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Dive into the research topics where William T. Buttler is active.

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Featured researches published by William T. Buttler.


Physical Review Letters | 1998

Practical Free-Space Quantum Key Distribution over 1 km

William T. Buttler; Richard Hughes; Paul G. Kwiat; S. K. Lamoreaux; Gabriel G. Luther; G. L. Morgan; Jane E. Nordholt; Charles G. Peterson; Charles M. Simmons

A working free-space quantum key distribution system has been developed and tested over an outdoor optical path of {approximately}1 km at Los Alamos National Laboratory under nighttime conditions. Results show that free-space quantum key distribution can provide secure real-time key distribution between parties who have a need to communicate secretly. Finally, we examine the feasibility of surface to satellite quantum key distribution. {copyright} {ital 1998} {ital The American Physical Society}


Physical Review Letters | 2000

Daylight quantum key distribution over 1.6 km

William T. Buttler; Richard Hughes; S. K. Lamoreaux; G. L. Morgan; Jane E. Nordholt; C. G. Peterson

Quantum key distribution (QKD) has been demonstrated over a point-to-point 1.6-km atmospheric optical path in full daylight. This record transmission distance brings QKD a step closer to surface-to-satellite and other long-distance applications.


Journal of Applied Physics | 2007

Effects of shock-breakout pressure on ejection of micron-scale material from shocked tin surfaces

Michael Zellner; M. Grover; J. E. Hammerberg; R. S. Hixson; Adam Iverson; G. S. Macrum; K. B. Morley; A. W. Obst; R. T. Olson; J. R. Payton; P. A. Rigg; Nathan Routley; G. D. Stevens; W. D. Turley; L. R. Veeser; William T. Buttler

This effort investigates the relation between ejecta production and shock-breakout pressure (PSB) for Sn shocked with a Taylor shockwave (unsupported) to pressures near the solid-on-release/partial melt-on-release phase transition region. The shockwaves were created by detonation of high explosive (HE) PBX-9501 on the front side of Sn coupons. Ejecta production at the backside or free side of the Sn coupons was characterized through use of piezoelectric pins, optical shadowgraphy, x-ray attenuation radiography, and optical-heterodyne velocimetry. Ejecta velocities, dynamic volume densities, and areal densities were then correlated with the shock-breakout pressure of Sn surfaces characterized by roughness average of Ra=16 μin or Ra=32 μin.


Physical Review A | 1998

Free-space quantum-key distribution

William T. Buttler; Richard Hughes; Paul G. Kwiat; Gabriel G. Luther; G. L. Morgan; Jane E. Nordholt; Charles G. Peterson; Charles M. Simmons

Nonproliferation and International Security,Los Alamos, NM 87545(February 1, 2008)A working free-space quantum key distribution (QKD)system has been developed and tested over a 205-m indooroptical path at Los Alamos National Laboratory under fluo-rescent lighting conditions. Resultsshow that free-space QKDcan provide secure real-time key distribution between partieswho have a need to communicate secretly.PACS Numbers: 42.79.Sz, 03.65-w


Journal of Applied Physics | 2005

Piezoelectric characterization of ejecta from shocked tin surfaces

W. S. Vogan; William W. Anderson; M. Grover; J. E. Hammerberg; N. S. P. King; S. K. Lamoreaux; G. S. Macrum; K. B. Morley; P. A. Rigg; G. D. Stevens; W. D. Turley; L. R. Veeser; William T. Buttler

Using piezoelectric diagnostics, we have measured densities and velocities of ejected particulate as well as “free-surface velocities” of bulk tin targets shock loaded with high explosive. The targets had finely grooved, machined finishes ranging from 10 to 250μin. Two types of piezoelectric sensor (“piezopins”), lithium niobate and lead zirconate titanate, were compared for durability and repeatability; in addition, some piezopins were “shielded” with foam and metal foil in order to mitigate premature failure of the pins in high ejecta regimes. These experiments address questions about ejecta production at a given shock pressure as a function of surface finish; piezopin results are compared with those from complementary diagnostics such as x-ray radiography and time-resolved optical transmission techniques. The mass ejection shows a marked dependence on groove characteristics and cannot be described by a groove defect theory alone.


Journal of Applied Physics | 2008

Probing the underlying physics of ejecta production from shocked Sn samples

Michael Zellner; W. Vogan McNeil; J. E. Hammerberg; R. S. Hixson; A. W. Obst; R. T. Olson; J. R. Payton; P. A. Rigg; Nathan Routley; G. D. Stevens; W. D. Turley; L. R. Veeser; William T. Buttler

This effort investigates the underlying physics of ejecta production for high explosive (HE) shocked Sn surfaces prepared with finishes typical to those roughened by tool marks left from machining processes. To investigate the physical mechanisms of ejecta production, we compiled and re-examined ejecta data from two experimental campaigns [W. S. Vogan et al., J. Appl. Phys. 98, 113508 (1998); M. B. Zellner et al., ibid. 102, 013522 (2007)] to form a self-consistent data set spanning a large parameter space. In the first campaign, ejecta created upon shock release at the back side of HE shocked Sn samples were characterized for samples with varying surface finishes but at similar shock-breakout pressures PSB. In the second campaign, ejecta were characterized for HE shocked Sn samples with a constant surface finish but at varying PSB.


Journal of Applied Physics | 2012

Experimental study of ejecta from shock melted lead

Yongtao Chen; Haibo Hu; Tiegang Tang; Guowu Ren; Qingzhong Li; Rongbo Wang; William T. Buttler

This effort investigates the dynamic properties of ejecta from explosively shocked, melted Pb targets. The study shows that the ejecta cloud that expands beyond the shocked surface is characterized by a high density and low velocity fragment layer between the free-surface and the high velocity micro-jetting particle cloud. This slow, dense ejecta layer is liquid micro-spall. The properties of micro-spall layer, such as the mass, density and velocity, were diagnosed in a novel application of an Asay window, while micro-jetting particles by lithium niobate piezoelectric pins and high speed photography. The total mass-velocity distribution of ejecta, including micro-spall fragments and micro-jetting particles, is presented. Furthermore, the sensitivity of ejecta production to slight variations in the shockwave drive using the Asay foil is studied.


Journal of Applied Physics | 2007

Dynamic comparisons of piezoelectric ejecta diagnostics

William T. Buttler; Michael Zellner; R. T. Olson; P. A. Rigg; R. S. Hixson; J. E. Hammerberg; A. W. Obst; J. R. Payton; Adam Iverson; J. A. Young

We investigate the quantitative reliability and precision of three different piezoelectric technologies for measuring ejected areal mass from shocked surfaces. Specifically we performed ejecta measurements on Sn shocked at two pressures, P≈215 and 235 kbar. The shock in the Sn was created by launching a impactor with a powder gun. We self-compare and cross-compare these measurements to assess the ability of these probes to precisely determine the areal mass ejected from a shocked surface. We demonstrate the precision of each technology to be good, with variabilities on the order of ±10%. We also discuss their relative accuracy.


Journal of Applied Physics | 2014

Experimental observations on the links between surface perturbation parameters and shock-induced mass ejection

S. K. Monfared; D. Oro; M. Grover; J. E. Hammerberg; Brandon LaLone; C. L. Pack; M. M. Schauer; G. D. Stevens; Joseph B. Stone; W. D. Turley; William T. Buttler

We have assembled together our ejecta measurements from explosively shocked tin acquired over a period of about ten years. The tin was cast at 0.99995 purity, and all of the tin targets or samples were shocked to loading pressures of about 27 GPa, allowing meaningful comparisons. The collected data are markedly consistent, and because the total ejected mass scales linearly with the perturbations amplitudes they can be used to estimate how much total Sn mass will be ejected from explosively shocked Sn, at similar loading pressures, based on the surface perturbation parameters of wavelength and amplitude. Most of the data were collected from periodic isosceles shapes that approximate sinusoidal perturbations. Importantly, however, we find that not all periodic perturbations behave similarly. For example, we observed that sawtooth (right triangular) perturbations eject more mass than an isosceles perturbation of similar depth and wavelength, demonstrating that masses ejected from irregular shaped perturbatio...


Boundary-Layer Meteorology | 2001

Circulatory Patterns of Air Pollutants within the Barcelona Air Basin in a Summertime situation: Lidar and Numerical Approaches

Cecilia Soriano; José María Baldasano; William T. Buttler; K. R. Moore

This work examines circulatory patterns of airpollutants in the area of Barcelona (Spain), a regionwith strong coastal and orographic influences. Thiswas achieved through exploitation ofelastic-backscatter lidar data and by numericalsimulation of the atmosphere with a meteorologicalmesoscale model (MEMO). Lidar data were acquired inJuly 1992 during a collaborative campaign between LosAlamos National Laboratory (LANL) and the PolytechnicUniversity of Catalonia (UPC). The lidar providedinformation about the distribution of aerosols and theprevailing winds, determined by application of amaximum cross-correlation algorithm toelastic-backscatter lidar data. Lidar winds are usedto evaluate high altitude winds simulated by themodel. This study showed that circulatory patterns inBarcelona are correlated with daytime convectivevertical mixing, sea-breeze circulations, and verticalforcing caused by mountain thermal and mechanicaleffects.

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S. K. Lamoreaux

Los Alamos National Laboratory

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Jane E. Nordholt

Los Alamos National Laboratory

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G. D. Stevens

Los Alamos National Laboratory

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Richard Hughes

Los Alamos National Laboratory

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J. E. Hammerberg

Los Alamos National Laboratory

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Michael Zellner

Los Alamos National Laboratory

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P. A. Rigg

Los Alamos National Laboratory

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W. D. Turley

Los Alamos National Laboratory

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D. Oro

Los Alamos National Laboratory

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G. L. Morgan

Los Alamos National Laboratory

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