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Dive into the research topics where Steven C. Bender is active.

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Featured researches published by Steven C. Bender.


IEEE Journal of Quantum Electronics | 2009

Demonstration of Bias-Controlled Algorithmic Tuning of Quantum Dots in a Well (DWELL) MidIR Detectors

Woo-Yong Jang; Majeed M. Hayat; J.S. Tyo; R. S. Attaluri; Thomas E. Vandervelde; Y. D. Sharma; R. V. Shenoi; A. Stintz; E.R. Cantwell; Steven C. Bender; Sang Jun Lee; Sam Kyu Noh; Sanjay Krishna

The quantum-confined Stark effect in intersublevel transitions present in quantum-dots-in-a-well (DWELL) detectors gives rise to a midIR spectral response that is dependent upon the detectors operational bias. The spectral responses resulting from different biases exhibit spectral shifts, albeit with significant spectral overlap. A postprocessing algorithm was developed by Sakoglu that exploited this bias-dependent spectral diversity to predict the continuous and arbitrary tunability of the DWELL detector within certain limits. This paper focuses on the experimental demonstration of the DWELL-based spectral tuning algorithm. It is shown experimentally that it is possible to reconstruct the spectral content of a target electronically without using any dispersive optical elements for tuning, thereby demonstrating a DWELL-based algorithmic spectrometer. The effects of dark current, detector temperature, and bias selection on the tuning capability are also investigated experimentally.


IEEE Journal of Quantum Electronics | 1991

Experimental results from the Los Alamos FEL photoinjector

Donald W. Feldman; Steven C. Bender; Bruce E. Carlsten; J. Early; R.B. Feldman; W.J.D. Johnson; A.H. Lumpkin; P.G. O'Shea; W.E. Stein; Richard L. Sheffield; L.M. Young

The authors report some initial measurements of electron beam properties from the new photoinjector installed as the front end on the Los Alamos free-electron laser (FEL). The FEL is being rebuilt with the photoinjector, added acceleration to 40 MeV, new diagnostics, and a beam line designed to minimize emittance growth. The authors measured the spatial and temporal properties of the beam at energies of about 15 MeV as a function of several parameters and the results have been compared to simulations. The operational characteristics of the important elements of the system and the theoretical comparisons are described. >


SPIE's International Symposium on Optical Science, Engineering, and Instrumentation | 1999

Multispectral Thermal Imager mission overview

Paul G. Weber; Brian C. Brock; Alfred J. Garrett; Barham W. Smith; Christoph C. Borel; William B. Clodius; Steven C. Bender; R. Rex Kay; Max L. Decker

The Multispectral Thermal Imager (MTI) is a research and development project sponsored by the Department of Energy and executed by Sandia and Los Alamos National Laboratories and the Savannah River Technology Center. Other participants include the U.S. Air Force, universities, and many industrial partners. The MTI mission is to demonstrate the efficacy of highly accurate multispectral imaging for passive characterization of industrial facilities and related environmental impacts from space. MTI provides simultaneous data for atmospheric characterization at high spatial resolution. Additionally, MTI has applications to environmental monitoring and other civilian applications. The mission is based in end-to-end modeling of targets, signatures, atmospheric effects, the space sensor, and analysis techniques to form a balanced, self-consistent mission. The MTI satellite nears completion, and is scheduled for launch in late 1999. This paper describes the MTI mission, development of desired system attributes, some trade studies, schedule, and overall plans for data acquisition and analysis. This effort drives the sophisticated payload and advanced calibration systems, which are the overall subject of the first session at this conference, as well as the data processing and some of the analysis tools that will be described in the second segment.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1994

Demonstration of ultraviolet lasing with a low energy electron beam

P.G. O'Shea; Steven C. Bender; Donald A. Byrd; James W. Early; Donald W. Feldman; Clifford M. Fortgang; John C. Goldstein; Brian E. Newnam; Richard L. Sheffield; R.W. Warren; T. Zaugg

Abstract We report on the design details of the first ultraviolet (UV) free-electron laser (FEL) oscillator driven by low-energy electrons from a radio-frequency linear accelerator. In our experiment we used a high-current, high brightness electron beam in combination with a wiggler of novel design to produce an FEL that lased at wavelengths from 369 to 380 nm using 45.9–45.2 MeV electrons. In addition we performed a proof-of-principle experiment that demonstrated the first ever photolithography on a photoresist-coated silicon wafer using an FEL light source.


Sensors, Systems, and Next-Generation Satellites VI | 2003

On-orbit radiometric calibration over time and between spacecraft using the Moon

Hugh H. Kieffer; Thomas C. Stone; Robert A. Barnes; Steven C. Bender; Robert E. Eplee; Jeffrey A. Mendenhall; Lawrence Ong

The Robotic Lunar Observatory (ROLO) project has developed a spectral irradiance model of the Moon that accounts for variations with lunar phase through the bright half of a month, lunar librations, and the location of an Earth-orbiting spacecraft. The methodology of comparing spacecraft observations of the Moon with this model has been developed to a set of standardized procedures so that comparisons can be readily made. In the cases where observations extend over several years (e.g., SeaWiFS), instrument response degradation has been determined with precision of about 0.1% per year. Because of the strong dependence of lunar irradiance on geometric angles, observations by two spacecraft cannot be directly compared unless acquired at the same time and location. Rather, the lunar irradiance based on each spacecraft instrument calibration can be compared with the lunar irradiance model. Even single observations by an instrument allow inter-comparison of its radiometric scale with other instruments participating in the lunar calibration program. Observations by SeaWiFS, ALI, Hyperion and MTI are compared here.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1992

Initial results from the Los Alamos photoinjector-driven free-electron laser☆

P.G. O'Shea; Steven C. Bender; Donald A. Byrd; Bruce E. Carlsten; James W. Early; Donald W. Feldman; R.B. Feldman; W.J.D. Johnson; A.H. Lumpkin; Mark J. Schmitt; R.W. Springer; W.E. Stein; T. Zaugg

Abstract We report initial results on the APEX (APLE prototype experiment) photoinjector-driven infrared free-electron laser (FEL). The APEX FEL is operating in support of a Boeing Aerospace and Electronics/Los Alamos National Laboratory collaboration to build the average power laser experiment (APLE). Our system uses a high quantum efficiency (3–7%) multi-alkali photocathode, illuminated with a frequency-doubled Nd:YLF mode locked laser at 21.7 MHz. The photocathode is located in this first cell of a six-cell 1.3 GHz, 6 MeV photoinjector that feeds a linac with a final energy up to 40 MeV. Because the illuminating laser pulse on our photocathode is short (10 ps), no pulse compression is required in the linac. Emittance measurements made after the second linac tank at 15 MeV have shown that a normalized emittance (for 90% of the particles) of less than 50π mm mrad can be achieved at a peak micropulse current of 300 A. Our initial lasing has been at a wavelength of 3.6 μm over a 30 μs macropulse with an electron beam energy of 35 MeV and a 2.7 cm period permanent magnet wiggler. We are continuing to characterize and optimize our system, with particular emphasis on understanding and minimizing electron beam emittance-growth mechanisms, and subsequently improving the quality of the beam delivered to the wiggler.


SPIE's International Symposium on Optical Science, Engineering, and Instrumentation | 1999

Multispectral Thermal Imager (MTI) Payload Overview

Steven C. Bender; Brian C. Brock; D.M. Bullington; D.A. Byrd; P.J. Claassen; Max L. Decker; T.D. Henson; R. Rex Kay; R.E. Kidner; C.E. Lanes; C. Little; K.D. Marbach; N.G. Rackley; Jeffrey L. Rienstra; Barham W. Smith; R.B. Taplin; Paul G. Weber

MTI is a comprehensive research and development project that includes up-front modeling and analysis, satellite system design, fabrication, assembly and testing, on-orbit operations, and experimentation and data analysis. The satellite is designed to collect radiometrically calibrated, medium resolution imagery in 15 spectral bands ranging from 0.45 to 10.70 micrometer. The payload portion of the satellite includes the imaging system components, associated electronics boxes, and payload support structure. The imaging system includes a three-mirror anastigmatic off-axis telescope, a single cryogenically cooled focal plane assembly, a mechanical cooler, and an onboard calibration system. Payload electronic subsystems include image digitizers, real-time image compressors, a solid state recorder, calibration source drivers, and cooler temperature and vibration controllers. The payload support structure mechanically integrates all payload components and provides a simple four point interface to the spacecraft bus. All payload components have been fabricated and tested, and integrated.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1991

Performance of the Los Alamos HIBAF accelerator at 17 MeV

Donald W. Feldman; Steven C. Bender; Bruce E. Carlsten; James W. Early; R.B. Feldman; W.J.D. Johnson; A.H. Lumpkin; P.G. O'Shea; W.E. Stein; Richard L. Sheffield; K.F. McKenna

Abstract The Los Alamos free electron laser (FEL) is being rebuilt with a photoelectric injector and 40 MeV beam energy for a lower emittance, brighter beam. Tests of the Los Alamos high-brightness accelerator FEL (HIBAF) system have been conducted including the photoinjector and first 17 MeV of acceleration. The photoinjector is designed to operate with a micropulse charge of 5 nC, peak current of 300 A. energy spread of 0.3%, and emittance of 50π mm mrad. Measurements of temporal and spatial beam characteristics have been made up to 10 nC per micropulse for both single micropulses and macropulses. The operational characteristics of the system components, e.g., drive laser and photoinjector are described. The results of beam and rf measurements are briefly presented and compared to simulation. The effects of nonaxially symmetric rf fields in the on axis coupled accelerator structure were observed and are discussed.


International Journal of Remote Sensing | 2003

Deployment test of the NIST EOS Thermal-infrared Transfer Radiometer

Joseph P. Rice; Steven C. Bender; William H. Atkins; F. J. Lovas

The National Institute of Standards and Technology (NIST) Thermal-infrared Transfer Radiometer (TXR), developed for the National Aeronautics and Space Administration (NASA) Earth Observing System (EOS), was deployed at the remote sensing radiometric calibration facility at Los Alamos National Laboratory (LANL). The purpose of the deployment was to test the ability of the TXR to operate off-site of NIST in a host cryogenic vacuum chamber, and to provide an end-to-end verification of the radiance scale in the LANL facility. The TXR was calibrated pre-trip and post-trip at NIST against a water bath black body in ambient conditions. At LANL, the TXR was operated in a liquid nitrogen cooled vacuum chamber, mounted in the same position that remote sensing instruments occupy during their pre-flight calibrations. The results from the TXR 5 µm channel show that the LANL radiance scale agrees with that of the NIST water bath black body to within a radiance uncertainty of - 0.16% ( k = 2). This corresponds to a brightness temperature uncertainty of 50 mK ( k = 2) at 300 K. Thus, the TXR has demonstrated its ability to provide an economical end-to-end system-level verification of the component-level radiometric scale assigned to a calibration facility. Such verifications provide an extra level of confidence in the radiometric accuracy of flight instrument calibration facilities that has hitherto not been possible.


Applied Spectroscopy | 2014

Planetary Geochemical Investigations Using Raman and Laser-Induced Breakdown Spectroscopy

Samuel Michael Clegg; Roger C. Wiens; Anupam K. Misra; Shiv K. Sharma; James L. Lambert; Steven C. Bender; Raymond Thorson Newell; Kristy Nowak-Lovato; Sue Smrekar; M. Darby Dyar; S. Maurice

An integrated Raman spectroscopy and laser-induced breakdown spectroscopy (LIBS) instrument is a valuable geoanalytical tool for future planetary missions to Mars, Venus, and elsewhere. The ChemCam instrument operating on the Mars Curiosity rover includes a remote LIBS instrument. An integrated Raman-LIBS spectrometer (RLS) based on the ChemCam architecture could be used as a reconnaissance tool for other contact instruments as well as a primary science instrument capable of quantitative mineralogical and geochemical analyses. Replacing one of the ChemCam spectrometers with a miniature transmission spectrometer enables a Raman spectroscopy mineralogical analysis to be performed, complementing the LIBS chemical analysis while retaining an overall architecture resembling ChemCam. A prototype transmission spectrometer was used to record Raman spectra under both Martian and Venus conditions. Two different high-pressure and high-temperature cells were used to collect the Raman and LIBS spectra to simulate surface conditions on Venus. The resulting LIBS spectra were used to generate a limited partial least squares Venus calibration model for the major elements. These experiments demonstrate the utility and feasibility of a combined RLS instrument.

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A.H. Lumpkin

Los Alamos National Laboratory

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Donald A. Byrd

Los Alamos National Laboratory

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Brian D. McVey

Los Alamos National Laboratory

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John C. Goldstein

Los Alamos National Laboratory

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W.E. Stein

Los Alamos National Laboratory

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Bruce E. Carlsten

Los Alamos National Laboratory

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Richard L. Sheffield

Los Alamos National Laboratory

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James W. Early

Los Alamos National Laboratory

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