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I Chesnick, T Todorov, J M. Centeno, Dale Newbury, John A. Small, K Potter
Paramagnetic manganese (II) can be employed as a calcium surrogate to enhance the sensitivity of the magnetic resonance microscopy (MRM) technique to the processing of calcium during the bone formation process. At high doses, osteoblasts can take up
Robert A. Fletcher, Nicholas W. Ritchie, Ian M. Anderson, John A. Small
This chapter describes microscopy and microanalysis techniques used for the characterization of collected, individual particles in a variety of instruments. The instruments discussed are the light microscope, electron microscopes (both scanning and
Ryna B. Marinenko, Shirley Turner, David S. Simons, Savelas A. Rabb, Rolf L. Zeisler, Lee L. Yu, Dale E. Newbury, Rick L. Paul, Nicholas W. Ritchie, Stefan D. Leigh, Michael R. Winchester, Lee J. Richter, Douglas C. Meier, Keana C. Scott, D Klinedinst, John A. Small
Bulk SiGe wafers cut from single-crystal boules and two SiGe thick films (4 m and 5 m thick) on Si wafers were evaluated with the electron probe microanalyzer for the extent of heterogeneity and composition for use as reference materials needed by the
Ryna B. Marinenko, Shirley Turner, Dale E. Newbury, Robert L. Myklebust, Lee L. Yu, Rolf L. Zeisler, David S. Simons, John A. Small
Bulk SiGe wafers cut from single-crystal boules and SiGe thick films on Si wafers were evaluated with the electron probe microanalyzer for the extent of heterogeneity and composition for use as reference standards needed by the microelectronics industry in
Dianne L. Poster, John A. Small, Michael T. Postek
The National Nanotechnology Initiative (NNI) in its 2006 document, Environmental, Health, and Safety Research Needs for Engineered Nanoscale Materials (available at www.nano.gov), identifies standards and standard measurement protocols as a critical
John G. Gillen, J Batteas, Chris A. Michaels, P Chi, John A. Small, Eric S. Windsor, Albert J. Fahey, Jennifer R. Verkouteren, W Kim
A C60+ primary ion source has been coupled to an ion microscope SIMS instrument to examine sputtering of silicon with an emphasis on possible application of C60+ depth profiling for high depth resolution SIMS analysis of silicon semiconductor materials
Dale E. Newbury, Kent D. Irwin, Gene C. Hilton, David A. Wollman, John A. Small, John M. Martinis
Electron probe x-ray microanalysis is based upon the use of a focused, high current density electron beam, 5 keV to 30 keV in energy, to excite characteristic x-rays from a picogram mass of a solid target. X-ray spectral measurements are currently
Dale E. Newbury, J H. Scott, Scott A. Wight, J T. Armstrong, John A. Small
Transmission (TEM) and scanning electron microscopes (SEM) provide ideal platforms for electron and x-ray spectrometry to characterize nanoscale particles and nanostructured bulk materials. Electron spectrometry includes electron energy loss spectrometry
John A. Small, Dale Newbury, John Henry J. Scott, L. King, Sae Woo Nam, Kent D. Irwin, Steven Deiker, Shaul Barkan, Jan Iwanczyk
NIST, Gaithersburg has recently installed a first generation silicon drift detector (SDD) from Photon Imaging and the NIST Boulder microcalorimeter energy dispersive x-ray spectrometer (υcal-EDS) on a JEOL 840 SEM, as shown in Fig. 1. [1,2] The instrument
John A. Small, Dale E. Newbury, J H. Scott, L R. King, Sae Woo Nam, Kent D. Irwin, Steven Deiker, S Barkan, E Iwaniczko
NIST, Gaithersburg has recently installed a first generation silicon drift dectector (SDD) from Photon Imaging and the NIST Boulder microcalorimeter energy dispersive x-ray spectrometer ( cal-EDS) on a JEOL 840 SEM1 , as shown in Fig.1. [1,2] The
In recent years, there have been a series of advancements in electron beam instruments and x-ray detectors which may make it possible to improve significantly the quality of results from the quantitative electron-probe analysis of individual particles
Kent D. Irwin, James A. Beall, Steven Deiker, Gene C. Hilton, L. King, Sae Woo Nam, Dale Newbury, Carl D. Reintsema, John A. Small, Leila R. Vale
High-energy-resolution cryogenic microcalorimeters are a powerful new tool for x-ray microanalysis. With demonstrated energy resolution 20 times better than with conventional semiconductor EDS, microcalorimeters are useful in applications such as nanoscale
Over the years several different methods have been developed for the quantitative x-ray microanalysis of individual particles Small (1981), Armstrong (1991). Despite the large number of quantitative methods available, the accuracy for the x-ray
Dale E. Newbury, David A. Wollman, Sae Woo Nam, Gene C. Hilton, Kent D. Irwin, John A. Small, John M. Martinis
Analytical x-ray spectrometry for electron beam instruments has been significantly advanced with the development of the NIST microcalorimeter energy dispersive x-ray spectrometer (mcal EDS). The mcal EDS operates by measuring the temperature rise when a
In this study, we investigated the relative contributions of automic number (Z) and density (p) to the degradation of the electron backscatter diffraction (EBSD) pattern quality for nanoparticles 2O 3 particles approximately 200 nm in diameter mounted on
In recent years, field-emission gun scanning electron microscopes, FEG-SEMs, with high-brightness electron guns and excellent performance at low electron beam energies (E 0 less then or equal to 5 keV) have become readily available. Concurrently the
This chapter describes microscopes and microprobes used for analysis of collected, individual particles. The instruments discussed are the light microscope, electron microscopes (scanning, environmental and transmission), electron microprobes, laser
Recently, an electron backscatter diffraction (EBSD) system was developed that uses a 1024 x 1024 CCD camera coupled to a thin phosper. This camera has been shown to produce excellent EBSD patterns. In this system, crystallographic information is
Recently, an electron backscatter diffraction EBSD system was developed that uses a 1024 x 1024 CCD camera coupled to a thin scintillator rather than photographic film. In this system, crystallagraphic information is determined and coupled with the
In January of 1992 the ISO Council announced the acceptance of resolution 50/1991 establishing TC202 Microbeam Analysis. The China State Bureau of Technology Supervision (CSBTS) was appointed by the ISO council as secretariat of TC 202 and remains in this
The energy of the electron beam, in conventional electron probe microanalysis, is generally in the range of 15-25 keV which provides the necessary overvoltage to excite efficiently the K and L x-ray lines for elements with atomic numbers in the range of