Radiation Laboratory

A unique high-energy radiation laboratory is functioning at the Institute, in which studies Can be performed and thick items can be controlled using powerful X-ray units and betatrons. 

W. E. Dunn, T. Vermeulen, C. R. Wilke, and T. T. Word, Report UCRL 10394 (1962), Univ. of California Radiation Laboratory as cited iu reference 4. 

H. Cheung, Critical Keview of Heat Pipe Theory and Applications, DCKT-50453, Lawrence Radiation Laboratory, University of California, Livermore, Calif., 1968. 

Bromley, L. A., Thermal Conductivity of Gases at Moder ate Pr essur es, University of California Radiation Laboratory, Report No. UCRL-1852, Berkeley, CA (1952). 

Lelevier, R. and Ragent, B., Lectures on Hydrodynamics and Shock Waves, Lawrence Radiation Laboratory, University of California Report No. UCRL-4333, Livermore, CA, 61 pp., April 1954. 

Wilkins, M. L. 1969. Calculation of elastic-plastic flow. Lawrence Radiation Laboratory report no. UCRL-7322 Rev. I. 

Kenneth S. Pitzer, Dean, College of Chemistry and Radiation Laboratory, University of California, Berkeley, California... 

Ref A. vonEgidy et al, A New Liquid Explosive, NTN , UCRL-5861, Lawrence Radiation Laboratory, Univ of Calif, Livermore (1960)... 

The x-ray measurements were made at the Stanford Synchrotron Radiation Laboratory which Is supported by DOE. 

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. 

We also found that in the field of materials science education, both education and work force needed considerable reorientation. For historical reasons (listed in the study) synthesis processing had been neglected at university and Government laboratories. We also looked at the debate about the role of a principal investigator versus large facilities, such as the synchrotron radiation laboratories. We concluded that materials science needs all of these different modes of research, and no particular approach is more decisively effective than another. 

Acknowledgement We are deeply indebted to Mr. Tadao Takada and Mrs. Sachiko Tojo who have contributed to the experiment. We also thank the members of the Radiation Laboratory of SANKEN, Osaka University, for running the linear accelerator. This work has been partly supported by a Grant-in-Aid for Scientific Research from the Ministry of Education, Science, Sport and Culture of Japan. 

Das Element 103 wurde zu Ehren des 1958 verstorbenen Direktors des Radiation Laboratory in Berkeley, Ernest O. Lawrence, als Lawrencium, Symbol Lw, bezeichnet. 

Howe, P.W., T. C. Parsons and L. E. Miles The Water Shielded Cave Facility for Totally Enclosed Master-Slave Operations at Lawrence Radiation Laboratory. Report UCRL-9657 (9- Okt. 1961). 

Hiskes, J. R. Tarter, C. B. Report UCRL-7088 Lawrence Radiation Laboratory Livermore CA, 1964. 

Division of Chemistry, National Research Council, Ottawa, Canada K1A 0R6 and Radiation Laboratory, University of Notre Dame, Notre Dame, IN 46556... 

Overview. Electrons orbiting in a magnetic field lose energy continually in the form of electromagnetic radiation (photons) emitted tangentially from the orbit. This light is called synchrotron radiation. The first dedicated synchrotron light source was the Stanford Synchrotron Radiation Laboratory (SSRL) (1977). Nowadays, many... 

LaVerne, J. A. (1988), Bibliography of Studies of the Heavy Particle Radiolysis of Liquids and Aqueous Solutions, Special Report SR-124 of the Notre Dame Radiation Laboratory, Notre Dame, Indiana. 

Hamilton, J. G. (1948b). Quarterly Report, Radiation Laboratory, University of California, Report No. UCRL-157 (National Technical Information Service, Springfield, Virginia). 

Bio-Medical Division Lawrence Radiation Laboratory University of California Livermore, California... 

This work was supported by a grant from the National Science Foundation (PCM 79-04915). JEH is the recipient of a National Science Foundation predoctoral fellowship. The synchrotron radiation used in many of these studies was provided by the Stanford Synchrotron Radiation Laboratory with the financial support of the National Science Foundation (under contract DMR 77-27489) in cooperation with the Department of Energy and by the National Institutes of Health SSRL biotechnology resource (RR-01749). 

George, G.N. Pickering, I.J. 1995. EXAFSPAK a Suite of Computer Programs for Analysis of X-ray Absorption Spectra. Stanford Synchrotron Radiation Laboratory, Stanford, CA, USA. 

The NEXAFS experiments were performed at the Stanford Synchrotron Radiation Laboratory, beamline 1-1. This line is equipped with a grasshopper monochromator, 1200 lines/mm, as described elsewhere (11). The entrance and exit slits were set at 15/im, yielding a resolution of AE/E=8 x 10 °E (E in eV) for light of 300 eV photon energy it resulted in a linewidth of about 0.7 eV. We estimate the total photon flux under those conditions to be on the order of 1 x 10 photons/sec. at 300 eV and for a ring current of 50 mA. 

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