mm, Flatness 1/4 @ 632.8 nm per 25mm, Surface Quality 60/40 scratches and dig, 50/50±5%, for random polarization, T=(Ts+Tρ)/2, R=(Rs+Rρ)/2, Beam Deviation <3 arc minutes, 20mm. hi an example 2, it has a Narrow Band: BK7 grade A optical glass, Broadband: SF5 optical glass, Dimension Tolerance ±0.2mm, Flatness 1/4 @ 632.8 nm per 25mm, Surface Quality 60/40 scratches and dig, Transmittance 45%±5%, Absorption <10%, Beam Deviation <3 arc minutes.
The polarizing beam splitter (206) is preferably a Narrow Band: BK7 grade A optical glass, Broadband: SF5 optical glass with a Dimension Tolerance ±0.2mm, Extinction Ratio >100:l, Flatness 1/4 @ 632.8 nm per 25mm, Surface Quality 60/40 scratches and dig, Principal Transmittance Tp>95% and Ts<l%, Principal Reflectance Rs>99% and Rp<5%, Beam Deviation <3 arc minutes. The polarizer (207) is preferably a linear NIR polarizer nominal 50% at 1550. Alternatively, the polarizer is a linear polarizer having an extinction ratio better than 10,000:1, High transmission, Wide acceptance angle, and Low wavefront distortion.
The retardation plate (208) preferably has dimensions 5mm x 5mm, Material: Crystal Quartz, Substrate: BK-7, 2mm thick, Bonding: Cement, Wavelength: 1550nm, Coating: AR < 0.5%. In an example 2, the plate is a Crystal quartz, having Dimension Tolerance +0.0, -0.2mm, Wavefront Distortion <l/8@632.8, Retardation Tolerance <l/500, Parallelism <1 arc second, Clear aperture >80%, Surface Quality 20/10 scratches & dig, Coating RO.2% on both surfaces at central wavelength.
The photorefractive crystal (209), in example 1, is a CdTe, Ge crystal germainium-doped to give a dark conductivity of 10"9 Ω cm"1 with dimensions 4 mm x 5 mm x 10 mm cut along [112], [111], and [HO] directions respectively having faces parallel to [110] polished, faces parallel to [111] silvered. In an example 2, a CdTe:V, crystal vanadium-doped is provided with dimensions 3 mm x 3 mm x 5 mm cut along [112], [111], and [UO] directions respectively having the faces parallel to [110] polished, faces parallel to [111] silvered. In an example 3, a GaAs crystal with no doping with dimensions 5 mm x 5 mm x 5 mm cut along [001], [110], and [110] directions respectively is provided that also has the faces parallel to [UO] polished. The mirror (210), in example 1, is preferably BK7, Pyrex or UV Fused Silica, and has a Dimension Tolerance: + 0.0, - 0.2mm, Thickness Tolerance: ± 0.2mm, Clear Aperture: > 80%, Flatness: 1/10 @ 633nm, Parallelism: <1 arc minute, Surface Quality: 20/10 (S/D), Bevel(Chamfer): 0.15~0.35mmx45° face width x 45° ±15°, Coating Surface(Sl): AOI=O0, R>99.8%, AOI=45°, R>99.5% (Rs>99.9%, Rp>99.2%. In example 2, the material is BK7 Grade A Optical Glass, and the Dimension Tolerance is + 0.0, - 0.2mm, Thickness Tolerance is ± 0.2mm, Clear Aperture is > 80%, Parallelism is <1 arc minute, Surface Quality is 60/40 (S/D), and Bevel(Chamfer) is 0.15~0.35mmx45° face width x 45° ±15° ).
The photodiode (211), in an example 1, is InGaAs Photodiode with a 15 MHz Bandwidth and a 1200-2600nm, 01mm Active Area, hi an example 2, it is an InGaAs Photodiode with a 1 GHz Bandwidth, and al000-1600nm, 75 urn Active Area.
Although the best mode contemplated by the inventors of carrying out the present invention is disclosed above, practice of the present invention is not limited thereto. It will be manifest that various additions, modifications and rearrangements of the features of the present invention may be made without deviating from the spirit and scope of the underlying inventive concept.
Moreover, the individual components need not be formed in the disclosed shapes, or assembled in the disclosed configuration, but could be provided in virtually any shape, and assembled in virtually any configuration. Further, although the components are described herein as physically separate modules, it will be manifest that these may be integrated into the apparatus with which it is associated. Furthermore, all the disclosed features of each disclosed embodiment can be combined with, or substituted for, the disclosed features of every other disclosed embodiment except where such features are mutually exclusive.
REFERENCES
Laser Ultrasonics: Techniques and Applications, CB. Scruby and L.E. Drain, Adam Hilger, Bristol, England, 1990.
K. Jarasiunas, V. Gudelis, P. Delaye, G. Roosen, Review of Scientific Instruments, Volume 69, Number 11, November 1998, pg 3776.
H. J. von Bardeleben, J.C. Launay, V. Mazoyer, Appl. Phys. Lett. 63 (8) 23 August 1993, pg 1140. K. Shcherbin, V. Danylyuk, Z. Zakharuk, I. Rarenko, M.B. Klein, Journal of Alloys and Compounds 371 (2004) pg. 191.
A. Blouin, J-P. Monchalin, Appl. Phys. Lett. 65 (8) 22 August 1994
R. K. Ing and J-P Moncalin, Appl. Phys. Lett. 59 (25) 16 December 1991, pg 3233.
L.A. Gologvan, G.I. Petrov, S.A. Gavrilov, V.A. Mel'nikov, L. Li, S.O. Knonrov, A.B. Fedotov, A.M. Zheltikov, P.K. Kashkarov, V. Y. Timoshenko, V. V. Yakovlev, Proc. Of SPIE, Vol. 5360, 2004, pg 333.
K. Kuroda, Y. Okazaki, T. Shimura, M. Chihara, M. Itoh, I. Ogura, Optics Letters, 15 (21), November 1990, pg 1197
O. Kobozev, A. Kamshilin, E. Raita, N. Nazhestkina, T. Jaaskelainen, Journal of Optics A, 3 (3) May 2001, L9.
P. Delaye, Appl. Phys. Lett. 67 (22) November 1995., pg 3251.
R. K. Ing. D. Royer, B. Pouet, S. Krishnaswamy, 1996 IEEE Ultrasonics Symposium, pg. 681.
B. Campagne, A. Blouin, L. Pujol, J.P. Monchalin, Review of Scientific Instruments, 72 (5), May 2001, pg. 2478.
Y. Iida, S. Ashihara, H. Ono, T. Shimura, K Kuroda, A. Kamshilin, O. Matoba, J. Opt. A. 5 (2003) S457.
Tokuyuki Honda, Toshihisa Yamashital, Hirokazu Matsumoto Optical Measurement of Ultrasonic Nanometer Motion of Rough Surface by Two- Wave Mixing in Bil2SiO20 Jpn. J. Appl. Phys. Vol.34(1995) 3737-3740 Part 1, No. 7A, 15 July 1995.
Kamshilin A A, Paivasaari K, Klein M B and Pouet B 2000 Appl. Phys. Lett. 11 4098-100.
P. Delaye, A. Blouin, D. Drolet, L.-A. de Montmorillon, G. Roosen and J.-P. Monchalin, Detection of ultrasonic motion of a scattering surface by photorefractive InP:Fe under an applied dc field J. Opt. Soc. Am. B, Opt. Phys. (USA) 14 (July 1997) 1723-34.
Leilei Peng, David D. Nolte, Ping Yu, Michael R. Melloch , Adaptive optical coherence-domain reflectometry using photorefractive quantum wells, JOSA B, Volume 21, Issue 11, 1953-1963, November 2004.
Kathryn Atherton, Brian Culshaw, Fengzhong Dong, Pan Jun, S. Gareth Pierce, Colin I. Swift, Generation and detection of broadband laser generated ultrasound from low-power laser sources, Proc. SPIE Vol. 4417, p. 19-32.
Honda T, Yamashita T and Matsumoto H 1995 Japan. J. Appl. Phys. 34 3737-40. Delaye P, Blouin A, Drolet D, de Montmorillon L-A5 Roosen G and Monchalin J-P 1997 J. Opt. Soc. Am. B 14 1723-34.
Ziari M5 Steier W H5 Ranon P M, Klein M B and Trivedi S B 1992 J. Opt. Soc. Am. B 9 1461-6 . Kamshilin A A5 Paivasaari K5 Klein M B and Pouet B 2000 Appl Phys. Lett. 77 4098-100.
Kamshilin A A5 Paivasaari K, Khomenko A V and Fuentes-Hernandez C A 1999 Opt. Lett. 24 832-4.
Kamshilin A A5 Iida Y5 Ashihara S5 Shimura T and Kuroda K 1999 Appl. Phys. Lett. 74 2575-7.
Glass A M5 Johnson A M5 Olson D H, Simpson W and Ballman A A 1984 Appl. Phys. Lett. 44 948-50.
Kuroda K5 Okazaki Y5 Shimura T5 Okamura H5 Chihara M5 Itoh M and Ogura I 1990 Opt. Lett. 15 1197-9.
Raita E, Kobozev O5 Kamshilin A A and Prokofiev V V5 2000 Opt. Lett. 25 1261-3.
Stepanov S and Petrov M P 1988, Photorefractive Materials and their Applications. Fundamental Phenomena ed P Gunter and J P Huignard (Berlin: Springer) p 263.
J. M. Smulko * and L. B. Kish, Sensors and Materials vol. 16, in press (2004)

Claims

CLAIMSWe claim:
1. A system for stand-off, non-invasive, non-radiological, eye-safe, non-consumable characterization of an object which comprises in combination: a. At least one pulsed laser emitter for directing energy at the surface of an object, wherein the ultrasonic wave is generated within the object to be characterized b. A remote means of measuring the vibrational excitation in the object, whereby the object is remotely characterized.
2. The apparatus of claim 1, wherein said remote means of measuring the vibrational excitation includes a laser vibrometer.
3. The apparatus of claim 1, wherein the object includes fluid-filled containers and pipes.
4. The apparatus of claim 1, wherein the object is a mold containing powders, liquids or solids.
5. The apparatus of claim 1, wherein the object is at least one of a shipping container, drum or tank used for transporting liquids.
6. A remote sensing device for determining the attributes of container comprising: a means for determining at least one of container dimensions, container materials, and container defects; a means for detecting at least one of a solid, a liquid, a gas and mixtures of a solid, liquid, and gas; a means for detecting at least one of the following: chemicals flowing in a pipe, waste flowing in a stream or river, and pollutants in a liquid stationary in a pool or tank; and a means for sampling by at least one mechanical/acoustical vibration, infrasonic means, audible means, and ultrasonic means.
7. The device of claim 6, wherein the means for sampling has a vibration launched by electromagnetic radiation.
8. The device of claim 6, wherein the means for sampling has a vibration launched by radio/microwave radiation.
9. The device of claim 6, wherein the means for sampling has a vibration is launched by terahertz radiation.
10. The device of claim 6, further including an optical sensor.
11. The device of claim 6, further including a pulsed laser with a generator for generating at least one of a single pulse, multiple pulses, a uniform time interval, a varying time interval, a pulse compression, a shaped pulse, and a phased array.
12. The device of claim 6, further including an X-Ray generator and detector.
13. The device of claim 10, wherein the optical sensor includes at least one of infrared, visible light, and ultraviolet.
14. The device of claim 6, further including interferometer vibrometer.
15. The device of claim 14, wherein the interferometer includes reference beam interferometer.
16. The device of claim 14, wherein the interferometer includes Single Beam Inteferometer.
17. The device of claim 14, wherein the interferometer includes Adaptive Interferometer.
18. The device of claim 6, further including two wave mixing.
19. The device of claim 6, further including four wave mixing.
PCT/US2006/016822 2005-05-04 2006-05-04 Method and apparatus of detecting an object WO2007070080A2 (en)

Priority Applications (5)

Application Number Priority Date Filing Date Title
JP2008510131A JP5306810B2 (en) 2005-05-04 2006-05-04 Method and apparatus for detecting an object
US11/913,414 US8151644B2 (en) 2005-05-04 2006-05-04 Method and apparatus of detecting an object
CA002606848A CA2606848A1 (en) 2005-05-04 2006-05-04 Method and apparatus of detecting an object
EP06752084A EP1883824A4 (en) 2005-05-04 2006-05-04 Method and apparatus of detecting an object
US13/443,335 US8555725B2 (en) 2005-05-04 2012-04-10 Method and apparatus of detecting an object

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
US67775105P 2005-05-04 2005-05-04
US60/677,751 2005-05-04

Related Child Applications (2)

Application Number Title Priority Date Filing Date
US11/913,414 A-371-Of-International US8151644B2 (en) 2005-05-04 2006-05-04 Method and apparatus of detecting an object
US13/443,335 Continuation US8555725B2 (en) 2005-05-04 2012-04-10 Method and apparatus of detecting an object

Publications (2)

Publication Number Publication Date
WO2007070080A2 true WO2007070080A2 (en) 2007-06-21
WO2007070080A3 WO2007070080A3 (en) 2008-01-03

Family

ID=38163366

Family Applications (1)

Application Number Title Priority Date Filing Date
PCT/US2006/016822 WO2007070080A2 (en) 2005-05-04 2006-05-04 Method and apparatus of detecting an object

Country Status (5)

Country Link
US (2) US8151644B2 (en)
EP (1) EP1883824A4 (en)
JP (1) JP5306810B2 (en)
CA (1) CA2606848A1 (en)
WO (1) WO2007070080A2 (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8151644B2 (en) 2005-05-04 2012-04-10 Brandt Innovative Technologies, Inc. Method and apparatus of detecting an object
US8482408B1 (en) 2008-12-08 2013-07-09 The United States Of America, As Represented By The Secretary Of The Navy Explosives and contraband detection system
EP3913361A1 (en) * 2020-05-20 2021-11-24 The Boeing Company Beam steering for laser ultrasonic inspection systems
US11973319B2 (en) 2017-11-17 2024-04-30 Uab Brolis Semiconductors Radiant beam combining of multiple multimode semiconductor laser diodes for directional laser beam delivery applications

Families Citing this family (15)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8179595B2 (en) * 2008-01-29 2012-05-15 Corning Incorporated Polarizing photorefractive glass
US9404899B1 (en) * 2011-03-14 2016-08-02 Raytheon Company Methods and apparatus for acoustic inspection of containers
US20130220017A1 (en) * 2012-02-23 2013-08-29 Sung Kim Non-destructive inspection apparatus for detecting internal defect of concrete structure using ultrasonic waves
US20150022658A1 (en) * 2013-07-16 2015-01-22 University Of North Carolina At Charlotte Noise reduction techniques, fractional bi-spectrum and fractional cross-correlation, and applications
US9395338B2 (en) * 2013-11-12 2016-07-19 Woods Hole Oceanographic' Institution Sensor system for environmental impact monitoring
US9778228B2 (en) 2013-11-12 2017-10-03 Woods Hole Oceanographic Institution Turbine sensor system for environmental impact monitoring
US9305344B2 (en) * 2014-04-22 2016-04-05 The Boeing Company Method for improving linear feature detectability in digital images
US10161909B2 (en) 2015-10-29 2018-12-25 Mustang Sampling Llc Steady state fluid flow verification for sample takeoff
US10151731B2 (en) * 2015-11-13 2018-12-11 The Boeing Comapny Ultrasonic system for nondestructive testing
US10942152B2 (en) * 2016-06-21 2021-03-09 Shimadzu Corporation Defect inspection device and method
US10634646B2 (en) * 2017-01-20 2020-04-28 GTBM, Inc. Acoustic frequency based system with crystalline transducer module for non-invasive detection of explosives, contraband, and other elements
US10229487B2 (en) * 2017-02-27 2019-03-12 Amazon Technologies, Inc. Optical vibrometric testing of container for items
TR201705816A2 (en) 2017-04-19 2018-10-22 Ford Otomotiv Sanayi As A VIBRATION AND NOISE CHARACTERISTIC MEASUREMENT SYSTEM AND METHOD
WO2020047279A1 (en) * 2018-08-31 2020-03-05 Board Of Trustees Of Michigan State University Laser system for blood or tissue assessment
US11493441B2 (en) * 2019-01-15 2022-11-08 Wyatt Technology Corporation Flow cell, read head, and skid attachment

Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4455268A (en) 1981-07-09 1984-06-19 Applied Polymer Technology, Inc. Control system for processing composite materials
US4758803A (en) 1987-07-13 1988-07-19 General Electric Company Marginal oscillator for acoustic monitoring of curing of plastics
US4862384A (en) 1987-08-03 1989-08-29 Rockwell International Corporation Method of measuring the dynamic viscosity of a viscous fluid utilizing acoustic transducer
US5505090A (en) 1993-11-24 1996-04-09 Holographics Inc. Method and apparatus for non-destructive inspection of composite materials and semi-monocoque structures
US5533339A (en) 1994-05-27 1996-07-09 The Boc Group Plc Air separation
US6029520A (en) 1998-10-09 2000-02-29 The Regents Of The University Of California Ultrasonic monitoring of resin curing in a press for the production of particle board and similar materials
US6518584B1 (en) 1999-10-25 2003-02-11 James Woodruff System and method for characterizing targets using two forms of optical irradiation and acoustic irradiation

Family Cites Families (32)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4543486A (en) * 1983-05-20 1985-09-24 The United States Of America As Represented By The Secretary Of The Army Method and apparatus for using a photoacoustic effect for controlling various processes utilizing laser and ion beams, and the like
US4567769A (en) * 1984-03-08 1986-02-04 Rockwell International Corporation Contact-free ultrasonic transduction for flaw and acoustic discontinuity detection
JPS61120041A (en) 1984-11-16 1986-06-07 Yoshinori Sugitani Correlation photoacoustic imaging method
JP3082208B2 (en) 1990-03-30 2000-08-28 株式会社日立製作所 Photoacoustic signal detection method and apparatus, and semiconductor element internal defect detection method
JPH04286933A (en) 1991-03-15 1992-10-12 Takenaka Komuten Co Ltd Method for detecting release of building exterior material
US5672830A (en) * 1994-10-04 1997-09-30 Massachusetts Institute Of Technology Measuring anisotropic mechanical properties of thin films
US5929337A (en) * 1994-11-11 1999-07-27 M & A Packaging Services Limited Non-mechanical contact ultrasound system for monitoring contents of a moving container
US5698787A (en) * 1995-04-12 1997-12-16 Mcdonnell Douglas Corporation Portable laser/ultrasonic method for nondestructive inspection of complex structures
US5821424A (en) * 1995-10-16 1998-10-13 Lockheed Idaho Technologies Company Method and apparatus for analyzing the fill characteristics of a packaging container
GB9522949D0 (en) * 1995-11-09 1996-01-10 M & A Packaging Serv Ltd Fill level measuring
US5932119A (en) 1996-01-05 1999-08-03 Lazare Kaplan International, Inc. Laser marking system
US5801312A (en) * 1996-04-01 1998-09-01 General Electric Company Method and system for laser ultrasonic imaging of an object
US5893363A (en) 1996-06-28 1999-04-13 Sonosight, Inc. Ultrasonic array transducer transceiver for a hand held ultrasonic diagnostic instrument
US6075603A (en) * 1997-05-01 2000-06-13 Hughes Electronics Corporation Contactless acoustic sensing system with detector array scanning and self-calibrating
US5886264A (en) * 1997-05-05 1999-03-23 Wayne State University System and method for predicting sound radiation and scattering from an arbitrarily shaped object
US6182512B1 (en) * 1997-06-13 2001-02-06 General Electric Company Method and apparatus for imaging thin structures
JPH1183433A (en) 1997-07-09 1999-03-26 Nippon Soken Inc Displacement amount meter and displacement amount measuring method
US5982482A (en) * 1997-07-31 1999-11-09 Massachusetts Institute Of Technology Determining the presence of defects in thin film structures
SE513148C2 (en) 1998-09-07 2000-07-17 Laszlo B Kiss Detection of chemicals based on resistance fluctuation spectroscopy
US6186004B1 (en) * 1999-05-27 2001-02-13 The Regents Of The University Of California Apparatus and method for remote, noninvasive characterization of structures and fluids inside containers
US6367328B1 (en) * 1999-07-12 2002-04-09 Digital Wave Corporation Noninvasive detection of corrosion, MIC, and foreign objects in fluid-filled containers using leaky guided ultrasonic waves
JP2003507727A (en) * 1999-08-23 2003-02-25 ザ トラスティーズ オブ ザ スティーブンス インスティテュート オブ テクノロジー Method and apparatus for remotely measuring vibration and properties of an object
US6593574B2 (en) * 1999-09-16 2003-07-15 Wayne State University Hand-held sound source gun for infrared imaging of sub-surface defects in materials
US20020100884A1 (en) * 2001-01-29 2002-08-01 Maddock Brian L.W. Digital 3-D model production method and apparatus
US6668654B2 (en) * 2001-08-15 2003-12-30 Lockheed Martin Corporation Method and apparatus for generating specific frequency response for ultrasound testing
US6856918B2 (en) * 2001-11-26 2005-02-15 Lockheed Martin Corporation Method to characterize material using mathematical propagation models and ultrasonic signal
GB0209053D0 (en) * 2002-04-22 2002-12-18 Bae Systems Plc Method and apparatus for laser vibrometry
US6938488B2 (en) * 2002-08-21 2005-09-06 Battelle Memorial Institute Acoustic inspection device
US7319639B2 (en) * 2004-12-20 2008-01-15 Luna Innovations Incorporated Acoustic concealed item detector
EP1883824A4 (en) 2005-05-04 2011-05-11 Brandt Innovative Technologies Inc Method and apparatus of detecting an object
US8220334B2 (en) * 2006-11-10 2012-07-17 Penrith Corporation Transducer array imaging system
EP2203733B1 (en) * 2007-10-25 2017-05-03 Washington University in St. Louis Confocal photoacoustic microscopy with optical lateral resolution

Patent Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4455268A (en) 1981-07-09 1984-06-19 Applied Polymer Technology, Inc. Control system for processing composite materials
US4758803A (en) 1987-07-13 1988-07-19 General Electric Company Marginal oscillator for acoustic monitoring of curing of plastics
US4862384A (en) 1987-08-03 1989-08-29 Rockwell International Corporation Method of measuring the dynamic viscosity of a viscous fluid utilizing acoustic transducer
US5505090A (en) 1993-11-24 1996-04-09 Holographics Inc. Method and apparatus for non-destructive inspection of composite materials and semi-monocoque structures
US5533339A (en) 1994-05-27 1996-07-09 The Boc Group Plc Air separation
US6029520A (en) 1998-10-09 2000-02-29 The Regents Of The University Of California Ultrasonic monitoring of resin curing in a press for the production of particle board and similar materials
US6518584B1 (en) 1999-10-25 2003-02-11 James Woodruff System and method for characterizing targets using two forms of optical irradiation and acoustic irradiation

Non-Patent Citations (4)

* Cited by examiner, † Cited by third party
Title
CB. SCRUBY; L.E. DRAIN; ADAM HILGER, LASER ULTRASONICS: TECHNIQUES AND APPLICATIONS, 1990
H. J. VON BARDELEBEN; J.C. LAUNAY; V. MAZOYER, APPL. PHYS. LETT., vol. 63, no. 8, 23 August 1993 (1993-08-23), pages 1140
K. JARASIUNAS; V. GUDELIS; P. DELAYE; G. ROOSEN, REVIEW OF SCIENTIFIC INSTRUMENTS, vol. 69, no. 11, November 1998 (1998-11-01), pages 3776
See also references of EP1883824A4

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8151644B2 (en) 2005-05-04 2012-04-10 Brandt Innovative Technologies, Inc. Method and apparatus of detecting an object
US8555725B2 (en) 2005-05-04 2013-10-15 Brandt Innovative Technologies, Inc. Method and apparatus of detecting an object
US8482408B1 (en) 2008-12-08 2013-07-09 The United States Of America, As Represented By The Secretary Of The Navy Explosives and contraband detection system
US11973319B2 (en) 2017-11-17 2024-04-30 Uab Brolis Semiconductors Radiant beam combining of multiple multimode semiconductor laser diodes for directional laser beam delivery applications
EP3913361A1 (en) * 2020-05-20 2021-11-24 The Boeing Company Beam steering for laser ultrasonic inspection systems
US11187679B1 (en) 2020-05-20 2021-11-30 The Boeing Company Beam steering for laser ultrasonic inspection systems

Also Published As

Publication number Publication date
JP2008542687A (en) 2008-11-27
CA2606848A1 (en) 2007-06-21
EP1883824A2 (en) 2008-02-06
WO2007070080A3 (en) 2008-01-03
US20130233084A1 (en) 2013-09-12
US8151644B2 (en) 2012-04-10
US20080289427A1 (en) 2008-11-27
JP5306810B2 (en) 2013-10-02
US8555725B2 (en) 2013-10-15
EP1883824A4 (en) 2011-05-11

Similar Documents

Publication Publication Date Title
US8151644B2 (en) Method and apparatus of detecting an object
CN107024542B (en) Airborne ultrasonic testing system for test object
Murfin et al. Laser-ultrasound detection systems: a comparative study with Rayleigh waves
Stratoudaki et al. Measurement of material nonlinearity using surface acoustic wave parametric interaction and laser ultrasonics
Blouin et al. Improved resolution and signal-to-noise ratio in laser-ultrasonics by SAFT processing
Johnson et al. Gas-coupled laser acoustic detection as a non-contact line detector for photoacoustic and ultrasound imaging
Krishnaswamy Theory and applications of laser-ultrasonic techniques
Zhang et al. Unraveling phononic, optoacoustic, and mechanical properties of metals with light-driven hypersound
Spytek et al. Non-contact detection of ultrasound with light–Review of recent progress
Blessing et al. Ultrasonic measurements of surface roughness
Vangi et al. Crack detection with gas-coupled laser acoustic detection technique
Devos et al. High-laser-wavelength sensitivity of the picosecond ultrasonic response in transparent thin films
Zamiri et al. Laser ultrasonic velocity measurement for phase transformation investigation in titanium alloy
Ohara et al. Monitoring growth of closed fatigue crack using subharmonic phased array
Zappia et al. Thz imaging for food inspections: A technology review and future trends
Zhang et al. Ultrafast laser-induced guided elastic waves in a freestanding aluminum membrane
US20110267599A1 (en) Systems, methods, devices, and computer readable media for terahertz radiation detection
McKie et al. Dual-beam interferometer for the accurate determination of surface-wave velocity
Royer et al. A sensitive ultrasonic method for measuring transient motions of a surface
Manzo et al. Application of a laser heterodyne technique to characterize surface acoustic waves generated via a pulsed laser excitation
Ma et al. Research of pesticide residues on fruit by terahertz spectroscopy technology
Blouin et al. Laser ultrasonics: a new tool for the industry
Ellwood The effect of microstructure and fatigue on the acoustoelastic response of aerospace materials
Maznev et al. Impulsive stimulated thermal scattering for sub-micron-thickness film characterization
Tanaka et al. Nondestructive detection of small defects by laser ultrasonics

Legal Events

Date Code Title Description
121 Ep: the epo has been informed by wipo that ep was designated in this application
ENP Entry into the national phase

Ref document number: 2606848

Country of ref document: CA

ENP Entry into the national phase

Ref document number: 2008510131

Country of ref document: JP

Kind code of ref document: A

NENP Non-entry into the national phase

Ref country code: DE

WWE Wipo information: entry into national phase

Ref document number: 2006752084

Country of ref document: EP

NENP Non-entry into the national phase

Ref country code: RU

WWE Wipo information: entry into national phase

Ref document number: 11913414

Country of ref document: US