Larry A. Franks
Sandia National Laboratories
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Featured researches published by Larry A. Franks.
Proceedings of SPIE | 2010
Arnold Burger; Larry A. Franks; R. B. James
This PDF file contains the Front Matter associated with SPIE Proceedings volume 7805, including the Title page, Copyright information, Table of Contents, and Conference Committee listing.
Proceedings of SPIE | 2013
Michael Fiederle; Arnold Burger; Larry A. Franks; R. B. James
This PDF file contains the front matter associated with SPIE Proceedings Volume 8852 including the Title Page, Copyright information, Table of Contents, Introduction, and Conference Committee listing.
Proceedings of SPIE | 2009
R. B. James; Larry A. Franks; Arnold Burger
This PDF file contains the front matter associated with SPIE Proceedings Volume 7449, including the Title Page, Copyright information, Table of Contents, the Conference Committee listing and introduction.
Proceedings of SPIE | 2008
Arnold Burger; Larry A. Franks; R. B. James
This PDF file contains the front matter associated with SPIE Proceedings Volume 7079, including the Title Page, Copyright information, Table of Contents, Introduction, and the Conference Committee listing.© (2008) COPYRIGHT SPIE--The International Society for Optical Engineering. Downloading of the abstract is permitted for personal use only.This PDF file contains the front matter associated with SPIE Proceedings Volume 7079, including the Title Page, Copyright information, Table of Contents, Introduction, and the Conference Committee listing.
Hard X-Ray, Gamma-Ray, and Neutron Detector Physics XIX 2017 | 2017
Mohan Li; Shiva Abbaszadeh; Michael Fiederle; Arnold Burger; Larry A. Franks; R. B. James; Stephen A. Payne
One electrode configuration frequently used in CZT detectors is the cross-strip pattern. The cathode-to-anode signal ratio (C/A) can be used to estimate the position of photon interaction in the direction perpendicular to the electrode plane. In addition, C/A is used to calibrate for the depth-dependent anode signal. Based on the design configuration of the electrode widths with respect to the CZT thickness, their measured energy spectrum varies due to the small pixel effect and charge trapping. In this work we evaluate the effect of a poor cathode energy resolution on the depth of interaction correction and anode signal recovery.
Hard X-Ray, Gamma-Ray, and Neutron Detector Physics XIX | 2017
A. E. Bolotnikov; G. S. Camarda; R. Gul; Gianluigi De Geronimo; J. Fried; G. Yang; A. Hossain; Luis A. Ocampo Giraldo; E. Vernon; R. B. James; Michael Fiederle; Arnold Burger; Larry A. Franks; Stephen A. Payne
We present new results from testing a small array of position-sensitive virtual Frisch-grid gamma-ray detectors. Such arrays provide high-detection efficiency, excellent energy and position resolution. They can be used in compact hand-held instruments or in large-area gamma ray imaging cameras. The high granularity position sensing enables these detectors to correct the response non-uniformity caused by crystal defects. This important feature allows one to achieve high detection performance while using standard-grade (unselected) CZT crystals, which is expected to reduce the overall cost of field deployable high-resolution CZT gamma ray detection instruments. Here, we report the results of testing several array prototypes with configurations designed for different applications.
Hard X-Ray, Gamma-Ray, and Neutron Detector Physics XIX | 2017
H. Paul Martinez; Nerine J. Cherepy; Robert D. Sanner; Patrick R. Beck; Stephen A. Payne; Charles R. Hurlbut; Michael Fiederle; Arnold Burger; Larry A. Franks; R. B. James
Plastic scintillators are widely deployed for ionizing radiation detection, as they can be fabricated in large sizes, for high detection efficiency. However, commercial plastics are limited in use for gamma spectroscopy, since their photopeak is very weak, due to low Z, and they are also limited in use for neutron detection, since proton recoils are indistinguishable from other ionizing radiation absorption events in standard plastics. We are working on scale up and production of transparent plastic scintillators based on polyvinyltoluene (PVT) loaded bismuth metallorganics for gamma spectroscopy. When activated with standard organic fluors, PVT scintillators containing 8 wt% bismuth provide energy resolution of 11% at 662 keV. When Iridium complex fluors are used, we can load plastics up to 20 wt% bismuth, while obtaining energy resolution of 10% at 662 keV. Another formulation, activated with Ir fluors for use as neutron radiography scintillator may be used for high energy neutron radiography. Acknowledgements This work was performed under the auspices of the U.S. DOE by Lawrence Livermore National Laboratory under Contract DE-AC52-07NA27344, and has been supported by the US DOE National Nuclear Security Administration, Defense Nuclear Nonproliferation Research and Development under Contract No. DE-AC03-76SF00098
Hard X-Ray, Gamma-Ray, and Neutron Detector Physics XIX | 2017
Utpal N. Roy; G. S. Camarda; Y. Cui; R. Gul; A. Hossain; G. Yang; R. B. James; Steven L. Hunter; Patrick R. Beck; Nerine J. Cherepy; Stephen A. Payne; Michael Fiederle; Arnold Burger; Larry A. Franks
Intrinsic materials can offer advantages over doped materials for some important applications. The doped material might suffer from non-uniform distribution of the dopant, such as fine-scale striations and larger scale segregation, which might affect the overall device response, especially for large-volume detectors such as those in demand for homeland security applications for gamma spectroscopy. Cs2LiCeCl6 (CLCC), being an intrinsic scintillator, can be grown in large volume to produce large detectors with good performance, provided the crystals are free from unwanted scattering centers. CLCC belongs to the elpasolite family and the structure is cubic, so large-volume ingots can be grown without the strains resulting from anisotropic thermal expansion coefficients. In this presentation, we will discuss extensive material characterization and device response of CLCC for gamma and thermal neutron detector applications.
Hard X-Ray, Gamma-Ray, and Neutron Detector Physics XIX | 2017
Gianluigi De Geronimo; R. Gul; J. Fried; A. Hossain; Kenan Ünlü; E. Vernon; G. Yang; R. B. James; Luis A. Ocampo Giraldo; A. E. Bolotnikov; G. S. Camarda; Michael Fiederle; Arnold Burger; Larry A. Franks; Stephen A. Payne
High-resolution position-sensing has been proposed to correct response non-uniformities in Cadmium Zinc Telluride (CZT) gamma ray detectors by virtually subdividing the area into small voxels and equalizing responses from each voxel. 3D pixelated detectors coupled with multichannel readout electronics are the most advanced type of CZT devices offering many options in signal processing and enhancing detector performance. The main hurdle in achieving high sub-pixel position resolution is the relatively low signal induced on the neighboring pixels because of the electrostatic shielding effect caused by the collecting pixel. In addition, to achieve high position sensitivity one should rely on time-correlated transient signals, which means that digitized output signals must be used. Previous results have shown the benefit of using a focused laser beam to study position resolution in 3D pixelated detectors. We present the results of our studies to measure the amplitude of the pixel signals so that these can be used to measure positions of the interaction points. This is done with the processing of digitized correlated time signals measured from several adjacent pixels taking into account rise-time and charge-sharing effects. In these measurements we used a focused pulsed laser to generate a 10-micron beam at one milliwatt (650-nm wavelength) over the detector surface while the collecting pixel was moved in cardinal directions. The results include measurements that present the benefits of combining conventional pixel geometry with digital pulse processing for the best approach in achieving sub-pixel position resolution with different pixel dimensions ranging from 0.5 mm to 1.72 mm.
Hard X-Ray, Gamma-Ray, and Neutron Detector Physics XIX | 2017
Erik L. Swanberg; Zachary M. Seeley; Patrick R. Beck; Brian Wihl; Nerine J. Cherepy; Stephen A. Payne; Steven L. Hunter; Scott E. Fisher; Peter A. Thelin; Todd Stefanik; Joel Kindem; Michael Fiederle; Arnold Burger; Larry A. Franks; R. B. James
Gadolinium Garnet transparent ceramics doped with Ce, ((Gd,Y,Ce)3(Ga,Al)5O12), for gamma-ray spectroscopy provide high density, high light yield, high energy resolution , high Z, mechanical robustness, and they are unreactive to air and water. Gadolinium garnet single crystals are costly to grow, due to their high melting points, and suffer from non-uniform light yield, due to Ce segregation. In contrast, transparent polycrystalline ceramic Garnets are never melted, and therefore are less costly to produce and provide the uniform light yield required to achieve high energy resolution with a scintillator. GYGAG(Ce) transparent ceramics offer energy resolution as good as R(662 keV) = 3.5%, in a pixelated detector utilizing Silicon photodiode array readout. We have developed a modular handheld detector based on pixelated GYGAG(Ce) on a photodiode array, that offers directional detection for point source detection as well as gamma spectroscopy. Individual modules can be assembled into detectors ranging from pocket-size to large panels, for a range of applications. Large GYGAG(Ce) transparent ceramics in the 2-5 in3 size range have been fabricated at LLNL. Instrumentation of these ceramics with Silicon photomultipliers (SiPMs) and super bi-alkali PMTs has been explored and energy resolution as good as R(662 keV) = 5% has been obtained. Further improvements with SiPM readout will leverage their high quantum efficiency in the 500-650 nm range where GYGAG(Ce) emits, and implement electronics that minimize the effect of SiPM dark current and capacitance on the pulse height spectra. This work was performed under the auspices of the U.S. DOE by Lawrence Livermore National Laboratory under Contract DE-AC52-07NA27344, and has been supported by the US Department of Homeland Security, Domestic Nuclear Detection Office, under competitively awarded IAA HSHQDC-12-X-00149 under Contract No. DE-AC03-76SF00098. LLNL-ABS-724480.