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Dive into the research topics where Daniel J. Schneberk is active.

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Featured researches published by Daniel J. Schneberk.


IEEE Transactions on Nuclear Science | 1990

Calculation of the rotational centers in computed tomography sinograms

Stephen G. Azevedo; Daniel J. Schneberk; J.P. Fitch; Harry E. Martz

An efficient method for accurately calculating the center-of-rotation, or projection center, for parallel computed tomography projection data, or sinograms, is described. This method uses all the data in the sinogram to estimate the center by a least-squares technique and requires no previous calibration scan. The method also finds the objects center-of-mass without reconstructing its image. Since the method uses the measured data, it is sensitive to noise in the measurements, but that sensitivity is relatively small compared to other techniques. Examples of its use on simulated and actual data are included. For fan-beam data over 360 degrees , two related methods are described to find the center in the presence or absence of a midline offset. >


International Journal of Radiation Applications and Instrumentation. Part A. Applied Radiation and Isotopes | 1990

Computed tomography systems and their industrial applications

Harry E. Martz; Stephen G. Azevedo; James M. Brase; K.E. Waltjen; Daniel J. Schneberk

Abstract x-Ray computed axial tomography (CT) provides cross-sectional views of materials, components, and assemblies for industrial non-destructive evaluation. We have applied CT imaging to quantitatively measure the 3-D distribution ogf x-ray attenuation at reasonably high resolutions. In our industrial x-ray CT-studies, we have centered on two technical approaches: a first-generation translate/rotate CT system that consist of well-collimated (∼ 0.55 mm) photon source detector, and a third-generation scanner that uses a fluoroscopy detector.


Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms | 1991

Computerized tomography studies of concrete samples

Harry E. Martz; G.P. Roberson; M.F. Skeate; Daniel J. Schneberk; Stephen G. Azevedo

Abstract X-ray computerized tomography (CAT or CT) is a sophisticated imaging technique that provides cross-sectional views of materials, components and assemblies for industrial nondestructive evaluation (NDE). We have studied the feasibility of using CT as an inspection tool for reinforced concrete and the use of multi-energy, linear, attenuation techniques to deduce variations in density (ρ) and/or atomic number (Z) that could be caused by varying the types of concrete mixes and/or compaction in the concrete itself. To perform this study, we designed and built a prototype medium-/high-energy (200- to 2000 keV) CT scanner — ZCAT — to image small concrete samples (± 30 cm in diameter and ± 75 cm in height) with a spatial resolution of about 2 mm. We used ZCAT to quantitatively inspect a 20 cm concrete cube with 1.27 cm diameter reinforcing bars (rebars) and to measure p and/or Z variations in a 20 cm diameter concrete cylinder. We describe the ZCAT scanner design, some of its physical limitations and the data-acquisition parameters used in our study. Our results and those of others [1,2] show that CT can be used to inspect reinforced concrete and to distinguish material p and/or Z variations within concrete.


Proceedings of SPIE | 1993

Three-dimensional dynamic thermal imaging of structural flaws by dual-band infrared computed tomography

Nancy DelGrande; Kenneth W. Dolan; Philip F. Durbin; Michael R. Gorvad; B. T. Kornblum; Dwight E. Perkins; Daniel J. Schneberk; Arthur B. Shapiro

We discuss three-dimensional dynamic thermal imaging of structural flaws using dual-band infrared (DBIR) computed tomography. Conventional (single-band) thermal imaging is difficult to interpret. It yields imprecise or qualitative information (e.g., when subsurface flaws produce weak heat flow anomalies masked by surface clutter). We use the DBIR imaging technique to clarify interpretation. We capture the time history of surface temperature difference patterns at the epoxy-glue disbond site of a flash-heated lap joint. This type of flawed structure played a significant role in causing damage to the Aloha Aircraft fuselage on the aged Boeing 737 jetliner. The magnitude of surface-temperature differences versus time for 0.1 mm air layer compared to 0.1 mm glue layer, varies from 0.2 to 1.6 degree(s)C, for simultaneously scanned front and back surfaces. The scans are taken every 42 ms from 0 to 8 s after the heat flash. By ratioing 3 - 5 micrometers and 8 - 12 micrometers DBIR images, we located surface temperature patterns from weak heat flow anomalies at the disbond site and remove the emissivity mask from surface paint of roughness variations. Measurements compare well with calculations based on TOPAX3D, a three-dimensional, finite element computer model. We combine infrared, ultrasound and x-ray imaging methods to study heat transfer, bond quality and material differences associated with the lap joint disbond site.


IEEE Transactions on Nuclear Science | 2011

Real-Time Reconstruction for 3-D CT Applied to Large Objects of Cultural Heritage

R. Brancaccio; M. Bettuzzi; F. Casali; M.P. Morigi; G. Levi; A. Gallo; G. Marchetti; Daniel J. Schneberk

In this paper, we describe the work done in order to run the CT 3-D reconstruction algorithm on the 120 GB raw data from the more than 25\thinspace000 radiographs acquired from the Kongo Rikishi (XIII century) Japanese wooden statue. The work was done using the Microsoft (Redmond) HPC cluster and then on a local cluster at the INFN of Bologna. A speed-up factor of 75 was reached.


SPIE's 1993 International Symposium on Optics, Imaging, and Instrumentation | 1993

Potential of Computed Tomography for inspection of aircraft components

Stephen G. Azevedo; Harry E. Martz; Daniel J. Schneberk

Computed Tomography (CT) using penetrating radiation (x- or gamma-rays) can be used in a number of aircraft applications. This technique results in 3D volumetric attenuation data that is related to density and effective atomic number. CT is a transmission scanning method that must allow complete access to both sides of the object under inspection; the radiation source and detection systems must surround the object. This normally precludes the inspection of some large or planar (large aspect ratio) parts of the aircraft. However, we are pursuing recent limited-data techniques using object model information to obtain useful data from the partial information acquired. As illustrative examples, we describe how CT was instrumental in the analysis of particular aircraft components. These include fuselage panels, single crystal turbine blades, and aluminum-lithium composites.


IEEE Transactions on Nuclear Science | 2016

System-Independent Characterization of Materials Using Dual-Energy Computed Tomography

Stephen G. Azevedo; Harry E. Martz; Maurice B. Aufderheide; William D. Brown; Kyle M. Champley; Jeffrey S. Kallman; G. Patrick Roberson; Daniel J. Schneberk; Isaac M. Seetho; Jerel A. Smith

We present a new decomposition approach for dual-energy computed tomography (DECT) called SIRZ that provides precise and accurate material description, independent of the scanner, over diagnostic energy ranges (30 to 200 keV). System independence is achieved by explicitly including a scanner-specific spectral description in the decomposition method, and a new X-ray-relevant feature space. The feature space consists of electron density, ρe, and a new effective atomic number, Ze, which is based on published X-ray cross sections. Reference materials are used in conjunction with the system spectral response so that additional beam-hardening correction is not necessary. The technique is tested against other methods on DECT data of known specimens scanned by diverse spectra and systems. Uncertainties in accuracy and precision are less than 3% and 2% respectively for the (ρe, Ze) results compared to prior methods that are inaccurate and imprecise (over 9%).


Proceedings of SPIE | 2015

Transparent ceramic scintillators for gamma spectroscopy and MeV imaging

Nerine J. Cherepy; Zachary M. Seeley; S.A. Payne; Erik L. Swanberg; Patrick R. Beck; Daniel J. Schneberk; G. F. Stone; R. Perry; Brian Wihl; Scott E. Fisher; Steve Hunter; Peter A. Thelin; R. R. Thompson; N. M. Harvey; T. Stefanik; J. Kindem

We report on the development of two new mechanically rugged, high light yield transparent ceramic scintillators: (1) Ce-doped Gd-garnet for gamma spectroscopy, and (2) Eu-doped Gd-Lu-bixbyite for radiography. GYGAG(Ce) garnet transparent ceramics offer ρ = 5.8g/cm3, Zeff = 48, principal decay of <100 ns, and light yield of 50,000 Ph/MeV. Gdgarnet ceramic scintillators offer the best energy resolution of any oxide scintillator, as good as R(662 keV) = 3% (Si-PD readout) for small sizes and typically R(662 keV) < 5% for cubic inch sizes. For radiography, the bixbyite transparent ceramic scintillator, (Gd,Lu,Eu)2O3, or “GLO,” offers excellent x-ray stopping, with ρ = 9.1 g/cm3 and Zeff = 68. Several 10” diameter by 0.1” thickness GLO scintillators have been fabricated. GLO outperforms scintillator glass for high energy radiography, due to higher light yield (55,000 Ph/MeV) and better stopping, while providing spatial resolution of >8 lp/mm.


Proceedings of SPIE | 1993

Three-dimensional nonintrusive imaging of obscured objects by x-ray and gamma-ray computed tomography

Harry E. Martz; Daniel J. Schneberk; G. P. Roberson

Members of the Nondestructive Evaluation Section at the Lawrence Livermore National Laboratory (LLNL) are implementing the advanced three-dimensional imaging technique of x- and gamma-ray computed tomography (CAT or CT) for industrial and scientific obscured object evaluation. This technique provides internal and external views of materials, components, and assemblies nonintrusively. Our work includes building of CT scanners as well as data preprocessing, image reconstruction, display and analysis algorithms. These capabilities have been applied to a variety of industrial and scientific NDE applications. We have used CT to study various objects with obscured features at our laboratory ranging in size from 1 mm3 to 1 m3. In these studies, CT has revealed flaws (e.g. cracks, voids, and inclusions), internal and external dimensional information, differences in elemental composition or material density, and other important material characteristics. CT has also been used to localize, identify, and quantify radioisotopes within canisters. As illustrative examples, we describe how CT was instrumental in the analysis of concrete specimens, diesel engine thermocouple plugs, jet engine turbine blades, ballistic target materials, and radioactive waste canisters.


IEEE Transactions on Nuclear Science | 1991

Nuclear-spectroscopy based, first-generation, computerized tomography scanners

Harry E. Martz; G.P. Roberson; Daniel J. Schneberk; Stephen G. Azevedo

A number of inexpensive, nuclear-spectroscopy-based, first-generation, computerized tomography (CT) scanners have been built to satisfy most Lawrence Livermore National Laboratory (LLNL) CT inspection requirements. The authors describe these CT scanners in detail and discuss their advantages and disadvantages when compared to the more common and more recent current-integration-based scanners. The major advantage of nuclear-spectroscopy-based scanners is that they can be used to determine all internal, spatially distributed, effective-atomic-number and density map within the object. It is also shown, how these scanners can be used to acquire meaningful chemical information for nondestructive characterization of materials and dimensional information for evaluating assembled components. >

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Harry E. Martz

Lawrence Livermore National Laboratory

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Peter J. Shull

Lawrence Livermore National Laboratory

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Stephen G. Azevedo

Lawrence Livermore National Laboratory

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G.P. Roberson

Lawrence Livermore National Laboratory

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Kenneth W. Dolan

Lawrence Livermore National Laboratory

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Dwight E. Perkins

Lawrence Livermore National Laboratory

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James M. Brase

Lawrence Livermore National Laboratory

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A. J. De Groot

Lawrence Livermore National Laboratory

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Anil K. Jain

University of California

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Anthony J. De Groot

Lawrence Livermore National Laboratory

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