EuroNNAc2011. Leonida A. GIZZI. Istituto Nazionale di OTTICA INO - CNR, Pisa, Italy INFN, Pisa and LNF-Frascati, Italy

Size: px
Start display at page:

Download "EuroNNAc2011. Leonida A. GIZZI. Istituto Nazionale di OTTICA INO - CNR, Pisa, Italy INFN, Pisa and LNF-Frascati, Italy"

Transcription

1 SELF-INJECTION Test Experiment (SITE) Leonida A. GIZZI Istituto Nazionale di OTTICA INO - CNR, Pisa, Italy INFN, Pisa and LNF-Frascati, Italy

2 CONTENTS Scenario and motivations FLAME laser system Self-injection test experiment (S.I.T.E.) Plans and forward look Conclusions

3 THE NATIONAL INSTITUTE OF OPTICS Istituto Nazionale di Ottica (INO) Milano Trento Venezia Sesto F. Pisa FIRENZE Napoli Lecce U.O.S. INO-CNR Firenze, Polo Scientifico Sesto Fiorentino Trento, BEC centre Pisa, Adriano Gozzini Area della Ricerca CNR di Pisa Napoli, Area della Ricerca CNR di Pozzuoli Lecce, Arnesano

4 The Intense Laser Irrad. INO-Pisa CNR - DIPARTIMENTO MATERIALI E DISPOSITIVI (Dir. M. Inguscio) Progetto: OPTICS, PHOTONICS AND PLASMAS (Resp. S. De Silvestri) Unit (Commessa): HIGH FIELD PHOTONICS (Head: Leo A. Gizzi) High field photonics for the generation of ultrashort radiation pulses and high energy particles; Development of broadband laser amplifiers for stategic studies on Inertial Confinement Fusion; PEOPLE Antonio Giulietti (CNR) Head of INO-Pisa Danilo GIULIETTI (Univ. Pisa, CNR)* Leonida A. GIZZI (CNR)* Luca LABATE (CNR)* Petra KOESTER (CNR & Univ. of Pisa)* Giancarlo BUSSOLINO (CNR) Gabriele CRISTOFORETTI (CNR) Moreno VASELLI (CNR-Associato)* Walter BALDESCHI (CNR) Tech. Antonella ROSSI (CNR) Tech. The 3TW laser The compressor The Laboratory Tadzio LEVATO (LNF-INFN), Ass. Naveen PATHAK (UNIPI & CNR), PhD * Also at INFN View of Lungarni Marina di Pisa Chiesa della Spina

5 CNR: Italian Research Network Extreme Light Infrastructure ELI-Italy Consiglio Nazionale delle Ricerche (CNR) Istituto di Fotonica e Nanotecnologie (IFN, Milano-Padova) Istituto Nazionale di Ottica (INO, Firenze-Pisa) Aims Forefront research on lasers and photonics Link to pan-european research infrastructures (ELI) Training of qualified personnel on lasers and photonics Technology transfer to high tech SME (national and international)

6 ELI-Italy - Research Topics High energy radiation and particles Optimization of electron laser driven accelerator -ray source by laser accelerated electrons Radiotherapy applications Attosecond science and applications Schemes for attosecond pulse generation in XUV Diagnostics for attosecond pulse characterization XUV beam lines for attosecond spectroscopy of atoms and molecules Frequency combs Frequency comb from Near-IR to IR Spectral purity and tunability of laser sources locked to the combs Solid state and fiber amplifiers of frequency combs

7 Pursue LPA in the medium term to OUR PLANS FOR LPA a) establishing LPA for future high energy accelerators (collaboration with INFN PLASMONX project); Injector-like approach: seek conditions for compact, all-optical ultra-high gradient, multi-gev, 10 Hz accelerator under controlled laserplasma interaction conditions; Implement plasma schemes (ext. inj., comb.) to enhance existing conventional accelerators; b) bio-medical (industrial) applications of table-top configurations installation in Pisa); Explore the physics of LPA at TW level and 10s of MeVs and find optimum conditions for efficient acceleration with long term operation and stable averaged output applicable to therapy (e.g. IORT).

8 PLASMONX PROJECT LOCATIONS Theo. Exp.

9 LINAC AND LASER AREA AT LNF-FRASCATIFRASCATI

10 LINAC - LASER AREA AT LNF-FRASCATIFRASCATI A dedicated area for LINAC and LASER combined operations LWFA with external injection + Thomson scattering; COMB FLAME lab Newly established LWA with selfinjection + Thomson Scattering SPARC bunker Previously existing FLAME beam e - -beam FLAME Target area Following talks by Luca SERAFINI and Massimo FERRARIO

11 SPARC LINAC at LNF Acceleration with external injection LASER LASER Photoinjector solenoid RF sections quadrupoles dipoles RF deflector collimator 25º 25º 11º 1.5m 10.0 m 5.4 m 14.5 m Diagnostic 1-6 Undulator modules

12 FLAME LASER LABORATORY STATUS OF COMMISSIONING March 2007 Building construction starts October 2010 First LPA electrons 10 mrad December 2010 LPA at >100 MeV level LASER HARDWARE INSTALLATION COMPLETED TEST EXPERIMENT (SELF-INJECTION) STARTED < 50 TW AWAITING SAFETY AND RADIATION PROTECTION AUTHORIZ.

13 FLAME A NEW LASER INSTALLATION Frascati Laser for Acceleration and Multi-disciplinary Experiments

14 FLAME A NEW LASER INSTALLATION Frascati Laser for Acceleration and Multi-disciplinary Experiments LASER UNDERGROUND TARGET AREA (LASER ONLY) TO LINAC

15 FLAME LAB: OVERVIEW LAB INCLUDES LASER, RADIOPROTECTED TARGET AREA FOR LASER-TARGET EXPERIMENTS AND TRANSPORT OF LASER TO SPARC FOR LASER-LINAC OPERATION TRANSPORT TO SPARC TARGET AREA LASER INSTALLATION

16 FLAME TARGET AREA Main beam ( up to 250 TW) vacuum transport line

17 FLAME TARGET AREA Radiation protection walls Main beam (>250 TW) Vacuum transport line Beam transport to sparc bunker Interaction vacuum chamber Compressor vacuum chamber

18 FLAME TARGET AREA: SHIELDING Main beam (>250 TW) Vacuum transport line Radiation protection walls Interaction point Main turning mirror Off-axis parabola Interaction vacuum chamber Electron spectrometer

19 TARGET CHAMBER TOP VIEW

20 ELECTRON SPECTROMETER Finalita : misura spettro energetico elettroni accelerati Energia massima: - Primi test di prova con p 10 MeV, esperimenti a piena potenza possono raggiungere l energia di 10 GeV - L accelerazione di ioni prevede la produzione di protoni con T 10Mev Risoluzione: 1% su largo range Forma del fascio iniziale: -Sorgente puntiforme con 1mrad dispersione angolare iniziale Magnete Il Prototipo rivelatore Working principle R. Faccini et al., Multi-GeV electron spectrometer Nucl. Instrum. Meth. Phys. Res, A 623, (2010). EXPECTED PERFORMANCE RELATIVE ERROR ON MOMENTUM

21 VERT. AND HORIZ. SHIELDING 10 Hz operation

22 LASER: PROJECT REQUIREMENTS FLAME to operate a 250 TW, 10 Hz system Basic issues/challenges (project driven): Pulse contrast (>10 10 ) Pulse duration (<30 fs) Performance stability to compare with LINAC Mechanical stability (< 2 µm at focal spot)

23 LASER BANDWIDTH CONTROL 7J FLAME spectrum With mazzler Without mazzler

24 LASER PULSE COMPRESSION Corner cube Big Grating Output Little Grating PH53 PH52 Periscope PH51 Input Efficiency of the vacuum compressor >70% Pulse duration with the test compressor Spider measurements natural duration < 55 fs corrected duration < 25 fs

25 LASER PULSE CONTRAST Best pulse duration (<25 fs) (with Mazzler loop) Natural pulse duration (<55 fs) Contrast well within specs; ASE contrast at natural pulse duration compares with plasma mirror!

26 LASER BEAM QUALITY Active spatial phase control technique can be used to correct moderate distortions; Sensors are used to measure intensity and phase map of the beam; Deformable mirrors are used to correct the measured wave front distortions in a close loop; wavefront S.-W. Bahk et al., Optics Letters 29, 2837 (2004)

27 ADAPTIVE OPTICS AT FLAME FLAME will be equipped with mechanical deformable mirror

28 ADAPTIVE OPTICS AT FLAME FLAME ADAPTIVE OPTICS WILL CORRECT AT 1% WAVELENGTH

29 FINAL AMPLIFIER: FULL ENERGY Final amplifier operational with all YAG pump lasers Pulse energy: 7.34 J (before compression)

30 LASER AT TARGET CHAMBER CENTER Pointing stability at TCC

31 SUMMARY OF FLAME LASER Summary of performance (to date) Energy before 7.3 J Vacuum compressor transmission > 70% Pulse duration down to 23 fs ASE Contrast ratio: better than 2x10 9 Pre-Pulse Contrast better than 10 8 RMS Pulse 0.8 % Pointing Stability (incl. path) < 2µrad Phase front correction needed adaptive optics; Full power vacuum compression to be performed;

32 SELF-INJECTION DESIGN* *L. A. Gizzi et al., Laser-plasma acceleration with self-injection: A test experiment for the sub-pw FLAME laser system at LNF-Frascati, Il Nuovo Cimento C, 32, 433 (2009).

33 FLAME TEST EXPERIMENT ON SELF-INJECTION

34 SIMULAZIONI SELF-INJECTION (DI C. BENEDETTI ET AL.,)

35 ALADYN SIMULATIONS (DI C. BENEDETTI ET AL.,)

36 INPUT parameters L gasjet = 4 mm n e = W/cm 3 t = 30 fs I 0 = W/cm 2 w 0 = 16 µm S.I.T.E. ACCELERATION GOAL Keywords: Compactness, medium to high energy electrons Reliability (reproducibility and stability) Moderate to small energy spread Expected OUTPUT param. E = 900 MeV DE D = 3.3 % Q = 0.6 nc Bunch length = 1.8 µm Average current = 50 ka Beam divergence = 2.8 mrad

37 SELF-INJECTION TEST EXPERIMENT: OPERATION PRESCRIPTIONS Test experiment carried out under supervision of Radiation Safety Officer Laser power so far limited to 50 TW; Test on reliability of laser alignement procedures, operation and performance; Minimum set of experimental diagnostics to establish key physical paramenters: laser propagation and focusing, target reliability, electron beam production and energy;

38 Highly collimated electron bunches are generated along the laser propagation direction with high reproducibility. 40 mrad 40 mrad

39 Due to pointing instability/intensity intensity distribution profile of the laser pulse sometimes less directional electron bunches were generated. 40 mrad 40 mrad

40 SAMPLE ENERGY SPECTRUM Recent spectra acquired at 1 J laser energy on target and 35 fs: expected intensity at focus: 7E18 W/cm2 Energy dispersion with a 0.9 T magnetic dipole Electrons at lanex screen Lineout Pixel N. Energy of LPA electrons entering the multi 100 MeV range

41 OVERALL POINTING STABILITY WITHIN 20 mrad

42 >50% shots with divergence better than 6 mrad

43 Charge in the bunch weakly dependant on overall (incl. uncollimated) charge 40 mrad

44 SELF-INJECTION TEST EXPERIMENT: PRELIMINARY CONCLUSIONS First test run at <50 TW laser power completed; Acceleration process established at >100 MeV level; Relatively stable production of collimated electron bunches; At higher laser energies evidence of laser beam break-out (with double bunch production!) at focal point due to phase front distortions; AO needed; Next test run at >50 TW awaiting authorization;

45 FORWARD LOOK Repetitive* and stable operation of SITE: > Control of laser stability Mechanical stability concrete basement Thermal stability stabilized clean room > Radiation protection for continuous operation; Underground target area with up to 1m top shield; Remote control of target area operations > Reliable continuous operation of gas target Continuous gas-jet target * L. A. Gizzi et al., High repetition rate laser systems: targets, diagnostics and radiation protection AIP Conf. Proc. Vol. 1209, pp doi: /

46 CONTINUOUS GAS-JET TARGET Target enhancement for long-term repetitive operation; M. De Cesare et al., NIM-B, , 2010

47 FORWARD LOOK - APPLICATIONS ALL-OPTICAL THOMSON SCATTERING SOURCE Preliminary point design (mammography)*: 0.8 J pulse driving the e-beam 4 J producing TS 12 μm FWHM at W/cm 2 Q= 20 pc with a mean energy of about 32 MeV with energy spread of 10% (rms) Long rms size σ L = 0.27 μm, transverse rms size σ T = 0.47 μm transverse norm. emittance ε = 0.23 mm mrad (L.A.Gizzi et al., Eur. Phys. J. ST, 175, 3 10 (2009) 1 fs-long X-ray pulse of mean energy 20 kev energy spread of 25% rms total flux N = photons/shot (i.e Hz) * P. Tomassini, et al., Proc. of the LPAW 2007, IEEE Trans. Plasma Sci. (2007)

48 S.I.T.E. - ADDRESSING QUESTIONS 1/2 Plans for development of facilities with schedule Complete FLAME commissioning at full laser power (2011) Develop hardware to enable double-beam (0, 90, 180 ) configuration (Staging, All-optical Thomson scattering ) (end ) Establish repetitive (10Hz) operation (continuous gas-jet) year perspective (level of approved support: funded/proposed/idea) Complete SITE single beam 4 mm gas-jet, full laser energy to establish acceleration performance and limitations - funded months All-optical X-ray source development (Thomson) proposals in progress Staging for all-optical external injection - concept Laser development / replace front-end with OPCPA - exploratory

49 S.I.T.E. - ADDRESSING QUESTIONS 2/2 Motivation and objectives Establish reliable and stable operation of SITE as a platform for selected applications; implement beam energy control; Acceleration goals (summary table) Stable and long term 10Hz operation of a high charge,>1gev, < 3% energy spread, <3mrad divergence Application goals All-optical Thomson scattering final specifications t.b.d. Possibilities for open access Under discussion endorsement expected also from EuroNNAc networking Expectations for network Promote delivery of reliable LPA technology Embed laser technology development strategies.

50 T. Levato, L. Labate, N. Pathak, F. Piastra, C.A.Cecchetti, D.Giulietti, L.A. Gizzi ILIL-INO, CNR, Pisa, Italy, Sez. INFN, Pisa, Italy, LNF, INFN, Frascati, Italy, Dip. di Fisica, Univ. di Pisa, Italy, N. Drenska, R. Faccini, S. Martellotti, V. Lollo, P. Valente, Sez. INFN Roma-1, Roma, Italy, Dip. Fisica, Univ. La Sapienza, Roma, Italy, C. Benedetti LOASIS Group, LBNL, Berkeley, USA

51 HEAD OF COMMISSIONING Leonida A. GIZZI (CNR, INFN) TECHNICAL MANAGER Giampiero DI PIRRO (LNF) SUBSYSTEMS (Contact persons) Laser Installation Andrea GHIGO (LNF), Leonida A. GIZZI (CNR-INFN) Danilo GIULIETTI ((UNIPI, CNR, INFN-PI) Laser operations and control command Tadzio LEVATO(LNF) and Luca LABATE (CNR & INFN-PI) FLAME-SPARC interfaces Laser, Optical, Electronics, Mechanics Giancarlo GATTI FLAME systems: clean room, water cooling and air conditioning Luigi PELLEGRINO(LNF, Servizio Impianti a Fluido della DT) Electricity network Ruggero RICCI (LNF, Servizio Impianti Elettrici della DT) Ethernet network Massimo PISTONI (LNF) FLAME software interfaces Elisabetta PACE (LNF) Beam Transport air+ vacuum - FLAME buildings Valerio LOLLO (LNF), Alberto CLOZZA (LNF, Servizio Vuoto della DA) & Andrea GAMUCCI (CNR & INFN-PI) SAFETY Sandro VESCOVI (LNF), Tadzio LEVATO (LNF), Carlo VICARIO(LNF) SAFETY (Radiation protection) Adolfo ESPOSITO (LNF) FLAME Target Area - laser beams (main and probe) control, focusing and diagnostics Luca LABATE (CNR & INFN-PI) FLAME Target Area - test experiments diagnostics and remote control Carlo A. CECCHETTI (LNF & IPCF-CNR Pisa) FLAME web site and outreach Leonida A. GIZZI & Luca LABATE Logistics Oreste CERAFOGLI (LNF, Servizio Edilizia della DT) Technical and Engineering support Luciano CACCIOTTI (LNF)

52 SUMMER SCHOOL ON LASER-PLASMA ACCELERATION Varenna, Lago di Como, Italy

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

Comb beam for particle-driven plasma-based accelerators

Comb beam for particle-driven plasma-based accelerators A. Mostacci, on behalf of the SPARC team Comb beams are sub-picosecond, high-brightness electron bunch trains generated via the velocity bunching technique. Such bunch trains can be used to drive tunable

More information

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

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

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

Speed Network Marketing, Energy Selection and Optimal Timetable

Speed Network Marketing, Energy Selection and Optimal Timetable COULOMB11 Optical Acceleration of Ions and Perspective for Biomedicine G. Turchetti Conclusive remarks The regime currently most investigated is TNSA. The problem is not maximum energy. Limits come from

More information

University of Pécs in ELI

University of Pécs in ELI Dept. of Experimental Physics Institute of Physics 7624 Pécs, Ifjúság ú. 6. http://physics.ttk.pte.hu University of Pécs in ELI József Fülöp fulop@fizika.ttk.pte.hu Budapest, April 16, 2008 Outline ELI

More information

STAR: State of the art

STAR: State of the art 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 MaTeRiA EU/National Funding PON Ricerca e Competititvità

More information

Status of High Current Ion Sources. Daniela Leitner Lawrence Berkeley National Laboratory

Status of High Current Ion Sources. Daniela Leitner Lawrence Berkeley National Laboratory http://ecrgroup.lbl.gov Status of High Current Ion Sources Daniela Leitner Lawrence Berkeley National Laboratory October, 27th, 2003 1 Content Overview of available high current sources Requirements for

More information

Development and Commissioning of the Orion Laser Facility

Development and Commissioning of the Orion Laser Facility Development and Commissioning of the Orion Laser Facility Colin Danson, Senior Project Manager, Orion Tom Bett, Colin Brown, Stuart Duffield, Ray Edwards, David Egan, Stephen Elsmere, Jim Firth, Mark Girling,

More information

Slice Emittance Measurements at the SLAC Gun Test Facility*

Slice Emittance Measurements at the SLAC Gun Test Facility* SLAC-PUB-954 September Slice Emittance Measurements at the SLAC Gun Test Facility* D. H. Dowell, P. R. Bolton, J.E. Clendenin, P. Emma, S.M. Gierman, C.G. Limborg, B.F. Murphy, J.F. Schmerge Stanford Linear

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

PoS(PhotoDet 2012)068

PoS(PhotoDet 2012)068 Characterization of the Hamamatsu R11265 multi-anode photomultiplier tube with single photon signals Luca CADAMURO, Marta CALVI, Andrea GIACHERO,, Matteo MAINO, Clara MATTEUZZI, Gianluigi PESSINA Dipartimento

More information

Damping Wigglers in PETRA III

Damping Wigglers in PETRA III Damping Wigglers in PETRA III WIGGLE2005, Frascati 21-22.2.2005 Winni Decking, DESY-MPY Introduction Damping Wiggler Parameters Nonlinear Dynamics with DW Operational Aspects Summary DESY and its Accelerators

More information

BEAM OPERATION OF THE PAL-XFEL INJECTOR TEST FACILITY

BEAM OPERATION OF THE PAL-XFEL INJECTOR TEST FACILITY Proceedings of FEL2014, Basel, Switzerland WEB02 BEAM OPERATION OF THE PAL-XFEL INJECTOR TEST FACILITY J.-H. Han, J. Hong, J. H. Lee, M. S. Chae, S. Y. Baek, H. J. Choi, T. Ha, J. Hu, W. H. Hwang, S. H.

More information

Robust Algorithms for Current Deposition and Dynamic Load-balancing in a GPU Particle-in-Cell Code

Robust Algorithms for Current Deposition and Dynamic Load-balancing in a GPU Particle-in-Cell Code Robust Algorithms for Current Deposition and Dynamic Load-balancing in a GPU Particle-in-Cell Code F. Rossi, S. Sinigardi, P. Londrillo & G. Turchetti University of Bologna & INFN GPU2014, Rome, Sept 17th

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

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

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

STUDY OF THE TRANSVERSE BEAM EMITTANCE OF THE BERN MEDICAL CYCLOTRON

STUDY OF THE TRANSVERSE BEAM EMITTANCE OF THE BERN MEDICAL CYCLOTRON Proceedings of IBIC15, Melbourne, Australia - Pre-Release Snapshot 17-Sep-15 1:3 MOPB41 STUDY OF THE TRANSVERSE BEAM EMITTANCE OF THE BERN MEDICAL CYCLOTRON K. P. Nesteruka,, M. Augera, S. Braccinia, T.

More information

Study of electron cloud at MI and slip stacking process simulation

Study of electron cloud at MI and slip stacking process simulation Study of electron cloud at MI and slip stacking process simulation Alexandr S. Valkovich Purpose 1.Understand the slip stacking process which happens in the Main Injector. 2. Calculation of bunch distortion

More information

Designing and Manufacturing Femtoseconds Ultra-broadband Lasers: Proven, Hands-free Reliability

Designing and Manufacturing Femtoseconds Ultra-broadband Lasers: Proven, Hands-free Reliability Technical Note Designing and Manufacturing Femtoseconds Ultra-broadband Lasers: Proven, Hands-free Reliability This whitepaper reviews how design choices, manufacturing steps and testing protocols substantially

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

HIGH CURRENT OPERATION OF THE ACSI TR30 CYCLOTRON

HIGH CURRENT OPERATION OF THE ACSI TR30 CYCLOTRON HIGH CURRENT OPERATION OF THE ACSI TR30 CYCLOTRON 18 th International Conference on Cyclotrons and their Applications, Sicily, 2007 Vasile Sabaiduc, Project Manager, RF Senior Engineer Advanced Cyclotron

More information

A Compact Linac for Proton Therapy Based on a Dielectric Wall Accelerator

A Compact Linac for Proton Therapy Based on a Dielectric Wall Accelerator UCRL-CONF-236077 A Compact Linac for Proton Therapy Based on a Dielectric Wall Accelerator G. J. Caporaso, T. R. Mackie, S. Sampayan, Y. -J. Chen, D. Blackfield, J. Harris, S. Hawkins, C. Holmes, S. Nelson,

More information

Laser plasma wakefield acceleration and ICAN

Laser plasma wakefield acceleration and ICAN Laser plasma wakefield acceleration and ICAN Laura Corner John Adams Institute, University of Oxford Special thanks to S.M. Hooker ICAN workshop, Paris, April 28 th 2014 Outline The basic idea. Experimental

More information

Dinamica dell Electron Cloud: Calcolo dei Coefficienti della Mappa

Dinamica dell Electron Cloud: Calcolo dei Coefficienti della Mappa Dinamica dell Electron Cloud: Calcolo dei Coefficienti della Mappa T. Demma 1, S.Petracca 2,3, A. Stabile 2 1 LNF INFN, Frascati 2 Dipartimento di Ingegneria - Universita' del Sannio - Benevento 3 Sezione

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

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

ID Objective Requirements Description of Test Date & Examiner 15 Verify that the optics?? OMC

ID Objective Requirements Description of Test Date & Examiner 15 Verify that the optics?? OMC NAOMI OMC/NCU Acceptance Tests at the University of Durham ATC Document number AOW/GEN/RAH/15.0/06/00 OMC/NCU acceptance tests DRAFT (Version date: 2 nd June 2000) wht-naomi-44 The ID numbers are those

More information

Reliability and Availability Aspects of. the IPHI Project

Reliability and Availability Aspects of. the IPHI Project Reliability and Availability Aspects of the IPHI Project Pierre-Yves Beauvais CEA/DSM/DAPNIA for the IPHI Team 18/02/2002 Pierre-Yves Beauvais, CEA Saclay 1 Table of contents Brief description of IPHI

More information

An optical readout configuration for advanced massive GW detectors

An optical readout configuration for advanced massive GW detectors An optical readout configuration for advanced massive GW detectors Francesco Marin, Livia Conti, Maurizio De Rosa Dipartimento di Fisica, Università di Firenze,LENS and INFN, Sezione di Firenze Via Sansone,

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

Results: Low current (2 10 12 ) Worst case: 800 MHz, 12 50 GeV, 4 turns Energy oscillation amplitude 154 MeV, where

Results: Low current (2 10 12 ) Worst case: 800 MHz, 12 50 GeV, 4 turns Energy oscillation amplitude 154 MeV, where Status Focus has shifted to a neutrino factory Two comprehensive designs of acceleration (liancs, arcs) Jefferson Lab, for Fermilab Study CERN (Keil et al.) Jefferson Lab study Low (2 10 12 ) charge per

More information

Figure 1: Lattice drawing for the APS storage ring.

Figure 1: Lattice drawing for the APS storage ring. PERFORMANCE OF THE ADVANCED PHOTON SOURCE Glenn Decker Advanced Photon Source, Argonne National Laboratory 9700 South Cass Avenue, Argonne, Illinois 60439 USA Abstract The Advanced Photon Source (APS)

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

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

ISTITUTO NAZIONALE DI FISICA NUCLEARE

ISTITUTO NAZIONALE DI FISICA NUCLEARE ISTITUTO NAZIONALE DI FISICA NUCLEARE Sezione di Trieste INFN/TC-2/7 1 aprile 22 A novel scheme for the integrated voltage divider of Silicon Drift Detectors P. Burger 1, C. Piemonte 2, A. Rashevsky 3,

More information

Fiber Optic Tweezers and Optical Stretcher: biophotonic tools for single cell studies

Fiber Optic Tweezers and Optical Stretcher: biophotonic tools for single cell studies Fiber Optic Tweezers and Optical Stretcher: biophotonic tools for single cell studies F. Bragheri, L. Ferrara, P. Minzioni, I. Cristiani Electronics Department, University of Pavia, Italy francesca.bragheri@unipv.it

More information

11th International Computational Accelerator Physics Conference (ICAP) August 19 24, 2012, Rostock-Warnemünde (Germany)

11th International Computational Accelerator Physics Conference (ICAP) August 19 24, 2012, Rostock-Warnemünde (Germany) Numerical Modeling of RF Electron Sources for FEL-Accelerators Erion Gjonaj Computational Electromagetics Laboratory (TEMF), Technische Universität Darmstadt, Germany 11th International Computational Accelerator

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

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

10 Project Costs and Schedule

10 Project Costs and Schedule II-367 10 Project Costs and Schedule 10.1 Overview The investment costs given in this chapter include all components necessary for the baseline design of TESLA, as described in chapters 3 to 9. Not included

More information

Maintenance Management on LMJ H. GRAILLOT, I. GRANET CEA/CESTA/DLP

Maintenance Management on LMJ H. GRAILLOT, I. GRANET CEA/CESTA/DLP Maintenance Management on LMJ H. GRAILLOT, I. GRANET CEA/CESTA/DLP Maintenance and Reliability Workshop Synchrotron SOLEIL 9/10 November 2011 1 Maintenance Management on LMJ: outline LMJ context: What

More information

How To Use A Proton For Radiation Therapy

How To Use A Proton For Radiation Therapy Proton Cancer Therapy: Using Laser Accelerate Protons for Radiation Therapy A Thesis Submitted in Partial Fulfillment of the Requirements for Graduation with Research Distinction in Engineering Physics

More information

NANOFLAM. Projet ANR Blanc 2011 BS0401001. Aide allouée: 337 000, durée 36+8 mois (fin : Mai 2015) Laboratoire H. Curien

NANOFLAM. Projet ANR Blanc 2011 BS0401001. Aide allouée: 337 000, durée 36+8 mois (fin : Mai 2015) Laboratoire H. Curien Laboratoire H. Curien Centre de Physique Théorique F. Courvoisier R. Stoian & T. Itina A. Couairon NANOFLAM Projet ANR Blanc 2011 BS0401001 Contrôle de la filamentation et de la génération de plasma avec

More information

Radiant Dyes Laser Accessories GmbH

Radiant Dyes Laser Accessories GmbH New NarrowScan New Resonator Design Improved Sine Drive Unit Autotracking Frequency doubling, tripling and mixing Wavelength Separation Unit Frequency Stabilization Temperature Stabilization Wavelength

More information

Acousto-optic modulator

Acousto-optic modulator 1 of 3 Acousto-optic modulator F An acousto-optic modulator (AOM), also called a Bragg cell, uses the acousto-optic effect to diffract and shift the frequency of light using sound waves (usually at radio-frequency).

More information

Photonic crystal based immunosensor for clinical diagnosis

Photonic crystal based immunosensor for clinical diagnosis 1,4 ID:31132 2 nd year of the PhD in Electronic Devices Official Tutors: Prof. M. De Vittorio 1,2,3, Ing. Tiziana Stomeo 1, Prof. Fabrizio Pirri 4, Prof. Carlo Ricciardi 4 Collaborators: A. Qualtieri 1,

More information

Systems, Inc. Energy Advanced

Systems, Inc. Energy Advanced Systems, Inc. nergy Advanced ADVAND NRGY SYSTMS, IN Our Mission To be the supplier of choice for advanced radiation sources, high brightness commercial accelerator applications, government accelerator

More information

ADONE THE FRASCATI 1.5 GeV ELECTRON POSITRON STORAGE RING

ADONE THE FRASCATI 1.5 GeV ELECTRON POSITRON STORAGE RING 703 ADONE THE FRASCATI 1.5 GeV ELECTRON POSITRON STORAGE RING F. Amman, R. Andreani, M. Bassetti, M. Bernardini, A. Cattani, V. Chimenti, G. Corazza, D. Fabiani, E. Ferlenghi, A. Massarotti, C. Pellegrini,

More information

Understanding Laser Beam Parameters Leads to Better System Performance and Can Save Money

Understanding Laser Beam Parameters Leads to Better System Performance and Can Save Money Understanding Laser Beam Parameters Leads to Better System Performance and Can Save Money Lasers became the first choice of energy source for a steadily increasing number of applications in science, medicine

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

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

16th International Toki Conference on Advanced Imaging and Plasma Diagnostics

16th International Toki Conference on Advanced Imaging and Plasma Diagnostics 16th International Toki Conference on Advanced Imaging and Plasma Diagnostics Temperature Diagnostics for Field-Reversed Configuration Plasmas on the Pulsed High Density (PHD) Experiment Hiroshi Gota,

More information

Activities at the University of Frankfurt (IAP)

Activities at the University of Frankfurt (IAP) Activities at the University of Frankfurt (IAP) Holger Podlech Ulrich Ratzinger Oliver Kester Institut für Angewandte Physik (IAP) Goethe-Universität Frankfurt am Main H. Podlech 1 Development of 325 MHz

More information

RAY TRACING UNIFIED FIELD TRACING

RAY TRACING UNIFIED FIELD TRACING RAY TRACING Start to investigate the performance of your optical system using 3D ray distributions, dot diagrams of ray positions and directions, and optical path length. GEOMETRIC FIELD TRACING Switch

More information

Optical Link ASICs for LHC Upgrades

Optical Link ASICs for LHC Upgrades Optical Link ASICs for LHC Upgrades K.K. Gan, H.P. Kagan, R.D. Kass, J. Moore, S. Smith The Ohio State University July 30, 2009 K.K. Gan DPF2009 1 Outline Introduction VCSEL driver chip PIN receiver/decoder

More information

FIBER LASER STRAIN SENSOR DEVICE

FIBER LASER STRAIN SENSOR DEVICE FIBER LASER STRAIN SENSOR DEVICE E. Maccioni (1,2), N. Beverini (1,2), M. Morganti (1,2) F. Stefani (2,3), R. Falciai (4), C. Trono (4) (1) Dipartimento di Fisica E. Fermi Pisa (2) INFN Sez. Pisa (3) Dipartimento

More information

Stato dei Progetti Speciali SPARC/SPARX e NTA-PLASMONX

Stato dei Progetti Speciali SPARC/SPARX e NTA-PLASMONX Stato dei Progetti Speciali SPARC/SPARX e NTA-PLASMONX Luca Serafini - INFN / Milano SPARC inizia a produrre fisica con misure sul fascio ad alta brillanza prime evidenze sperimentali della teoria inviluppo

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

World-first Proton Pencil Beam Scanning System with FDA Clearance

World-first Proton Pencil Beam Scanning System with FDA Clearance Hitachi Review Vol. 58 (29), No.5 225 World-first Proton Pencil Beam Scanning System with FDA Clearance Completion of Proton Therapy System for MDACC Koji Matsuda Hiroyuki Itami Daishun Chiba Kazuyoshi

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

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

Curriculum Vitae. Max-Planck-Institut für Plasmaphysik, Garching, Munich (Germany)

Curriculum Vitae. Max-Planck-Institut für Plasmaphysik, Garching, Munich (Germany) Curriculum Vitae Personal information Surname / First name Spagnolo Silvia Place / date of birth Vicenza (Italy), 22nd May 1982 Nationality Italian Address Via Lago di Fimon 4B, 36057 Arcugnano, Vicenza

More information

Gravity measurements with atom interferometry

Gravity measurements with atom interferometry Gravity measurements with atom interferometry Fiodor Sorrentino, 28/10/2010 Dipartimento di Fisica e Astronomia, Università di Firenze & INFN, Polo Scientifico di Sesto Fiorentino,via Sansone 1-50019 Sesto

More information

Stefano Colafranceschi

Stefano Colafranceschi Stefano Colafranceschi CERN, European Organization for Nuclear Research Physics Department (PH) Route de Meyrin Tel: +41 76 487 2881 CH-1211 Geneva Fax: +41 22 76 78940 Switzerland email: stefano.colafranceschi@cern.ch

More information

& Tunnel Cross Section

& Tunnel Cross Section CLIC workshop Working group: Two beam hardware and Integration ti CLIC Civil Engineering Layouts & Tunnel Cross Section John Osborne TS-CE Acknowledgements : C.Wyss, J-L Baldy, N.Baddams 17 October 2007

More information

Time out states and transitions

Time out states and transitions Time out states and transitions Spectroscopy transitions between energy states of a molecule excited by absorption or emission of a photon hn = DE = E i - E f Energy levels due to interactions between

More information

Spectral Measurement Solutions for Industry and Research

Spectral Measurement Solutions for Industry and Research Spectral Measurement Solutions for Industry and Research Hamamatsu Photonics offers a comprehensive range of products for spectroscopic applications, covering the, Visible and Infrared regions for Industrial,

More information

Measurement of the gravitational constant G by atom interferometry

Measurement of the gravitational constant G by atom interferometry Measurement of the gravitational constant G by atom interferometry Fiodor Sorrentino Dipartimento di Fisica & LENS, Università di Firenze & INFN MAGIA Misura Accurata di G mediante Interferometria Atomica

More information

Realization of a UV fisheye hyperspectral camera

Realization of a UV fisheye hyperspectral camera Realization of a UV fisheye hyperspectral camera Valentina Caricato, Andrea Egidi, Marco Pisani and Massimo Zucco, INRIM Outline Purpose of the instrument Required specs Hyperspectral technique Optical

More information

SIMULATIONS OF ELECTRON CLOUD BUILD-UP AND SATURATION IN THE APS *

SIMULATIONS OF ELECTRON CLOUD BUILD-UP AND SATURATION IN THE APS * SIMULATIONS OF ELECTRON CLOUD BUILD-UP AND SATURATION IN THE APS * K. C. Harkay and R. A. Rosenberg, ANL, Argonne, IL 60439, USA M. A. Furman and M. Pivi, LBNL, Berkeley, CA 94720, USA Abstract In studies

More information

Tom Wilson Product Marketing Manager Delivery Systems Varian Medical Systems International AG. CERN Accelerator School, May 2015

Tom Wilson Product Marketing Manager Delivery Systems Varian Medical Systems International AG. CERN Accelerator School, May 2015 INDUSTRIAL DESIGN Tom Wilson Product Marketing Manager Delivery Systems Varian Medical Systems International AG VARIAN ONCOLOGY SYSTEMS 1 VARIAN ONCOLOGY SYSTEMS CERN Accelerator, May 2015 Industrial Design

More information

Soil degradation monitoring by active and passive remote-sensing means: examples with two degradation processes

Soil degradation monitoring by active and passive remote-sensing means: examples with two degradation processes Soil degradation monitoring by active and passive remote-sensing means: examples with two degradation processes Naftaly Goldshleger, *Eyal Ben-Dor,* *Ido Livne,* U. Basson***, and R.Ben-Binyamin*Vladimir

More information

Flameless Technology for Particulate Emissions Suppression

Flameless Technology for Particulate Emissions Suppression Flameless Technology for Particulate Emissions Suppression M. Malavasi, C. Allouis, A. D'Anna Report RSE/2009/108 Ente per le Nuove tecnologie, l Energia e l Ambiente RICERCA SISTEMA ELETTRICO Flameless

More information

ISTITUTO NAZIONALE DI FISICA NUCLEARE CONSIGLIO DIRETTIVO DELIBERAZIONE N. 12977 DELIBERA

ISTITUTO NAZIONALE DI FISICA NUCLEARE CONSIGLIO DIRETTIVO DELIBERAZIONE N. 12977 DELIBERA ISTITUTO NAZIONALE DI FISICA NUCLEARE CONSIGLIO DIRETTIVO DELIBERAZIONE N. 12977 Il Consiglio Direttivo dell Istituto Nazionale di Fisica Nucleare, riunito a Roma in data 29 novembre 2013 alla presenza

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

Solar Energy. Outline. Solar radiation. What is light?-- Electromagnetic Radiation. Light - Electromagnetic wave spectrum. Electromagnetic Radiation

Solar Energy. Outline. Solar radiation. What is light?-- Electromagnetic Radiation. Light - Electromagnetic wave spectrum. Electromagnetic Radiation Outline MAE 493R/593V- Renewable Energy Devices Solar Energy Electromagnetic wave Solar spectrum Solar global radiation Solar thermal energy Solar thermal collectors Solar thermal power plants Photovoltaics

More information

SPATIAL-TIME PATTERN OF ELECTRICAL FIELD OF TERAHERTZ PULSE IN THE FAR FIELD

SPATIAL-TIME PATTERN OF ELECTRICAL FIELD OF TERAHERTZ PULSE IN THE FAR FIELD NANOSYSTEMS: PHYSICS, CHEMISTRY, MATHEMATICS, 2013, 4 (2), P. 206 213 SPATIAL-TIME PATTERN OF ELECTRICAL FIELD OF TERAHERTZ PULSE IN THE FAR FIELD M. S. Kulya 1, Ya. V. Grachev 1, V. G. Bespalov 1, V.

More information

PIPELINE LEAKAGE DETECTION USING FIBER-OPTIC DISTRIBUTED STRAIN AND TEMPERATURE SENSORS WHITE PAPER

PIPELINE LEAKAGE DETECTION USING FIBER-OPTIC DISTRIBUTED STRAIN AND TEMPERATURE SENSORS WHITE PAPER PIPELINE LEAKAGE DETECTION USING FIBER-OPTIC DISTRIBUTED STRAIN AND TEMPERATURE SENSORS WHITE PAPER Lufan Zou and Taha Landolsi OZ Optics Limited, 219 Westbrook Road, Ottawa, ON, Canada, K0A 1L0 E-mail:

More information

Experimental study of beam hardening artefacts in photon counting breast computed tomography

Experimental study of beam hardening artefacts in photon counting breast computed tomography Experimental study of beam hardening artefacts in photon counting breast computed tomography M.G. Bisogni a, A. Del Guerra a,n. Lanconelli b, A. Lauria c, G. Mettivier c, M.C. Montesi c, D. Panetta a,

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

Wavelength stabilized high-power diode laser modules

Wavelength stabilized high-power diode laser modules Wavelength stabilized high-power diode laser modules Bernd Köhler *, Thomas Brand, Matthias Haag, Jens Biesenbach DILAS Diodenlaser GmbH, Galileo-Galilei-Str. 10, 55129 Mainz-Hechtsheim, Germany ABSTRACT

More information

Modification of Pd-H 2 and Pd-D 2 thin films processed by He-Ne laser

Modification of Pd-H 2 and Pd-D 2 thin films processed by He-Ne laser Modification of Pd-H 2 and Pd-D 2 thin films processed by He-Ne laser V.Nassisi #, G.Caretto #, A. Lorusso #, D.Manno %, L.Famà %, G.Buccolieri %, A.Buccolieri %, U.Mastromatteo* # Laboratory of Applied

More information

Medical Applications of radiation physics. Riccardo Faccini Universita di Roma La Sapienza

Medical Applications of radiation physics. Riccardo Faccini Universita di Roma La Sapienza Medical Applications of radiation physics Riccardo Faccini Universita di Roma La Sapienza Outlook Introduction to radiation which one? how does it interact with matter? how is it generated? Diagnostics

More information

Round Table Italy-Russia at Dubna

Round Table Italy-Russia at Dubna Round Table Italy-Russia at Dubna Efforts in Fundamental Research and Perspectives for Applied S&T and Business Development Report by Marco Boiti President of Consortium E.I.N.S.T.E.IN. on Scientific cooperation

More information

ELENCO RIVISTE. Presidenza. Laboratori Nazionali di Frascati. New Scientist Physics Today Science Scienze

ELENCO RIVISTE. Presidenza. Laboratori Nazionali di Frascati. New Scientist Physics Today Science Scienze ELENCO RIVISTE Presidenza New Scientist Science Scienze Laboratori Nazionali di Frascati Advances in Physics American Journal of Physics Annals of Physics Applied Physics Letters Astronomy and Astrophysics

More information

RICH. INFN Perugia INFN Firenze CERN. M.Lenti

RICH. INFN Perugia INFN Firenze CERN. M.Lenti RICH INFN Perugia INFN Firenze CERN M.Lenti Separate pions from muons

More information

Chapter 3 SYSTEM SCANNING HARDWARE OVERVIEW

Chapter 3 SYSTEM SCANNING HARDWARE OVERVIEW Qiang Lu Chapter 3. System Scanning Hardware Overview 79 Chapter 3 SYSTEM SCANNING HARDWARE OVERVIEW Since all the image data need in this research were collected from the highly modified AS&E 101ZZ system,

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

Running in 2011 - Luminosity. Mike Lamont Verena Kain

Running in 2011 - Luminosity. Mike Lamont Verena Kain Running in 2011 - Luminosity Mike Lamont Verena Kain Presentations Many thanks to all the speakers! Experiments expectations Massi Ferro-Luzzi Pushing the limits: beam Elias Métral Pushing the limits:

More information

The IR FEL at the Fritz Haber Institute Berlin: A Tool for IR Spectroscopy of Molecules, Clusters, and Solids

The IR FEL at the Fritz Haber Institute Berlin: A Tool for IR Spectroscopy of Molecules, Clusters, and Solids The IR FEL at the Fritz Haber Institute Berlin: A Tool for IR Spectroscopy of Molecules, Clusters, and Solids Wieland Schöllkopf Fritz-Haber-Institut der Max-Planck-Gesellschaft, Berlin Outline 1. Design

More information

Millijoules high master-slave pulse ratio 532 nm picosecond laser

Millijoules high master-slave pulse ratio 532 nm picosecond laser Millijoules high master-slave pulse ratio 532 nm picosecond laser Zhao You Fan Zhongwei 1, Bai Zhenao 12, Zhang Guoxin 2, Lian Fuqiang 12, Zhao You 3, Shen Ming 3 1 Academy of Opto-Electronics, Chinese

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

High Power Neutral Beam Injection in LHD

High Power Neutral Beam Injection in LHD JP0655016 High Power Neutral Beam Injection in LHD K. Tsumori, Y. Takeiri, K. Nagaoka, K. Ikeda, M. Osakabe, Y. Oka, O. Kaneko, M. Shibuya, T. Kondo, M. Sato and E. Asano. National Institute for Fusion

More information

Mission: Cure, Research and Teaching. Marco Pullia Cnao design and commissioning

Mission: Cure, Research and Teaching. Marco Pullia Cnao design and commissioning CNAO design and commissioning Marco Pullia, CNAO Foundation What is the CNAO Foundation No profit organisation (Foundation) created with the financial law 2001 to build the national center for hadrontherapy

More information

Experiment 5. Lasers and laser mode structure

Experiment 5. Lasers and laser mode structure Northeastern University, PHYS5318 Spring 2014, 1 1. Introduction Experiment 5. Lasers and laser mode structure The laser is a very important optical tool that has found widespread use in science and industry,

More information