introduction to synchrotron radiation and it’s …...d. attwood 1 introsynchrad_apps2005.ppt...

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IntroSynchRad_Apps2005.ppt D. Attwood 1 Introduction to Synchrotron Radiation and it’s Applications David Attwood University of California, Berkeley and Center for X-Ray Optics Lawrence Berkeley National Laboratory (http://www.coe.berkeley.edu/AST/sxreuv)

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Page 1: Introduction to Synchrotron Radiation and it’s …...D. Attwood 1 IntroSynchRad_Apps2005.ppt Introduction to Synchrotron Radiation and it’s Applications David Attwood University

IntroSynchRad_Apps2005.pptD. Attwood 1

Introduction toSynchrotron Radiationand it’s Applications

David AttwoodUniversity of California, Berkeley

andCenter for X-Ray Optics

Lawrence Berkeley National Laboratory

(http://www.coe.berkeley.edu/AST/sxreuv)

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The Short Wavelength Regionof the Electromagnetic Spectrum

(1.1)

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Characteristic Absorption Edges forAlmost all Elements in this Spectral Region

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Energy Levels, Quantum Numbers, andAllowed Transitions for the copper Atom

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Electron Binding Energies, in Electron Volts (eV), for the Elements in their Natural Forms

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Broadly Tunable Radiation is Needed to Probe the Primary (n = 1 & n = 2) Resonances of the Elements

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• Surface science

• Magnetic materials

• Materials chemistry

• Environmental sciences

• Protein crystallogrphy

• Biomicroscopy

• Chemical dynamics

Typical Applications of Synchrotron Radiation

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Bright and Powerful X-Raysfrom Relativistic Electrons

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Synchrotron Radiationfrom Relativistic Electrons

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Some Useful Formulas for Synchrotron Radiation

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Three Forms of Synchrotron Radiation

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Bending Magnet Radiation Covers a Broad Region of the Spectrum, Including the Primary Absorption

Edges of Most Elements

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Third Generation Facilities, Like Elettra, Have Many Straight Sections and a Small Electron Beam

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Undulator Radiation from a Small Electron Beam Radiating into a Narrow Forward Cone

is Very Bright

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An Undulator Up Close

ALS U5 undulator, beamline 7.0, N = 89, λu = 50 mm

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Undulator Radiation

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Power in the Central Cone

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Power in the Central Radiation Cone for Three Soft X-Ray Undulators

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Power in the Central Radiation Cone for Three Soft X-Ray Undulators

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Power in the Central Radiation Cone for Three Soft X-Ray Undulators

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Brightness and Spectral Brightness

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Spectral Brightness is Useful for Experiments that Involve Spatially Resolved Studies

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The Transition from Undulator Radiation (K ≤ 1) to Wiggler Radiation (K >>1)

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Wiggler Radiation

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Stanford Permanent Magnet Wiggler

LBNL/EXXON/SSRL (1982), SSRL Beamline VI 55 pole (N = 27.5), λW = 7 cm

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Typical Parameters for Synchrotron Radiation

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Typical Parameters for Synchrotron Radiation

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Beamlines are Used to Transport Photons to the Sample, and Take a Desired Spectral Slice

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A Typical Beamline: Monochromator Plus Focusing Optics to Deliver Radiation to the Sample

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High Spectral Resolution (meV) Beamline

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Beamline 7.0 at Berkeley’s Advanced Light Source

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Time Structure of Synchrotron Radiation

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Variable Polarization Undulator Radiation

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What are the Relative Merits?

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A Single Storage Ring Serves Many Scientific User Groups

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Some Sample Applications

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ALS Beamlines After 5 Years

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ALS Beamlines After 5 Years (continued)

www.als.LBL.govwww-ssrl.slac.stanford.edu

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Lectures Available Over the Web Free

UC BerkeleyUC BerkeleyWebcastWebcast

www.coe.berkeley.edu/AST/sxreuv

AST 210 / EECS 213

(offered Fall 2005,starts Aug. 30, 2 pm PDT,

live over internet plus archived)