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National synchrotron light source

National Synchrotron Light Source User s Manual Guide to the VUVandX-Ray Beam Lines. (N. F. Gmur ed.) BNL informal report no. 45764, 1991. [Pg.226]

National Synchrotron Light Source (NSLS) at Brookhaven National Laboratory (BNL). [Pg.358]

This research has been funded by the Donors of the Petroleum Research Fund (ACS, grant 28336-G5) and by the National Science Foundation (CTS-940618). Support from the Layman Fund and the Research Council at the University of Nebraska is so acknowledged. We thank the National Synchrotron Light Source and the Stanford Synchrotron Radiation Laboratory for X-ray beamtime. [Pg.551]

In situ XRD spectra were collected on beam line X18A at the National Synchrotron Light Source (NSLS) located at Brookhaven National Laboratory (BNL). The X-ray wavelength (X) was 1.195 A. The step size of the 29 scan was 0.02° in the regions with Bragg reflections and 0.05° in the regions without reflections. The XRD spectra were collected in the transmission mode (Liu et al., 2004). [Pg.472]

Spectroscopic evaluation of the catalysts. The UV-Vis spectra of the Jacobsen Co-salen catalysts were collected in the transmission mode on a CARY-3E UV-Vis spectrophotometer by dissolving the catalysts in epichlorohydria The Co K-edge (7709 eV) X-ray absorption near edge stracture, XANES, of Jacobsen s Co-salen catalyst was collected during the HKR reaction at beamline XIO-C at National Synchrotron Light Source (NSLS), Brookhaven National Lab, Upton, NY. [Pg.392]

This effort was funded by the National Aeronautics and Space Administration (NASA) Grant NNX07AB93A under a project entitled Basic Studies for the Production and Upgrading of Fischer-Tropsch Synthesis Products to Fuels and the Commonwealth of Kentucky. This research was carried out, in part, at the National Synchrotron Light Source, Brookhaven National Laboratory, which is supported by the U.S. DOE, Divisions of Materials Science and Chemical Sciences. Special thanks to Dr. Nebojsa Marinkovic (Beamline X18b, NSLS, Brookhaven) for help with X AFS studies and Joel Young (University of Oklahoma, Department of Physics) for XAFS cell construction. [Pg.163]

National Synchrotron Light Source Brookhaven National Laboratory Upton, New York... [Pg.427]

A number of synchrotrons (including the National Synchrotron Light Source, New York, the Advanced Light Source, Berkley, and soon the Canadian Light Source, Saskatoon) operate mail-in crystallography services where a scientist can mail in crystals (prefrozen and mounted on loops) and data will be collected, processed (sometimes), and returned. This is becoming a method of choice, as it eliminates the need to travel to a synchrotron and speeds up the data collection procedure at the synchrotron also. [Pg.472]

The NEXAFS experiments were carried out on the U7A NIST/Dow Materials Soft X-ray Materials Characterization Facility at the National Synchrotron Light Source at Brookhaven National Laboratory (NSLS BNL)... [Pg.121]

The NEXAFS experiments reported here were carried out at the U1 Beamline of the National Synchrotron Light Source, Brookhaven National Laboratory. Details concerning the optics of the beamline, as well as the UHV chamber with facilities for high pressure reactions, have been described previously.7,8 In our experimental set-up, NEXAFS spectra can be recorded by measuring either the electron yield or fluorescence yield. While the electron yield method is sensitive only to the top few atomic... [Pg.233]

Figure 17.4. Schematic of a scanning transmission X-ray microscope. This setup uses soft X rays (250-800 eV) from an undulator on beamline XIA of the National Synchrotron Light Source in Brookhaven National Laboratory, Upton, NY. Figure 17.4. Schematic of a scanning transmission X-ray microscope. This setup uses soft X rays (250-800 eV) from an undulator on beamline XIA of the National Synchrotron Light Source in Brookhaven National Laboratory, Upton, NY.
Figure 1.8 Example of the spectral flux Ny of the undulator/wiggler radiation measured at the X-Al beam line at NSLS (National Synchrotron Light Source, Brookhaven National Laboratory, LISA) with the undulator parameters K = 1.50, X = 8 cm, N = 35, for a 500 mA beam current, with a 0.1% bandpass and a solid angle of 1 mrad2. The values are corrected for the beamline/monochromator efficiency and the photodiode detector response the dip at 4.4 nm is an artifact due to carbon contamination of the optical elements. From [BRA89], (Reproduced with permission from Review of Scientific Instruments.)... Figure 1.8 Example of the spectral flux Ny of the undulator/wiggler radiation measured at the X-Al beam line at NSLS (National Synchrotron Light Source, Brookhaven National Laboratory, LISA) with the undulator parameters K = 1.50, X = 8 cm, N = 35, for a 500 mA beam current, with a 0.1% bandpass and a solid angle of 1 mrad2. The values are corrected for the beamline/monochromator efficiency and the photodiode detector response the dip at 4.4 nm is an artifact due to carbon contamination of the optical elements. From [BRA89], (Reproduced with permission from Review of Scientific Instruments.)...
Dr G. Larry Carr National Synchrotron Light Source (NSLS), Brookhaven National Laboratory, 75 Brookhaven Avenue, Bldg 725B, Upton, NY 11973-5000, USA... [Pg.321]

For the studies presented in Sections IV and V, measurements were taken at IBM Beamline U8B (12) at the National Synchrotron Light Source. Monochromator energy resolution at the carbon K-edge was 0.2 eV. A display analyzer (13) with channel plates was used to detect secondary electrons in an 8 eV window centered at 42 eV. This energy was selected so that only the most surface-sensitive (minimum escape depth) electrons were detected. [Pg.39]

The metal-polymer studies were done in collaboration with C.A. Kovac, M.J. Goldberg, J.F. Morar and R.A. Poliak. The polymer-metal studies were done in collaboration with S.P. Kowalczyk. I wish to thank J. Stohr and A. Hitchcock for many enlightening discussions on NEXAFS techniques and interpretation and for timely access to their data throughout the course of these studies. Research was carried out in part at the National Synchrotron Light Source, Brookhaven National Laboratory, which is supported by the U.S. Department of Energy, Division of Materials Sciences and Division of Chemical Sciences. [Pg.45]

National Synchrotron Light Source at Brookhaven National Laboratory. With data such as these, structural research efforts are bolstered significantly and, as was mentioned at the beginning of this discussion, knowledge of the atomic positions in space is of immense value in the characterization of a material. [Pg.303]


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See also in sourсe #XX -- [ Pg.289 ]

See also in sourсe #XX -- [ Pg.323 ]




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Light sources

National Synchrotron Light Source at Brookhaven

Source synchrotron

Synchrotrons

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