STAR: State of the art

Size: px
Start display at page:

Download "STAR: State of the art"

Transcription

1 i n v e s t i a m o n e l v o s t r o f u t u r o STAR: State of the art Raffaele G. Agostino PON MaTeRiA Materials and Technologies for Advanced Research

2 MaTeRiA EU/National Funding PON Ricerca e Competititvità Scientific responsible: Prof. Mauro Ghedini MaTeRiA is a joint project aimed at developing a new Research Infrastructure inside the University of Calabria campus area Partners: UniCal, The University of Calabria & CNISM, Italian Consortium on Physical Sciences of Matter (1300 reasercher from 39 universities) Funding M STAR source - CNISM 6.6 M Laboratories and building - UniCal 0.7 M Master program UniCal Start Date: End Date:

3 MaTeRiA CENTER Sito STAR The highly specialized laboratories that constitute MaTeRiA will be organized in three progressive levels First level. STAR (Southern Europe Thomson Back-Scattering Source for Applied Research) equipped with the beam-line µtomo. Second level laboratories: 1. Preparation and characterization 2. Characterization of the mechanical and physical properties 3. Modeling and simulation 4. Prototyping 5. Advanced spectroscopy Third level. Network of existent departmental laboratories

4 STAR SOURCE AND µtomo BEAMLINE The TBS source and the microtomography station are developed by

5 STAR SOURCE From 3 rd and 4 th generation synchrotron sources to Inverse Compton Scattering (ICS) Thomson Back-Scattering (TBS) sources 50 m 10 m Courtesy of Dennis T. Palmer, G. Diraddo

6 FEL s and Thomson Sources common mechanism: collision between a relativistic electron and a (pseudo)electromagnetic wave 1-25 GeV electrons cm und. period l u Å kev photons e - Mirror MeV electrons Magnet Focussing parabola Å kev photons X-rays Dump 1.0/2.4 ev - Laser beam Courtesy of Luca Serafini

7 FEL resonance condition l R = l w ( 2 1+ a ) w 2g 2 (magnetostatic undulator) Example: for l R =1Å, l w =2 cm, E=7 GeV a w = 0.93l w cm [ ]B w [T] ( l R = l 1+ a 2 0 2) 4g 2 (electromagnetic undulator) Example: for l R =1Å, l=0.8 mm, E=25 MeV Courtesy of Luca Serafini a 0 µ l mm [ ] P TW R 0 [ mm] [ ] laser power laser spot size

8 Brilliance of X-ray sources l (nm) B Compton µ g 2 Courtesy of Luca Serafini

9 LAYOUT STAR (*) (*) (*) Phase 2 Courtesy of Dennis T. Palmer, G. Diraddo

10 10-80 / / / Courtesy of Luca Serafini

11 STAR: X-RAY BEAM FEATURES X-ray energy tuneable on a wide range up to hard X-rays Controlled BW Low divergence Time structure on the ps-scale Circular µm-sized x-ray source Linear polarization up to 99% switchable pulse to pulse (H vs. V) Simple evolution to higher energies and fluxes USER FACILITY

12 MATERIA/STAR SITE AT UNICAL Sito STAR

13 STAR BUILDING Area Risorse Mobiliari ed Immobiliari - UniCal Sito STAR ESSEBI s.r.l.

14 STAR BUILDING Sito STAR Courtesy of Dennis T. Palmer

15 WORK IN PROGRESS Sito STAR December 11 March 12 December 12 October 13

16 WORK IN PROGRESS Sito STAR Novembre December 11 March 12 December 12 January March April 14 13

17 BUILDING COSTS 2.0 M funded by PON Sito STAR 4.0 M funded by University of Calabria m 2 ground Building infrastructure ( m 3 ) Control room, electrical and air conditioning systems

18 µtomo beamline X-ray microtomography setup Innovative aspects: µtomo fully exploits the diffraction limited, monochromatic and tunable STAR X- rays: Phase contrast images are obtained by using the X-ray beam Chemically resolved radiography for an efficient quantitative analysis by means of the X-ray tunability Hard X-ray are used for high Z elements mapping Experimental techniques: PHase Contrast (PHC) radiography Chemically resolved radiographic images Micro-tomography and holotomography

19 Large Area X-ray Detector development for PhC NEXUS lab, UniCal LUCI DI SINCROTRONE CNR 22 Aprile 2014 LAYOUT µtomo (3) 1 Front end 2 X-ray transfer line 3 Slits 4 Sample-holder 5 Detectors pair 6 Detector stage 7 Data acquisition system (4) (5 ) (6 )

20 Application: high resolution radiography Radiographic Image of a bee collected at the Brookhaven TBS source in propagation mode

21 Application: µ-tomography Phase contrast micro-tomography and morphological analysis of a short carbon fibre reinforced polyamide F. Cosmi et al - Composites Science and Technology 71 (2011) Elettra Syrmep BL Micro-tomographic images (left) and correspondent MIL polar diagrams (right) in the shell and core regions.

22 Application: contrast by elements Standard angiography Iodine K-edge subtraction angiography B. Bertrand et al., European hearth Journal, 2005

23 Application: cultural heritage (a preliminary Analysis of the surface layer of a Rithon from Salto di Cariati R.G. Agostino, A. Taliano Grasso, Ceramiche di imitazione metallica di produzione italica: prime evidenze, in Atti del Conv. Enotri e Brettii in Magna Grecia, Rende, mm

24 STAR Field of interest Chemistry Material Science Physics Engineering Cultural Heritage Bio-medicine Geology

25 STAR - Scheduling Building Design Tender Realization STAR source MIUR Tender Design µtomo II level labs Design Tender III level labs Master Design Tender Realization T Design Realiz Realization Realization

26 STAR Next future A regional partner infrastructure for Material Science involving UniCal CNISM INFN Elettra CNR in connection with other light infrastructures (ELI-NP, SPARC-INFN, Elettra, ) open to the cooperation with scientific communities of the Mediterranean countries.

27 STAR Next Future LUCI DI SINCROTRONE CNR 22 Aprile 2014

Status of the FERMI@Elettra Free Electron Laser

Status of the FERMI@Elettra Free Electron Laser Status of the FERMI@Elettra Free Electron Laser E. Allaria on behalf of the FERMI team Work partially supported by the Italian Ministry of University and Research under grants FIRB-RBAP045JF2 and FIRB-RBAP06AWK3

More information

Experimental Study of Laser-Compton Scattering in the Non-linear Regime

Experimental Study of Laser-Compton Scattering in the Non-linear Regime Experimental Study of Laser-Compton Scattering in the Non-linear Regime Y. Kamiya, T. Kumita Department of Physics, Tokyo Metropolitan University S. Kashiwagi, T. Hirose, M. Washio Advanced Research Institute

More information

The STAR Project: Southern european Thomson source for Applied Research

The STAR Project: Southern european Thomson source for Applied Research The STAR Project: Southern european Thomson source for Applied Research Dennis T. Palmer, INFN - Milano for the STAR Project Team Channeling 2014 09 Oct 2014 Outline of Talk Introduction Beam Dynamics

More information

ESRF Upgrade Phase II: le nuove opportunitá per le linee da magnete curvante

ESRF Upgrade Phase II: le nuove opportunitá per le linee da magnete curvante LUCI DI SINCROTRONE CNR, ROMA 22 APRILE 2014 ESRF Upgrade Phase II: le nuove opportunitá per le linee da magnete curvante Sakura Pascarelli sakura@esrf.fr Page 2 INCREASE IN BRILLIANCE H emittance V emittance

More information

A Quick primer on synchrotron radiation: How would an MBA source change my x-ray beam. Jonathan Lang Advanced Photon Source

A Quick primer on synchrotron radiation: How would an MBA source change my x-ray beam. Jonathan Lang Advanced Photon Source A Quick primer on synchrotron radiation: How would an MBA source change my x-ray beam Jonathan Lang Advanced Photon Source APS Upgrade - MBA Lattice ε ο = 3100 pm ε ο = 80 pm What is emi7ance? I don t

More information

Development of on line monitor detectors used for clinical routine in proton and ion therapy

Development of on line monitor detectors used for clinical routine in proton and ion therapy Development of on line monitor detectors used for clinical routine in proton and ion therapy A. Ansarinejad Torino, february 8 th, 2010 Overview Hadrontherapy CNAO Project Monitor system: Part1:preliminary

More information

Polarization Dependence in X-ray Spectroscopy and Scattering. S P Collins et al Diamond Light Source UK

Polarization Dependence in X-ray Spectroscopy and Scattering. S P Collins et al Diamond Light Source UK Polarization Dependence in X-ray Spectroscopy and Scattering S P Collins et al Diamond Light Source UK Overview of talk 1. Experimental techniques at Diamond: why we care about x-ray polarization 2. How

More information

Call for proposals for experiments on the LMJ- PETAL laser facility from the Academic Community

Call for proposals for experiments on the LMJ- PETAL laser facility from the Academic Community Call for proposals for experiments on the LMJ- PETAL laser facility from the Academic Community ILP (Institut Lasers et Plasmas), CEA (Commissariat à l Energie Atomique et aux Energies Alternatives) and

More information

Raman spectroscopy Lecture

Raman spectroscopy Lecture Raman spectroscopy Lecture Licentiate course in measurement science and technology Spring 2008 10.04.2008 Antti Kivioja Contents - Introduction - What is Raman spectroscopy? - The theory of Raman spectroscopy

More information

Institute of Accelerator Technologies of Ankara University and TARLA Facility

Institute of Accelerator Technologies of Ankara University and TARLA Facility Institute of Accelerator Technologies of Ankara University and TARLA Facility Avni Aksoy Ankara University avniaksoy@ankara.edu.tr On behalf of IAT & TARLA Team Contents Brief history of TAC project Institute

More information

The He-Ne Laser * He-Ne Laser System. Power supply and ballast. interatomic collision. 1E-7 sec

The He-Ne Laser * He-Ne Laser System. Power supply and ballast. interatomic collision. 1E-7 sec The He-Ne Laser * I. Introduction The He-Ne laser (Figure 1) uses a low pressure (ca. 1 Torr He, 0.1 Torr Ne) mixture excited by a dc electric discharge. A ballast resistor is placed in series with the

More information

Electromagnetic Radiation

Electromagnetic Radiation Activity 17 Electromagnetic Radiation Why? Electromagnetic radiation, which also is called light, is an amazing phenomenon. It carries energy and has characteristics of both particles and waves. We can

More information

ULTRAFAST LASERS: Free electron lasers thrive from synergy with ultrafast laser systems

ULTRAFAST LASERS: Free electron lasers thrive from synergy with ultrafast laser systems Page 1 of 6 ULTRAFAST LASERS: Free electron lasers thrive from synergy with ultrafast laser systems Free electron lasers support unique time-resolved experiments over a wide range of x-ray wavelengths,

More information

Bright, brighter, brightest sorgenti di luce e scienza a Elettra e FERMI

Bright, brighter, brightest sorgenti di luce e scienza a Elettra e FERMI Bright, brighter, brightest sorgenti di luce e scienza a Elettra e FERMI Elettra until 2008 ELETTRA SR FERMI FEL Main difference SR recirculate beam multi bunch FEL single pass machine SR High pulse rate

More information

Scanning Electron Microscopy: an overview on application and perspective

Scanning Electron Microscopy: an overview on application and perspective Scanning Electron Microscopy: an overview on application and perspective Elvio Carlino Center for Electron Microscopy - IOM-CNR Laboratorio Nazionale TASC - Trieste, Italy Location of the Center for Electron

More information

Towards large dynamic range beam diagnostics and beam dynamics studies. Pavel Evtushenko

Towards large dynamic range beam diagnostics and beam dynamics studies. Pavel Evtushenko Towards large dynamic range beam diagnostics and beam dynamics studies Pavel Evtushenko Motivation Linacs with average current 1-2 ma and energy 1-2.5 GeV are envisioned as drivers for next generation

More information

Status of Radiation Safety System at

Status of Radiation Safety System at Status of Radiation Safety System at Taiwan Photon Source Joseph C. Liu Radiation and Operation Safety Division National Synchrotron Radiation Research Center, Taiwan NSRRC layout 1.5 GeV, 120m, 400 ma

More information

Answer: b. Answer: a. Answer: d

Answer: b. Answer: a. Answer: d Practice Test IV Name 1) In a single slit diffraction experiment, the width of the slit is 3.1 10-5 m and the distance from the slit to the screen is 2.2 m. If the beam of light of wavelength 600 nm passes

More information

Proton tracking for medical imaging and dosimetry

Proton tracking for medical imaging and dosimetry Proton tracking for medical imaging and dosimetry J.Taylor, P.Allport, G.Casse For the PRaVDA Consortium 1 Background and motivation - What is the PRaVDA experiment? - Why are we using Monte Carlo? GEANT4

More information

Beam Instrumentation Group, CERN ACAS, Australian Collaboration for Accelerator Science 3. School of Physics, University of Melbourne 4

Beam Instrumentation Group, CERN ACAS, Australian Collaboration for Accelerator Science 3. School of Physics, University of Melbourne 4 Prototype tests of a wide-band Synchrotron-Light based Beam Pattern Monitor for measuring charge-couple bunch instabilities in High-Energy Particle Accelerator Beams Sophie Dawson2,3, Mark Boland2,4, David

More information

Near-field scanning optical microscopy (SNOM)

Near-field scanning optical microscopy (SNOM) Adviser: dr. Maja Remškar Institut Jožef Stefan January 2010 1 2 3 4 5 6 Fluorescence Raman and surface enhanced Raman 7 Conventional optical microscopy-limited resolution Two broad classes of techniques

More information

PRACTICE EXAM IV P202 SPRING 2004

PRACTICE EXAM IV P202 SPRING 2004 PRACTICE EXAM IV P202 SPRING 2004 1. In two separate double slit experiments, an interference pattern is observed on a screen. In the first experiment, violet light (λ = 754 nm) is used and a second-order

More information

Physics and Technology of Particle Accelerators Basics, Overview and Outlook Simone Di Mitri, Elettra Sincrotrone Trieste University of Trieste, Dept. of Engineering 1 Prologue This seminar samples the

More information

Les Accélérateurs Laser Plasma

Les Accélérateurs Laser Plasma Les Accélérateurs Laser Plasma Victor Malka Laboratoire d Optique Appliquée ENSTA ParisTech Ecole Polytechnique CNRS PALAISEAU, France victor.malka@ensta.fr Accelerators : One century of exploration of

More information

The Invisible technology

The Invisible technology The Invisible technology A new method for anti-counterfeiting in the cultural heritage field Marco Peloi, Luca Gregoratti, Giuseppina Palma Elettra Sincrotrone Trieste 2 Invisible technology Elettra Sincrotrone

More information

X-rays Images. Prof. Dr. Lucas Ferrari de Oliveira UFPR Informatics Department

X-rays Images. Prof. Dr. Lucas Ferrari de Oliveira UFPR Informatics Department Prof. Dr. Lucas Ferrari de Oliveira UFPR Informatics Department Discovery: German physicist Wilhelm Röntgen in 1895; "X-rays" signify an unknown quantity; X-rays were found emanating from Crookes tubes

More information

Simulation of X-ray fluorescence from planetary surfaces

Simulation of X-ray fluorescence from planetary surfaces Simulation of X-ray fluorescence from planetary surfaces M. Bavdaz, P. Nieminen, A. Owens, T. Peacock ESA-ESTEC A. Mantero, M. G. Pia, S. Saliceti INFN Genova Cosmic rays, jovian electrons Solar X-rays,

More information

Undulators and wigglers for the new generation of synchrotron sources

Undulators and wigglers for the new generation of synchrotron sources Undulators and wigglers for the new generation of synchrotron sources P. Elleaume To cite this version: P. Elleaume. Undulators and wigglers for the new generation of synchrotron sources. Journal de Physique

More information

Powder diffraction and synchrotron radiation

Powder diffraction and synchrotron radiation Powder diffraction and synchrotron radiation Gilberto Artioli Dip. Geoscienze UNIPD CIRCe Center for Cement Materials single xl diffraction powder diffraction Ideal powder Powder averaging Textured sample

More information

The conceptual design of the Electron Spectrometer for the High Field Physics experiments at ELI-NP. S. Balascuta, Edmond Turcu

The conceptual design of the Electron Spectrometer for the High Field Physics experiments at ELI-NP. S. Balascuta, Edmond Turcu The conceptual design of the Electron Spectrometer for the High Field Physics experiments at ELI-NP S. Balascuta, Edmond Turcu 1 Outline The acceleration of the electrons by Laser Wake Fields, using two

More information

Bronx High School of Science Regents Physics

Bronx High School of Science Regents Physics Bronx High School of Science Regents Physics 1. Orange light has a frequency of 5.0 10 14 hertz in a vacuum. What is the wavelength of this light? (A) 1.5 10 23 m (C) 6.0 10 7 m (B) 1.7 10 6 m (D) 2.0

More information

Diffraction of Laser Light

Diffraction of Laser Light Diffraction of Laser Light No Prelab Introduction The laser is a unique light source because its light is coherent and monochromatic. Coherent light is made up of waves, which are all in phase. Monochromatic

More information

UV/Vis Spectroscopy. Varka Evi-Maria Ph.D. Chemist AUTH Thessaloniki 2012

UV/Vis Spectroscopy. Varka Evi-Maria Ph.D. Chemist AUTH Thessaloniki 2012 UV/Vis Spectroscopy Varka Evi-Maria Ph.D. Chemist AUTH Thessaloniki 2012 Introduction of Spectroscopy The structure of new synthesised molecules or isolated compounds from natural sources in the lab must

More information

Physics 30 Worksheet # 14: Michelson Experiment

Physics 30 Worksheet # 14: Michelson Experiment Physics 30 Worksheet # 14: Michelson Experiment 1. The speed of light found by a Michelson experiment was found to be 2.90 x 10 8 m/s. If the two hills were 20.0 km apart, what was the frequency of the

More information

The APS and synchrotron facilities in the US and worldwide: a network perspective

The APS and synchrotron facilities in the US and worldwide: a network perspective The APS and synchrotron facilities in the US and worldwide: a network perspective J. Murray Gibson Director, Advanced Photon Source Associate Laboratory Director, ANL for Photon Sciences Presented at the

More information

The European X-ray Free-Electron Laser Facility European XFEL Massimo Altarelli. www.xfel.eu

The European X-ray Free-Electron Laser Facility European XFEL Massimo Altarelli. www.xfel.eu The European X-ray Free-Electron Laser Facility European XFEL Massimo Altarelli European X-ray Free-Electron Laser Facility 22607 Hamburg, Germany www.xfel.eu The European XFEL 2 Undulator Tunnels First

More information

MICROFOCUSING OF THE FERMI@ELETTRA FEL BEAM WITH A K-B ACTIVE OPTICS SYSTEM: SPOT SIZE PREDICTIONS. Lorenzo Raimondi

MICROFOCUSING OF THE FERMI@ELETTRA FEL BEAM WITH A K-B ACTIVE OPTICS SYSTEM: SPOT SIZE PREDICTIONS. Lorenzo Raimondi MICROFOCUSING OF THE FERMI@ELETTRA FEL BEAM WITH A K-B ACTIVE OPTICS SYSTEM: SPOT SIZE PREDICTIONS Lorenzo Raimondi PADReS Group Sincrotrone Trieste SCpA 1 FERMI@Elettra seeded FEL FEL 1 FEL 2 FEL 1 from

More information

PHYS 222 Spring 2012 Final Exam. Closed books, notes, etc. No electronic device except a calculator.

PHYS 222 Spring 2012 Final Exam. Closed books, notes, etc. No electronic device except a calculator. PHYS 222 Spring 2012 Final Exam Closed books, notes, etc. No electronic device except a calculator. NAME: (all questions with equal weight) 1. If the distance between two point charges is tripled, the

More information

Development and Experimental Performance Evaluation of a Dose-Rate meter for Pulsed Beam.

Development and Experimental Performance Evaluation of a Dose-Rate meter for Pulsed Beam. 5 th International Workshop on Radiation Safety at Synchrotron Radiation Sources Development and Experimental Performance Evaluation of a Dose-Rate meter for Pulsed Beam. A. Vascotto 1, K. Casarin 1, S.

More information

Instytut Fizyki Doświadczalnej Wydział Matematyki, Fizyki i Informatyki UNIWERSYTET GDAŃSKI

Instytut Fizyki Doświadczalnej Wydział Matematyki, Fizyki i Informatyki UNIWERSYTET GDAŃSKI Instytut Fizyki Doświadczalnej Wydział Matematyki, Fizyki i Informatyki UNIWERSYTET GDAŃSKI I. Background theory. 1. Electromagnetic waves and their properties. 2. Polarisation of light: a) unpolarised

More information

Development of a Low Frequency Superconducting RF Electron Gun. September 2010

Development of a Low Frequency Superconducting RF Electron Gun. September 2010 Development of a Low Frequency Superconducting RF Electron Gun Contract DE-FG02-07ER84861 07ER84861 Terry Grimm September 2010 Outline Collaboration Concept Scientific justification Design electromagnetic

More information

FLS 2010 Storage Ring Working Group Session 4: Future ring technology and design issues

FLS 2010 Storage Ring Working Group Session 4: Future ring technology and design issues FLS 2010 Storage Ring Working Group Session 4: Future ring technology and design issues 10:45 11:10 Limits to achievable stability Glenn Decker, APS 11:10 11:35 Stability and alignment of NSLS II magnet

More information

Electron spectroscopy Lecture 1-21. Kai M. Siegbahn (1918 - ) Nobel Price 1981 High resolution Electron Spectroscopy

Electron spectroscopy Lecture 1-21. Kai M. Siegbahn (1918 - ) Nobel Price 1981 High resolution Electron Spectroscopy Electron spectroscopy Lecture 1-21 Kai M. Siegbahn (1918 - ) Nobel Price 1981 High resolution Electron Spectroscopy 653: Electron Spectroscopy urse structure cture 1. Introduction to electron spectroscopies

More information

X-Ray Free Electron Lasers

X-Ray Free Electron Lasers X-Ray Free Electron Lasers Lecture 1. Introduction. Acceleration of charged particles Igor Zagorodnov Deutsches Elektronen Synchrotron TU Darmstadt, Fachbereich 18 0. April 015 General information Lecture:

More information

EXPERIMENTAL CONDITIONS FOR CROSS SECTION MEASUREMENTS FOR ANALYTICAL PURPOSES. L. Csedreki 1. Abstract. I. Introduction

EXPERIMENTAL CONDITIONS FOR CROSS SECTION MEASUREMENTS FOR ANALYTICAL PURPOSES. L. Csedreki 1. Abstract. I. Introduction ACTA PHYSICA DEBRECINA XLVI, 25 (2012) EXPERIMENTAL CONDITIONS FOR CROSS SECTION MEASUREMENTS FOR ANALYTICAL PURPOSES L. Csedreki 1 1 Institute of Nuclear Research of the Hungarian Academy of Sciences,

More information

Instrumenter til E-XFEL. Martin Meedom Nielsen Section for Neutrons and X-rays for Materials Physics

Instrumenter til E-XFEL. Martin Meedom Nielsen Section for Neutrons and X-rays for Materials Physics Instrumenter til E-XFEL Martin Meedom Nielsen Section for Neutrons and X-rays for Materials Physics Enlightening Science European XFEL a leading new research facility 2 The European XFEL (X-Ray Free-Electron

More information

Pump-probe experiments with ultra-short temporal resolution

Pump-probe experiments with ultra-short temporal resolution Pump-probe experiments with ultra-short temporal resolution PhD candidate: Ferrante Carino Advisor:Tullio Scopigno Università di Roma ƒla Sapienza 22 February 2012 1 Pump-probe experiments: generalities

More information

Libera at ELETTRA: prehistory, history and present state

Libera at ELETTRA: prehistory, history and present state Libera at ELETTRA: prehistory, history and present state S. Cleva, S. Bassanese, R. De Monte, G. Gaio, M. Lonza, C. Scafuri Elettra - Sincrotrone Trieste 1 ELETTRA and FERMI@Elettra plants ELETTRA (SR):

More information

Nanometer-scale imaging and metrology, nano-fabrication with the Orion Helium Ion Microscope

Nanometer-scale imaging and metrology, nano-fabrication with the Orion Helium Ion Microscope andras@nist.gov Nanometer-scale imaging and metrology, nano-fabrication with the Orion Helium Ion Microscope Bin Ming, András E. Vladár and Michael T. Postek National Institute of Standards and Technology

More information

THE DUKE FEL LIGHT SOURCE FACILITY

THE DUKE FEL LIGHT SOURCE FACILITY THE DUKE FEL LIGHT SOURCE FACILITY J. M. J. Madey, Director, and the Faculty and Staff of the FEL Laboratory PO Box 90319, Duke University, Durham, NC 27708 Abstract FEL research has proceeded during the

More information

Zero Degree Extraction using an Electrostatic Separator

Zero Degree Extraction using an Electrostatic Separator Zero Degree Extraction using an Electrostatic Separator L. Keller Aug. 2005 Take another look at using an electrostatic separator and a weak dipole to allow a zero degree crossing angle a la the TESLA

More information

Planning for the National Ignition Campaign on NIF

Planning for the National Ignition Campaign on NIF Planning for the National Ignition Campaign on NIF Presentation to Fusion Power Associates Annual Meeting Dec 3-4, 2008 Lawrence Livermore National Laboratory John Lindl NIF Programs Chief Scientist Lawrence

More information

6) How wide must a narrow slit be if the first diffraction minimum occurs at ±12 with laser light of 633 nm?

6) How wide must a narrow slit be if the first diffraction minimum occurs at ±12 with laser light of 633 nm? Test IV Name 1) In a single slit diffraction experiment, the width of the slit is 3.1 10-5 m and the distance from the slit to the screen is 2.2 m. If the beam of light of wavelength 600 nm passes through

More information

Data-analysis scheme and infrastructure at the X-ray free electron laser facility, SACLA

Data-analysis scheme and infrastructure at the X-ray free electron laser facility, SACLA Data-analysis scheme and infrastructure at the X-ray free electron laser facility, SACLA T. Sugimoto, T. Abe, Y. Joti, T. Kameshima, K. Okada, M. Yamaga, R. Tanaka (Japan Synchrotron Radiation Research

More information

Applications of New, High Intensity X-Ray Optics - Normal and thin film diffraction using a parabolic, multilayer mirror

Applications of New, High Intensity X-Ray Optics - Normal and thin film diffraction using a parabolic, multilayer mirror Applications of New, High Intensity X-Ray Optics - Normal and thin film diffraction using a parabolic, multilayer mirror Stephen B. Robie scintag, Inc. 10040 Bubb Road Cupertino, CA 95014 Abstract Corundum

More information

THE TESLA TEST FACILITY AS A PROTOTYPE FOR THE GLOBAL ACCELERATOR NETWORK

THE TESLA TEST FACILITY AS A PROTOTYPE FOR THE GLOBAL ACCELERATOR NETWORK THE TESLA TEST FACILITY AS A PROTOTYPE FOR THE GLOBAL ACCELERATOR NETWORK K. Rehlich, DESY, Hamburg, Germany Abstract The next generation of large accelerators facilities will be produced and operated

More information

Wir schaffen Wissen heute für morgen

Wir schaffen Wissen heute für morgen Diffractive optics for photon beam diagnostics at hard XFELs Wir schaffen Wissen heute für morgen PSI: SLAC: ESRF: SOLEIL: APS: SACLA: EuroXFEL C. David, S. Rutishauser, P. Karvinen, Y. Kayser, U. Flechsig,

More information

Laue lens for Nuclear Medicine

Laue lens for Nuclear Medicine Laue lens for Nuclear Medicine PhD in Physics Gianfranco Paternò Ferrara, 6-11-013 Supervisor: prof. Vincenzo Guidi Sensors and Semiconductors Lab, Department of Physics and Earth Science, University of

More information

X-Rays and Magnetism From Fundamentals to Nanoscale Dynamics

X-Rays and Magnetism From Fundamentals to Nanoscale Dynamics X-Rays and Magnetism From Fundamentals to Nanoscale Dynamics Joachim Stöhr Stanford Synchrotron Radiation Laboratory X-rays have come a long way 1895 1993 10 cm 10 µm 100 nm Collaborators: SSRL Stanford:

More information

Technical Meeting on the Socio-Economic Benefits of Ion Beam Accelerators for Developing Member States

Technical Meeting on the Socio-Economic Benefits of Ion Beam Accelerators for Developing Member States Technical Meeting on the Socio-Economic Benefits of Ion Beam Accelerators for Developing Member States Vienna, Austria 19 23 October 2015 Ref. No.: F1-TM-49620 Information Sheet A. Background Ion beam

More information

Short overview of TEUFEL-project

Short overview of TEUFEL-project Short overview of TEUFEL-project ELAN-meeting may 2004 Frascati (I) Contents Overview of TEUFEL project at Twente Photo cathode research Recent experience Outlook Overview FEL Drive laser Photo cathode

More information

Physics 111 Homework Solutions Week #9 - Tuesday

Physics 111 Homework Solutions Week #9 - Tuesday Physics 111 Homework Solutions Week #9 - Tuesday Friday, February 25, 2011 Chapter 22 Questions - None Multiple-Choice 223 A 224 C 225 B 226 B 227 B 229 D Problems 227 In this double slit experiment we

More information

PUMPED Nd:YAG LASER. Last Revision: August 21, 2007

PUMPED Nd:YAG LASER. Last Revision: August 21, 2007 PUMPED Nd:YAG LASER Last Revision: August 21, 2007 QUESTION TO BE INVESTIGATED: How can an efficient atomic transition laser be constructed and characterized? INTRODUCTION: This lab exercise will allow

More information

Physics Opportunities for High Angular Momentum Photons

Physics Opportunities for High Angular Momentum Photons Physics Opportunities for High Angular Momentum Photons Andrei Afanasev The George Washington University, USA Forum on a laser back scattering facility at the MAX IV ring 24th Annual User Meeting, November

More information

Guide to Understanding X-ray Crystallography

Guide to Understanding X-ray Crystallography Guide to Understanding X-ray Crystallography What is X-ray Crystallography and why do I need to learn it? X-ray Crystallography is a scientific method of determining the precise positions/arrangements

More information

The Invisible technology

The Invisible technology The Invisible technology A new method for anti counterfeiting in the cultural heritage field Marco Peloi marco.peloi@elettra.eu Elettra - Sincrotrone Trieste S.C.p.A The technology Invisible Elettra Sincrotrone

More information

COMPARISON OF FOUR DATA ANALYSIS SOFTWARE FOR COMBINED X-RAY REFLECTIVITY AND GRAZING INCIDENCE X-RAY FLUORESCENCE MEASUREMENTS

COMPARISON OF FOUR DATA ANALYSIS SOFTWARE FOR COMBINED X-RAY REFLECTIVITY AND GRAZING INCIDENCE X-RAY FLUORESCENCE MEASUREMENTS COMPARISON OF FOUR DATA ANALYSIS SOFTWARE FOR COMBINED X-RAY REFLECTIVITY AND GRAZING INCIDENCE X-RAY FLUORESCENCE MEASUREMENTS Bérenger Caby (1), Fabio Brigidi (2), Dieter Ingerle (3), Blanka Detlefs

More information

Projects and R&D activities

Projects and R&D activities Projects and R&D activities J.M. Jimenez On behalf of the Vacuum, Surface and Coatings Group (VSC) Vacuum, Surface and Coatings group* Mandate Design, construction, operation, maintenance and upgrade of

More information

Polarization of Light

Polarization of Light Polarization of Light References Halliday/Resnick/Walker Fundamentals of Physics, Chapter 33, 7 th ed. Wiley 005 PASCO EX997A and EX999 guide sheets (written by Ann Hanks) weight Exercises and weights

More information

Photonic Hydrophones based on Coated Fiber Bragg Gratings

Photonic Hydrophones based on Coated Fiber Bragg Gratings Photonic Hydrophones based on Coated Fiber Bragg Gratings M. Pisco, M. Moccia, M. Consales, V. Galdi, A. Cutolo, A. Cusano Optoelectronics Division, Engineering Department, University of Sannio, Benevento,

More information

TES microcalorimeters for future X ray missions. Athena and Beyond: TES detectors for future X-ray missions. Luigi Piro IAPS/INAF

TES microcalorimeters for future X ray missions. Athena and Beyond: TES detectors for future X-ray missions. Luigi Piro IAPS/INAF Athena and Beyond: TES detectors for future X-ray missions IAPS/INAF 1 Setting the stage Science drivers for a Integral Field Spectrometer in X-rays Driving Requirements and mapping into detector Scenarios

More information

Results from first tests of TRD prototypes for CBM. DPG Frühjahrstagung Münster 2011 Pascal Dillenseger Institut für Kernphysik Frankfurt am Main

Results from first tests of TRD prototypes for CBM. DPG Frühjahrstagung Münster 2011 Pascal Dillenseger Institut für Kernphysik Frankfurt am Main Results from first tests of TRD prototypes for CBM DPG Frühjahrstagung Münster 2011 Pascal Dillenseger Institut für Kernphysik Contents Overview of the CBM experiment CBM-TRD General TRD requirements The

More information

Laboratory #3 Guide: Optical and Electrical Properties of Transparent Conductors -- September 23, 2014

Laboratory #3 Guide: Optical and Electrical Properties of Transparent Conductors -- September 23, 2014 Laboratory #3 Guide: Optical and Electrical Properties of Transparent Conductors -- September 23, 2014 Introduction Following our previous lab exercises, you now have the skills and understanding to control

More information

SILA Sistema Integrato di Laboratori per l Ambiente. CENTRE FOR MICROSCOPY AND MICROANALYSIS Scientific coordinator: Prof.ssa Rosanna De Rosa

SILA Sistema Integrato di Laboratori per l Ambiente. CENTRE FOR MICROSCOPY AND MICROANALYSIS Scientific coordinator: Prof.ssa Rosanna De Rosa CENTRE FOR MICROSCOPY AND MICROANALYSIS Scientific coordinator: Prof.ssa Rosanna De Rosa 0 The Centre for Microscopy and Microanalysis (CM2) is an interdisciplinary service centre, a comprehensive suite

More information

The BESSY HOM Damped Cavity with Ferrite Absorbers. Review of prototype cavity test results, taperedwaveguidesvshomogenouswaveguides

The BESSY HOM Damped Cavity with Ferrite Absorbers. Review of prototype cavity test results, taperedwaveguidesvshomogenouswaveguides The BESSY HOM Damped Cavity with Ferrite Absorbers E. Weihreter / BESSY Review of prototype cavity test results, taperedwaveguidesvshomogenouswaveguides Design of a ferrite loaded ridged circular waveguide

More information

BIG data big problems big opportunities Rudolf Dimper Head of Technical Infrastructure Division ESRF

BIG data big problems big opportunities Rudolf Dimper Head of Technical Infrastructure Division ESRF BIG data big problems big opportunities Rudolf Dimper Head of Technical Infrastructure Division ESRF Slide: 1 ! 6 GeV, 850m circonference Storage Ring! 42 public and CRG beamlines! 6000+ user visits/y!

More information

Leti Introduction and Overview

Leti Introduction and Overview Leti Introduction and Overview Leti Day in Tokyo, October 3rd 2012 Laurent Malier 2012 Leti 2012 1 CEA The CEA at a glance Commissariat à l Énergie Atomique et aux Énergies Alternatives is one of the largest

More information

Optical Fibres. Introduction. Safety precautions. For your safety. For the safety of the apparatus

Optical Fibres. Introduction. Safety precautions. For your safety. For the safety of the apparatus Please do not remove this manual from from the lab. It is available at www.cm.ph.bham.ac.uk/y2lab Optics Introduction Optical fibres are widely used for transmitting data at high speeds. In this experiment,

More information

Services for Synchrotron deployment and operations

Services for Synchrotron deployment and operations 1 Services for Synchrotron deployment and operations Tadeusz Szymocha ACK Cyfronet AGH M. Stankiewicz, A. Wawrzyniak, P. Goryl, M. Zajac, M. Nowak, L. Zytniak, F. Melka Narodowe Centrum Promeniowania Synchrotronowego,

More information

emission of light from atoms discrete line spectra - energy levels, Franck-Hertz experiment

emission of light from atoms discrete line spectra - energy levels, Franck-Hertz experiment Introduction Until the early 20 th century physicists used to explain the phenomena in the physical world around them using theories such a mechanics, electromagnetism, thermodynamics and statistical physics

More information

Cathode Ray Tube. Introduction. Functional principle

Cathode Ray Tube. Introduction. Functional principle Introduction The Cathode Ray Tube or Braun s Tube was invented by the German physicist Karl Ferdinand Braun in 897 and is today used in computer monitors, TV sets and oscilloscope tubes. The path of the

More information

NEAR FIELD OPTICAL MICROSCOPY AND SPECTROSCOPY WITH STM AND AFM PROBES

NEAR FIELD OPTICAL MICROSCOPY AND SPECTROSCOPY WITH STM AND AFM PROBES Vol. 93 (1997) A CTA PHYSICA POLONICA A No. 2 Proceedings of the 1st International Symposium on Scanning Probe Spectroscopy and Related Methods, Poznań 1997 NEAR FIELD OPTICAL MICROSCOPY AND SPECTROSCOPY

More information

bulk 5. Surface Analysis Why surface Analysis? Introduction Methods: XPS, AES, RBS

bulk 5. Surface Analysis Why surface Analysis? Introduction Methods: XPS, AES, RBS 5. Surface Analysis Introduction Methods: XPS, AES, RBS Autumn 2011 Experimental Methods in Physics Marco Cantoni Why surface Analysis? Bulk: structural function Electrical/thermal conduction Volume increases

More information

Raman Spectroscopy. 1. Introduction. 2. More on Raman Scattering. " scattered. " incident

Raman Spectroscopy. 1. Introduction. 2. More on Raman Scattering.  scattered.  incident February 15, 2006 Advanced Physics Laboratory Raman Spectroscopy 1. Introduction When light is scattered from a molecule or crystal, most photons are elastically scattered. The scattered photons have the

More information

Hard X-Ray polarimetry with position sensitive germanium detectors - studies of the recombination transitions into highly charged ions

Hard X-Ray polarimetry with position sensitive germanium detectors - studies of the recombination transitions into highly charged ions Hard X-Ray polarimetry with position sensitive germanium detectors - studies of the recombination transitions into highly charged ions Dissertation zur Erlangung des Doktorgrades der Naturwissenschaften

More information

FY 2016 Laboratory Directed Research and Development (LDRD) Program

FY 2016 Laboratory Directed Research and Development (LDRD) Program Call for Proposals FY 2016 Laboratory Directed Research and Development (LDRD) Program I. Overview The purpose of the LDRD program is to encourage innovation, creativity, originality, and quality to keep

More information

The European X-ray Free-Electron Laser: A Truly European Project. Massimo Altarelli. massimo.altarelli@xfel.eu

The European X-ray Free-Electron Laser: A Truly European Project. Massimo Altarelli. massimo.altarelli@xfel.eu The European X-ray Free-Electron Laser: A Truly European Project Massimo Altarelli European X-ray Free-Electron Laser Facility 22607 Hamburg, Germany massimo.altarelli@xfel.eu Important dates in the history

More information

hypothesis of Louis de Broglie (1924): particles may have wave-like properties

hypothesis of Louis de Broglie (1924): particles may have wave-like properties Wave properties of particles hypothesis of Louis de Broglie (1924): particles may have wave-like properties note: it took almost 20 years after noting that waves have particle like properties that particles

More information

C-DEBI Research Coordination Network

C-DEBI Research Coordination Network C-DEBI Research Coordination Network Module 3 Analyze Data Brandy M. Toner June 2012 University of Minnesota C-DEBI Research Coordination Network Module 3 Analyze Data Brandy M. Toner June 2012 University

More information

Laboratorio Regionale LiCryL CNR-INFM

Laboratorio Regionale LiCryL CNR-INFM Laboratorio Regionale LiCryL CNR-INFM c/o Physics Department - University of Calabria, Ponte P. Bucci, Cubo 33B, 87036 Rende (CS) Italy UNIVERSITÀ DELLA CALABRIA Dipartimento di FISICA Researchers Dr.

More information

Active and passive structural health monitoring system based on arrays of ultrasonic guided waves transducers

Active and passive structural health monitoring system based on arrays of ultrasonic guided waves transducers DINFO Dipartimento di Ingegneria dell Informazione Department of Information Engineering Active and passive structural health monitoring system based on arrays of ultrasonic guided waves transducers L.

More information

Recent Measurements and Plans for the SLAC Compton X- Ray Source

Recent Measurements and Plans for the SLAC Compton X- Ray Source SLAC-PUB-11689 Recent Measurements and Plans for the SLAC Compton X- Ray Source A.E. Vlieks*, R. Akre*, G. Caryotakis*, C. DeStefano #, W.J. Frederick #, J.P. Heritage #, N.C. Luhmann Jr. #, D. Martin*,

More information

Ionospheric Research with the LOFAR Telescope

Ionospheric Research with the LOFAR Telescope Ionospheric Research with the LOFAR Telescope Leszek P. Błaszkiewicz Faculty of Mathematics and Computer Science, UWM Olsztyn LOFAR - The LOw Frequency ARray The LOFAR interferometer consist of a large

More information

Modern Classical Optics

Modern Classical Optics Modern Classical Optics GEOFFREY BROOKER Department of Physics University of Oxford OXPORD UNIVERSITY PRESS Contents 1 Electromagnetism and basic optics 1 1.1 Introduction 1 1.2 The Maxwell equations 1

More information

Radiation Detection and Measurement

Radiation Detection and Measurement Radiation Detection and Measurement June 2008 Tom Lewellen Tkldog@u.washington.edu Types of radiation relevant to Nuclear Medicine Particle Symbol Mass (MeV/c 2 ) Charge Electron e-,! - 0.511-1 Positron

More information

Sensori ottici e laser nelle applicazioni industriali

Sensori ottici e laser nelle applicazioni industriali Sensori ottici e laser nelle applicazioni industriali Guido GIULIANI Pavia giuliani@julight.it 1 Outline Optical sensors in industry: why? Types of optical sensors optical barriers distance measurement

More information

Accelerator Physics WS 2011/12

Accelerator Physics WS 2011/12 Lecture: Accelerator Physics Heidelberg WS 2011/12 Prof. A. Schöning Physikalisches Institut der Universität Heidelberg Introduction 1 Goal of this Lecture Introduction to Accelerator Physics: experimental

More information

The MAX IV Laboratory - We make the invisible visible. Scanditronix users meeting OSLO /15 Jonny Ahlbäck

The MAX IV Laboratory - We make the invisible visible. Scanditronix users meeting OSLO /15 Jonny Ahlbäck The MAX IV Laboratory - We make the invisible visible Scanditronix users meeting OSLO 2013-05- 1 MAX IV Laboratory; My view Physics; Synchrotron light Laboratory with two parts 1. MAX-lab; The existing

More information

Christine E. Hatch University of Nevada, Reno

Christine E. Hatch University of Nevada, Reno Christine E. Hatch University of Nevada, Reno Roadmap What is DTS? How Does it Work? What Can DTS Measure? Applications What is Distributed Temperature Sensing (DTS)? Temperature measurement using only

More information

AUTOMATION OF OPERATIONS ON THE VEPP-4 CONTROL SYSTEM

AUTOMATION OF OPERATIONS ON THE VEPP-4 CONTROL SYSTEM 10th ICALEPCS Int. Conf. on Accelerator & Large Expt. Physics Control Systems. Geneva, 10-14 Oct 2005, PO1.072-7 (2005) AUTOMATION OF OPERATIONS ON THE VEPP-4 CONTROL SYSTEM A. Bogomyagkov, S. Karnaev,

More information