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Dive into the research topics where Gary E. Hogan is active.

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Featured researches published by Gary E. Hogan.


Nature | 2003

Surveillance: Radiographic imaging with cosmic-ray muons

Konstantin N. Borozdin; Gary E. Hogan; C. L. Morris; William C. Priedhorsky; A. Saunders; Larry J. Schultz; Margaret E. Teasdale

Despite its enormous success, X-ray radiography has its limitations: an inability to penetrate dense objects, the need for multiple projections to resolve three-dimensional structure, and health risks from radiation. Here we show that natural background muons, which are generated by cosmic rays and are highly penetrating, can be used for radiographic imaging of medium-to-large, dense objects, without these limitations and with a reasonably short exposure time. This inexpensive and harmless technique may offer a useful alternative for detecting dense materials — for example, a block of uranium concealed inside a truck full of sheep.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1999

An 800-MeV proton radiography facility for dynamic experiments

N. S. P. King; E. Ables; Kenneth J. Adams; K.R Alrick; J.F. Amann; Stephen Balzar; P.D Barnes; M.L Crow; S.B Cushing; J.C Eddleman; T.T Fife; Paul Flores; D Fujino; R.A Gallegos; N.T Gray; E.P Hartouni; Gary E. Hogan; Vanner H. Holmes; Steven A. Jaramillo; J.N Knudsson; R.K London; R.R Lopez; T.E McDonald; J.B. McClelland; F. E. Merrill; Kevin Bruce Morley; C. L. Morris; F.J Naivar; E.L Parker; Hae-Sim Park

The capability has been successfully developed at the Los Alamos Nuclear Science Center (LANSCE) to utilize a spatially and temporally prepared 800-MeV proton beam to produce proton radiographs. A series of proton bursts are transmitted through a dynamically varying object and transported, via a unique magnetic lens system, to an image plane. The magnetic lens system permits correcting for the effects of multiple coulomb scattering which would otherwise completely blur the spatially transmitted information at the image plane. The proton radiographs are recorded on either a time integrating film plate or with a recently developed multi-frame electronic imaging camera system. The latter technique permits obtaining a time dependent series of proton radiographs with time intervals (modulo 358 ns) up to many microseconds and variable time intervals between images. One electronically shuttered, intensified, CCD camera is required per image. These cameras can detect single protons interacting with a scintillating fiber optic array in the image plane but also have a dynamic range which permits recording radiographs with better than 5% statistics for observation of detailed density variations in the object. A number of tests have been carried out to characterize the quality of the proton radiography system for absolute mass determination, resolution, and dynamic range. Initial dynamic experiments characterized the temporal and spatial behavior of shock propagation in high explosives with up to six images per experiment. Based on experience with the prototype system, a number of upgrades are being implemented including the anticipated capability for enhanced mass discrimination through differential multiple coulomb scattering radiographs and more images with improved imaging techniques.


Physical Review D | 2002

Search for the lepton family number nonconserving decay mu+ ---> e+ gamma

M. Ahmed; J. F. Amann; D. Barlow; K. Black; Richard D. Bolton; M. Brooks; Staffan Carius; Y. Chen; A. Chernyshev; H. M. Concannon; M. D. Cooper; Peter S. Cooper; J. Crocker; J. R. Dittmann; M. Dzemidzic; A. Empl; R. J. Fisk; E. Fleet; W. Foreman; Carl A. Gagliardi; D. Haim; A. Hallin; C. M. Hoffman; Gary E. Hogan; E. B. Hughes; Ed V. Hungerford; C. Jui; G. J. Kim; J. E. Knott; D. D. Koetke

The MEGA experiment, which searched for the muon- and electron-number violating decay μ +→e + γ, is described. The spectrometer system, the calibrations, the data taking procedures, the data analysis, and the sensitivity of the experiment are discussed. The most stringent upper limit on the branching ratio, B(μ + →e + γ)l1.2×10 -11 with 90% confidence, is derived from a likelihood analysis.


Science & Global Security | 2008

Tomographic Imaging with Cosmic Ray Muons

C. L. Morris; C. C. Alexander; Jeffrey Bacon; Konstantin N. Borozdin; D. J. Clark; R. Chartrand; C. J. Espinoza; Andrew M. Fraser; M. Galassi; J. A. Green; J. S. Gonzales; John J. Gomez; Nicolas W. Hengartner; Gary E. Hogan; Alexei V. Klimenko; M. Makela; P. McGaughey; J. Medina; F.E. Pazuchanics; William C. Priedhorsky; J. C. Ramsey; A. Saunders; R. C. Schirato; Larry J. Schultz; Michael James Sossong; G. S. Blanpied

Over 120 million vehicles enter the United States each year. Many are capable of transporting hidden nuclear weapons or nuclear material. Currently deployed X-ray radiography systems are limited because they cannot be used on occupied vehicles and the energy and dose are too low to penetrate many cargos. We present a new technique that overcomes these limitations by obtaining tomographic images using the multiple scattering of cosmic radiation as it transits each vehicle. When coupled with passive radiation detection, muon interrogation could contribute to safe and robust border protection against nuclear devices or material in occupied vehicles and containers.


Review of Scientific Instruments | 2003

Detection of high-Z objects using multiple scattering of cosmic ray muons

William C. Priedhorsky; Konstantin N. Borozdin; Gary E. Hogan; C. L. Morris; A. Saunders; Larry J. Schultz; Margaret E. Teasdale

We demonstrate that high-Z material can be detected and located in three dimensions using radiographs formed by cosmic-ray muons. Detection of high-Z material hidden inside large volume of ordinary cargo is an important and timely task given the danger associated with illegal transport of uranium and heavier elements. Existing radiography techniques are inefficient for shielded material, often expensive and involve radiation hazards, real and perceived. We recently demonstrated that radiographs can be formed using cosmic-ray muons [K. N. Borozdin et al., Nature (London) 422, 277 (2003)]. Here, we show that compact, high-Z objects can be detected and located in three dimensions with muon radiography. The natural flux of cosmic-ray muons [P. K. F. Grieder, Cosmic Rays at Earth (Elsevier, New York, 2001)], approximately 10 000 m−2 min−1, can form useful images in ∼1 min, using large-area muon detectors like those used in high-energy physics.


Physical Review Letters | 2002

Measurements of ultracold-neutron lifetimes in solid deuterium.

C. L. Morris; Juan-Manuel Anaya; T. J. Bowles; B. W. Filippone; P. Geltenbort; R. Hill; Masahiro Hino; Seth Hoedl; Gary E. Hogan; Takeo Ito; T. Kawai; K. Kirch; S. K. Lamoreaux; C.-Y. Liu; M. Makela; L.J. Marek; Jonathan W. Martin; R.N. Mortensen; A. Pichlmaier; A. Saunders; S. J. Seestrom; D. Smith; W. A. Teasdale; Brian Tipton; Masahiko Utsuro; A. R. Young; Junhua Yuan

We present the first measurements of the survival time of ultracold neutrons (UCNs) in solid deuterium (SD2). This critical parameter provides a fundamental limitation to the effectiveness of superthermal UCN sources that utilize solid ortho-deuterium as the source material. These measurements are performed utilizing a SD2 source coupled to a spallation source of neutrons, providing a demonstration of UCN production in this geometry and permitting systematic studies of the influence of thermal up-scatter and contamination with para-deuterium on the UCN survival time.


SHOCK COMPRESSION OF CONDENSED MATTER - 2003: Proceedings of the Conference of the American Physical Society Topical Group on Shock Compression of Condensed Matter | 2004

A Survey of High Explosive‐Induced Damage and Spall in Selected Metals Using Proton Radiography

D. B. Holtkamp; D. A. Clark; Eric N. Ferm; R. A. Gallegos; D. Hammon; W. F. Hemsing; Gary E. Hogan; V. H. Holmes; N. S. P. King; R. P. Liljestrand; R. P. Lopez; F. E. Merrill; C. L. Morris; Kevin Bruce Morley; M. M. Murray; Peter Pazuchanics; Kathy Prestridge; John P. Quintana; A. Saunders; T. Schafer; M. A. Shinas; H. L. Stacy

Multiple spall and damage layers can be created in metal when the free surface reflects a Taylor wave generated by high explosives. These phenomena have been explored in different thicknesses of several metals (tantalum, copper, 6061 T6‐aluminum, and tin) using high‐energy proton radiography. Multiple images (up to 21) can be produced of the dynamic evolution of damaged material on the microsecond time scale with a <50 ns “shutter” time. Movies and multiframe still images of areal and (Abel inverted) volume densities are presented. An example of material that is likely melted on release (tin) is also presented.


Intersections between particle and nuclear physics | 1997

Lepton flavor violation

Cooper, M.D. Brooks, M.; Gary E. Hogan

The connection of rare decays to supersymmetric grand unification is highlighted, and a review of the status of rare decay experiments is given. Plans for future investigations of processes that violate lepton flavor are discussed. A new result from the MEGA experiment, a search for {mu}{sup +} {yields} e{sup +} {gamma}, is reported to be B.R. < 3.8 x 10{sup -11} with 90% confidence.


Review of Scientific Instruments | 2011

Magnifying lens for 800 MeV proton radiography

F. E. Merrill; E. Campos; Camilo Espinoza; Gary E. Hogan; Brian J. Hollander; J. Lopez; F. G. Mariam; Deborah Jean Morley; C. L. Morris; Matthew Murray; A. Saunders; C. Schwartz; T. N. Thompson

This article describes the design and performance of a magnifying magnetic-lens system designed, built, and commissioned at the Los Alamos National Laboratory (LANL) for 800 MeV flash proton radiography. The technique of flash proton radiography has been developed at LANL to study material properties under dynamic loading conditions through the analysis of time sequences of proton radiographs. The requirements of this growing experimental program have resulted in the need for improvements in spatial radiographic resolution. To meet these needs, a new magnetic lens system, consisting of four permanent magnet quadrupoles, has been developed. This new lens system was designed to reduce the second order chromatic aberrations, the dominant source of image blur in 800 MeV proton radiography, as well as magnifying the image to reduce the blur contribution from the detector and camera systems. The recently commissioned lens system performed as designed, providing nearly a factor of three improvement in radiographic resolution.


Review of Scientific Instruments | 2013

Performance of the Los Alamos National Laboratory spallation-driven solid-deuterium ultra-cold neutron source

A. Saunders; M. Makela; Y. Bagdasarova; H. O. Back; J. G. Boissevain; L. J. Broussard; T. J. Bowles; R. Carr; S. Currie; B. W. Filippone; Antonio Garcia; P. Geltenbort; K. P. Hickerson; Roger E. Hill; J. Hoagland; Seth Hoedl; A. T. Holley; Gary E. Hogan; Takeyasu M. Ito; S. K. Lamoreaux; Chen-Yu Liu; J. Liu; R. R. Mammei; Jeffrey William Martin; D. Melconian; M. P. Mendenhall; C. L. Morris; R. Mortensen; R. W. Pattie; M. L. Pitt

In this paper, we describe the performance of the Los Alamos spallation-driven solid-deuterium ultra-cold neutron (UCN) source. Measurements of the cold neutron flux, the very low energy neutron production rate, and the UCN rates and density at the exit from the biological shield are presented and compared to Monte Carlo predictions. The cold neutron rates compare well with predictions from the Monte Carlo code MCNPX and the UCN rates agree with our custom UCN Monte Carlo code. The source is shown to perform as modeled. The maximum delivered UCN density at the exit from the biological shield is 52(9) UCN/cc with a solid deuterium volume of ~1500 cm(3).

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A. Saunders

Los Alamos National Laboratory

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C. L. Morris

Los Alamos National Laboratory

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T. J. Bowles

Los Alamos National Laboratory

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M. Makela

Los Alamos National Laboratory

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S. J. Seestrom

Los Alamos National Laboratory

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Takeyasu M. Ito

Los Alamos National Laboratory

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F. G. Mariam

Los Alamos National Laboratory

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B. W. Filippone

California Institute of Technology

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Anatolii P. Serebrov

Petersburg Nuclear Physics Institute

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