PPT-Stanford Synchrotron Radiation

Lightsource SSRL Michael Toney Synchrotron Materials Sciences Division SSRL SLAC National Accelerator Laboratory http wwwssrlslacstanfordedutoneygroup Outline 2 SSRL amp Synchrotron Radiation.
What is a synchrotron? A synchrotron is a machine that accelerates charged particles such as electrons to extremely high energies - creating an electron beam that travels at almost the speed of ligh NASM. 1. Exploring the Crab Nebula with the. Hubble, Chandra and Fermi. Space Telescopes. Roger Blandford. KIPAC. Stanford. Anasazi. Indians. 25 ii 2011. NASM. 2. Charles Messier. 25 ii 2011. NASM. 3. D. isproved. . Einstein's. . Relativity. Walter Orlov. Einstein's. . work. : . „. Does . the Inertia of a Body Depend upon its Energy-Content. ?”. „. The laws by which the states of physical systems alter are independent of the alternative, to which of two systems of coordinates, in uniform motion of parallel translation relatively to each other, these alterations of state are referred (principle of relativity. Linda Lim Stanford University Stanford Synchrotron Radiation Lightsource Stephens’ Law – “A Rietveld refinement is never perfected, merely abandoned” Demonstration: R Indus Synchrotrons Utilization Division. RRCAT, Indore. Advances in Science, Engineering and Technology Colloquium . TIFR, August 20, 2010. lodha@rrcat.gov.in. Focused X-Ray . Beams :. Generation . and Applications. continued. Rybicki. & . Lightman. Chapter 6. Also Course notes for “Essential Radio Astronomy” at NRAO, . Condon & Ransom. http://www.cv.nrao.edu/course/astr534/ERA.shtml. Synchrotron Theory: Summary of Results. issues. J.M. Jimenez. Main Topics. Introduction. Vacuum requirements. Vacuum engineering considerations. What was learnt?. Closing Remarks. Introduction. Accelerator vacuum requirements. LEP particle beams were travelling under vacuum to reduce beam-gas interaction which was responsible for:. Undulator. Radiation to Free Electron Lasing. 1. David Attwood. University of California, . Berkeley. http:/. /ast.. coe.berkeley.edu. /sxr2009. http:/. /ast.. coe.berkeley.edu. /srms. Synchrotron radiation. Sources and Optics for XAS. Apurva Mehta. X-ray absorption Spectroscopy. Basic Experiment :. Core electron binding energy, E. b. E. b. =XANES (. X-ay Absorption Near Edge Structure. ). =NEXAFS (. Near Edge X ray Absorption Fine Structure. C. McGuffey. . a. , W. . Schumaker. . a. , S. . Kneip. . b. , F. Dollar . a. , A. . Maksimchuk. a. , A. G. R. Thomas . a. , and K. . Krushelnick. . a. (a) University of Michigan, Center for Ultrafast Optical Science. Rybicki. & . Lightman. Chapter 6. Also Course notes for “Essential Radio Astronomy” at NRAO, . Condon & Ransom. http://www.cv.nrao.edu/course/astr534/ERA.shtml. Synchrotron Theory: Summary of Results. Ivan . Bazarov. 1. Outline. Motion in phase space: quantum picture. Wigner distribution and its connection to synchrotron radiation. Brightness definitions, transverse coherence. Synchrotron radiation in phase space. SSRL OverviewMatthew PadillaSSRL Safety OfficeNUFO 2015 Annual MeetingOak Ridge National LaboratoryStanford Synchrotron Radiation LightsourceSSRL produces extremely bright xrays as a resource for rese C. McGuffey. . a. , W. . Schumaker. . a. , S. . Kneip. . b. , F. Dollar . a. , A. . Maksimchuk. a. , A. G. R. Thomas . a. , and K. . Krushelnick. . a. (a) University of Michigan, Center for Ultrafast Optical Science.