Present status of 200keV polarized electron gun at Nagoya University
|
|
- Sybil Washington
- 5 years ago
- Views:
Transcription
1 Present status of 200keV polarized electron gun at Nagoya University Nagoya University Masahiro Yamamoto, N. Yamamoto, T. Nakanishi, S. Okumi, F. Furuta, M. Miyamoto, M. Kuwahara, K. Naniwa, K. Yasui KEK M. Kuriki, H. Matsumoto, M. Yoshioka
2 Features of the 200kV Gun Ceramic Preparation system is always ground level in spite of 200kV running. Load lock system Clean-Z (re-melted SUS316L) Electro-buff polishing (R<0.12μm) Dark current < 1nA photocathode surface Double ceramics insulation Atomic hydrogen cleaning
3 -200kV power supply Gun Chamber Insulation tank Beam extraction Preparation Chamber Laser pulse
4 Laser (1) CW Nd:YVO 4 SHG ps Ti:Sapphire CW Ti:Sapphire CW Nd:YVO 4 laser (SHG) (Millenia VsJ: Spectra Physics) Power 5W(max), 532nm Pico-second Ti:Sapphire laser (Tsunami PS: Spectra Physics) Pulse width 20 ±1 ps repetition MHz power 800 CW Ti:Sapphire laser (Model 3900: Spectra Physics) tuning range 750 ~ 950 nm average power 500 mw
5 Laser (2) Q-switch YAG Laser (GCR-18S: Spectra Physics) Pulse width ~20 ns repetition 10 Hz power Ti:Sapphire & SHG (LT-2211: LOTIS TII) FF ~ 40 SH ~ 10 THG Ti:Sapphire & SHG SHG Q-switch YAG THG (LOTIS TII) ~ 1 Cs 2 Te Photocathode experiment
6 Problem & Improvement
7 Lifetime problem Quantum Efficiency SLSP#16 (200kV Run) Bulk GaAs (Dark Run) Bulk GaAs (200kV Run) CH :2.0% 4 H O:3.6% 2 CO :8.0% 2 N /CO:10.3% 2 O 2 :0.4% Ar:0.6% H 2 :75.1% H2 N2/CO CO2 H2O CH4 O2 Ar Time(hour) Lifetime < 40 hours Lifetime was limited by harmful residual gases? Base Pressure : Pa H 2 O : Pa CO 2 : Pa
8 QE(t) = QE 0 exp Photocathode Lifetime t τ 1 τ = τ + gas τ + DC τ is determined by... 1 τ = 1 τ gas τ ion 1. Adsorption molecules 2. Field emission 3. Ionization The problem should be conquered first. τ gas << τ DC, τ ion
9 Improvement of a vacuum system Pumping Speed Base Pressure Before 1200 l/s 3.2e-9 Pa After 4640 l/s 5.7e-10 Pa NEG module WP950(saes getters) pumping speed (H 2 ) 430 l/s 8 Total 3440 l/s
10 Improvement of a lifetime Nomalized QE 1 Y = M0*e M1*X M M R After Before Y = M0*e M1*X M0 M1 R O :0.8% Ar:0.6% 2 CH :7.6% 4 H O:4.5% 2 CO :8.9% 2 H :39.4% 2 N /CO:24.1% 2 He:14.1% H2 He N2/CO CO2 H2O CH4 O2 Ar Time (h) Base Pressure : Pa Lifetime was improved ~ 150 hours H 2 O : Pa Total harmful gases were reduced to 1/5. CO 2 : Pa
11 Degradation of NEA Surface dn dt = N(t) α Ι gas N 0 N 0 :the number of initial dipole site α:the coefficient of destruction per one molecule. Ι gas :the density of harmful molecules flux τ gas = N 0 N 0 = ~ 1.4 x 10 5 [s] α I α 9.4 x 10 8 [/s/cm 2 gas ] ( ~ 40 hours ) N 0 = ~ 5.4 x 10 5 [s] α 2.2 x 10 8 [/s/cm 2 ] ( ~ 150 hours ) If N 0 = 3.3 x [/cm 2 ], α = 2.5 ~ 2.8 is estimated. I gas ~ 3.5 x 10 7 [/s/cm 2 ] is required for achieving 1000 h lifetime
12 Emittance Measurement System
13 Emittance Measurement System Not bakable ~10-10 Pa ~10-9 Pa the gun vacuum condition was satisfied. ~10-7 Pa Pepper Pot Mask (10µm holes)
14 Emittance Measurement System Optics Pepper Pot Chamber Sub Vacuum Chamber e-beam
15 Preliminary Result E = 80keV I beam =100nA (CW mode) He-Ne Laser ε rms ~ 1.1 π mm mrad Pulse test is preparing now.
16 Future Plan
17 Electrodes for High Field Gradient Gun Present 200keV Gun Clean-Z (re-melted SUS316L) With electro-buff polishing Limited E max ~ 10MV/m Dark Current [pa] Field emission dependence of electrodes materials Clean-Z Ti Mo Mo-Ti Emax ~ 30MV/m would be possible by using Mo cathode & Ti anode Achieving 500keV gun would be possible Field gradient [MV/m] F.Furuta et al. The result will be published in N.I.M.-A
18 Summary (1) Lifetime problem due to residual molecules was improved. before after Pumping Speed 1200 l/s ~ 4600 l/s Base Pressure Pa Pa Lifetime < 40 h ~ 150 h achieving longer lifetime would be possible... (2) Upgrading new gun chamber and electrodes. Change to Mo cathode and Ti anode from Clean-Z electrodes. Avoiding field emission to the gun chamber wall. (3) Emittance measurement system by pepper pot method has been constructed.
19 Mistakes... The electric connection between feed-through and NEG supporter was melted NEG modules were not activated sufficiently this time. The NEG supporter detected field emission from cathode more than -100kV bias voltage Upgrading to new large radius gun chamber is in progress.
Recent Status of Polarized Electron Sources at Nagoya University
Recent Status of Polarized Electron Sources at Nagoya University M. Kuwahara, N. Yamamoto, F. Furuta, T. Nakanishi, S. Okumi, M. Yamamoto, M. Kuriki *, T. Ujihara ** and K. Takeda ** Graduate School of
More informationInitial Emittance Measurements for Polarized Electron Gun with NEA-GaAs Type Photocathode
Initial Emittance Measurements for Polarized Electron Gun with NEA-GaAs Type Photocathode Naoto Yamamoto*, M. Yamamoto*, R. Sakai*, T. Nakanishi*, S. Okumi*, M. Kuwahara*, K. Tamagaki*, T. Morino*, A.
More informationJlab FEL Photoemission DC Guns
Jlab FEL Photoemission DC Guns Fay Hannon On behalf of the FEL team FLS 2010, 2 nd March 2 Operational Guns 1. FEL Gun 60m Gun Test Stand (GTS) 2. Backup gun, test stand with beam characterization beamline
More informationStatus of linear collider designs:
Status of linear collider designs: Electron and positron sources Design overview, principal open issues G. Dugan March 11, 2002 Electron sourcesfor 500 GeV CM machines Parameter TESLA NLC CLIC Cycle rate
More informationDevelopment of Cs 2 Te photocathode RF gun system for compact THz SASE-FEL
Development of Cs 2 Te photocathode RF gun system for compact THz SASE-FEL R. Kuroda, H. Ogawa, N. Sei, H. Toyokawa, K. Yagi-Watanabe, M. Yasumoto, M. Koike, K. Yamada, T. Yanagida*, T. Nakajyo*, F. Sakai*
More informationRecent PES Photocathode R&D at Nagoya University
Recent PES Photocathode R&D at Nagoya University M. Kuwahara, T. Nishitani a, T. Nakanishi, S. Okumi, M. Yamamoto, F. Furuta, M.Miyamoto, N. Yamamoto, K. Naniwa, K. Yasui, K. Yamaguchi b, O. Watanabe c,
More informationDark current at the Euro-XFEL
Dark current at the Euro-XFEL Jang-Hui Han DESY, MPY Observations at PITZ and FLASH Estimation for the European XFEL Ideas to reduce dark current at the gun DC at FLASH RF gun M1 M2 M3 M4 M5 M6 M7 6 undulator
More informationThe New Superconducting RF Photoinjector a High-Average Current & High-Brightness Gun
The New Superconducting RF Photoinjector a High-Average Current & High-Brightness Gun Jochen Teichert for the BESSY-DESY-FZD-MBI collaboration and the ELBE crew High-Power Workshop, UCLA, Los Angeles 14
More informationERL09 WG1 DC-Gun KEK JAEA
ERL09 WG1 DC-Gun KEK Cornell JLAB CEBAF JAEA JLAB FEL Daresbury Cornell Gun DC Photocathode Gun -750 kv Cathode Preparation and Load Lock 16.5 inch flange Insulator 750 kv, 100 ma HVPS Drive Laser Focusing
More informationPresent status and future of DC photoemission electron guns for high power, high brightness applications
Present status and future of DC photoemission electron guns for high power, high brightness applications DC photoemission electron guns using GaAs cathodes have been in use to produce polarized electrons
More informationICFA ERL Workshop Jefferson Laboratory March 19-23, 2005 Working Group 1 summary Ilan Ben-Zvi & Ivan Bazarov
ICFA ERL Workshop Jefferson Laboratory March 19-23, 2005 Working Group 1 summary Ilan Ben-Zvi & Ivan Bazarov Sincere thanks to all WG1 participants: Largest group, very active participation. This summary
More informationPresent status and future of DC photoemission electron guns for high power, high brightness applications
Present status and future of DC photoemission electron guns for high power, high brightness applications DC photoemission electron guns using GaAs cathodes have been in use to produce polarized electrons
More informationILC Particle Sources -Electron and PositronMasao KURIKI (Hiroshima University)
ILC Particle Sources -Electron and PositronMasao KURIKI (Hiroshima University) Introduction Electron Polarization is important for ILC. NEA GaAs is practically the only solution. Positron polarization
More informationMagnetized Beam Update (LDRD)
Magnetized Beam Update (LDRD) JLEIC Collaboration Meeting March 29, 2016 Riad Suleiman and Matt Poelker Outline Magnetized Bunched Electron Beam Requirements Magnetized Sources JLEIC Magnetized Beam LDRD
More informationDark Current at Injector. Jang-Hui Han 27 November 2006 XFEL Beam Dynamics Meeting
Dark Current at Injector Jang-Hui Han 27 November 2006 XFEL Beam Dynamics Meeting Considerations for the guns Ultra-low slice emittance of electron beams higher gradient at the gun cavity solenoid field
More informationLCLS Injector Prototyping at the GTF
LCLS Injector Prototyping at at the GTF John John Schmerge, SLAC SLAC November 3, 3, 23 23 GTF GTF Description Summary of of Previous Measurements Longitudinal Emittance Transverse Emittance Active LCLS
More informationPreliminary Report on Single and Multi-Crystal Diamond Electron Cathodes
Preliminary Report on Single and Multi-Crystal Diamond Electron Cathodes Eisuke. J. Minehara FEL Laboratory at Tokai, APRC, Kansai, JAERI, 2-4 Tokai, Naka, Ibaraki, 319-1195 JAPAN The next generation high
More informationMagnetized Beam LDRD. Abdullah Mamun On behalf of JLab Injector Group. JLEIC Collaboration Meeting Spring 2018, March 26-28,, Jefferson Lab
Magnetized Beam LDRD Abdullah Mamun On behalf of JLab Injector Group JLEIC Collaboration Meeting Spring 2018, March 26-28,, Jefferson Lab Outline Magnetized Bunched-Beam Electron Cooling LDRD Magnetized
More information1 AT/P5-05. Institute of Applied Physics, National Academy of Sciences of Ukraine, Sumy, Ukraine
1 AT/P5-05 H - Ion Source with Inverse Gas Magnetron Geometry for SNS Project V.A. Baturin, P.A. Litvinov, S.A. Pustovoitov, A.Yu. Karpenko Institute of Applied Physics, National Academy of Sciences of
More informationSRF GUN CHARACTERIZATION - PHASE SPACE AND DARK CURRENT MEASUREMENTS AT ELBE*
SRF GUN CHARACTERIZATION - PHASE SPACE AND DARK CURRENT MEASUREMENTS AT ELBE* E. Panofski #, A. Jankowiak, T. Kamps, Helmholtz-Zentrum Berlin, Berlin, Germany P.N. Lu, J. Teichert, Helmholtz-Zentrum Dresden-Rossendorf,
More informationThe CeB6 Electron Gun for the Soft-X-ray FEL Project at SPring-8
May 25, 2004 DESY, Hamburg, Germany The CeB6 Electron Gun for the Soft-X-ray FEL Project at SPring-8 K. Togawa SPring-8 / RIKEN Harima Institute T. Shintake, H. Baba, T. Inagaki, T. Tanaka SPring-8 / RIKEN
More informationAREAL Test Facility for Advanced Accelerator and Radiation Sources Concepts
2 nd European Advanced Accelerator Concepts AREAL Test Facility for Advanced Accelerator and Radiation Sources Concepts V. Tsakanov CANDLE SRI 13-19 Sep 2015, La Biodola, Isola d'elba Introduction 2nd
More informationExperimental Measurements of the ORION Photoinjector Drive Laser Oscillator Subsystem
Experimental Measurements of the ORION Photoinjector Drive Laser Oscillator Subsystem D.T Palmer and R. Akre Laser Issues for Electron RF Photoinjectors October 23-25, 2002 Stanford Linear Accelerator
More informationAccelerator R&D Opportunities: Sources and Linac. Developing expertise. D. Rubin, Cornell University
Accelerator R&D Opportunities: Sources and Linac D. Rubin, Cornell University Electron and positron sources Requirements Status of R&D Linac Modeling of beam dynamics Development of diagnostic and tuning
More informationHuashun Zhang. Ion Sources. With 187 Figures and 26 Tables Э SCIENCE PRESS. Springer
Huashun Zhang Ion Sources With 187 Figures and 26 Tables Э SCIENCE PRESS Springer XI Contents 1 INTRODUCTION 1 1.1 Major Applications and Requirements 1 1.2 Performances and Research Subjects 1 1.3 Historical
More informationMulti-Alkali Photocathodes Performance in a DC 300 kv Inverted Geometry electron gun
Multi-Alkali Photocathodes Performance in a DC 300 kv Inverted Geometry electron gun ADRIANA CANALES-RAMOS (Universidad Nacional Autónoma de México at Mexico City, Mexico, C.P. 04510) Mentor: CARLOS HERNÁNDEZ-GARCÍA
More informationPol. e + source based on Compton scattering with FEL & 4 mirror cavity 第 8 回全体打合せ, 30 September 2014 KEK, Junji Urakawa
Pol. e + source based on Compton scattering with FEL & 4 mirror cavity 第 8 回全体打合せ, 30 September 2014 KEK, Junji Urakawa Super conducting electron linear accelerator for FEL We assume super radiant mode
More informationH. Maesaka*, K. Togawa, T. Inagaki, K. Onoe, T. Tanaka, A. Higashiya, H. Baba, H. Matsumoto, H. Tanaka, Y. Otake and T. Shintake FLS 2010, SLAC
H. Maesaka*, K. Togawa, T. Inagaki, K. Onoe, T. Tanaka, A. Higashiya, H. Baba, H. Matsumoto, H. Tanaka, Y. Otake and T. Shintake FLS 2010, SLAC 1 Introduction Outline X-ray FEL Project at SPring-8 SCSS
More informationDiamond secondary emitter status & plans. Ilan Ben-Zvi Collider-Accelerator Department Brookhaven National Laboratory
Diamond secondary emitter status & plans Ilan Ben-Zvi Collider-Accelerator Department Brookhaven National Laboratory What is desired in a cathode of a CW, high brightness injector? Timing by a laser short
More informationCsK 2 Sb PHOTOCATHODE DEVELOPMENT FOR. Martin Schmeißer, Julius Kühn, Thorsten Kamps, Andreas Jankowiak Helmholtz-Zentrum Berlin
CsK 2 Sb PHOTOCATHODE DEVELOPMENT FOR Martin Schmeißer, Julius Kühn, Thorsten Kamps, Andreas Jankowiak Helmholtz-Zentrum Berlin 1 PHOTOCATHODES Photoinjector for berlinpro Aim: 0.5 mm mrad emittance from
More informationGEM-based gaseous Photomultipliers for UV and visible photon imaging. Dirk Mörmann Amos Breskin Rachel Chechik Marcin Balcerzyk Bhartendu Singh
GEM-based gaseous Photomultipliers for UV and visible photon imaging Dirk Mörmann Amos Breskin Rachel Chechik Marcin Balcerzyk Bhartendu Singh Gaseous Photomultiplier State of the art: Advantages: large
More informationUpdate on Development of High Current Bunched Electron Beam from Magnetized DC Photogun
Update on Development of High Current Bunched Electron Beam from Magnetized DC Photogun JLEIC Collaboration Meeting October 6, 2016 Riad Suleiman and Matt Poelker Magnetized Cooling JLEIC bunched magnetized
More informationDesign of Electron Gun
Design of Abhay Deshpande Scientist, Medical ics Division Society for Applied Microwave ics Engineering and Research SAMEER, IIT-B Campus, Powai Mumbai 400 076 abhay@sameer.gov.in Introduction of SAMEER
More informationField Emission and Channeling Radiation for High-Spectral-Brilliance X-ray Sources
Field Emission and Channeling Radiation for High-Spectral-Brilliance X-ray Sources Charles Brau, Bo Choi, William Gabella, Anthony Hmelo, John Kozub, Borislav Ivanov, Jonathan Jarvis, Marcus Mendenhall
More informationBeam dynamics studies for PITZ using a 3D full-wave Lienard-Wiechert PP code
Beam dynamics studies for PITZ using a 3D full-wave Lienard-Wiechert PP code Y. Chen, E. Gjonaj, H. De Gersem, T. Weiland TEMF, Technische Universität Darmstadt, Germany DESY-TEMF Collaboration Meeting
More informationDiagnostic Systems for Characterizing Electron Sources at the Photo Injector Test Facility at DESY, Zeuthen site
1 Diagnostic Systems for Characterizing Electron Sources at the Photo Injector Test Facility at DESY, Zeuthen site Sakhorn Rimjaem (on behalf of the PITZ team) Motivation Photo Injector Test Facility at
More informationTHE LCLS-II INJECTOR DESIGN*
THE LCLS-II INJECTOR DESIGN* J.F. Schmerge #, A. Brachmann, D. Dowell, A. Fry, R.K. Li, Z. Li, T. Raubenheimer, T. Vecchione, F. Zhou, SLAC, Menlo Park, CA 94025, USA A. Bartnik, I. Bazarov, B. Dunham,
More informationION Pumps for UHV Systems, Synchrotrons & Particle Accelerators. Mauro Audi, Academic, Government & Research Marketing Manager
ION Pumps for UHV Systems, Synchrotrons & Particle Accelerators Mauro Audi, Academic, Government & Research Marketing Manager ION Pumps Agilent Technologies 1957-59 Varian Associates invents the first
More informationDesign of an RF Photo-Gun (PHIN)
Design of an RF Photo-Gun (PHIN) R. Roux 1, G. Bienvenu 1, C. Prevost 1, B. Mercier 1 1) CNRS-IN2P3-LAL, Orsay, France Abstract In this note we show the results of the RF simulations performed with a 2-D
More informationHigh Gradient Tests of Dielectric Wakefield Accelerating Structures
High Gradient Tests of Dielectric Wakefield Accelerating Structures John G. Power, Sergey Antipov, Manoel Conde, Felipe Franchini, Wei Gai, Feng Gao, Chunguang Jing, Richard Konecny, Wanming Liu, Jidong
More informationDIAGNOSTIC TEST-BEAM-LINE FOR THE MESA INJECTOR
DIAGNOSTIC TEST-BEAM-LINE FOR THE MESA INJECTOR I.Alexander,K.Aulenbacher,V.Bechthold,B.Ledroit,C.Matejcek InstitutfürKernphysik,JohannesGutenberg-Universität,D-55099Mainz,Germany Abstract With the test-beam-line
More informationHIGH CURRENT AND HIGH BRIGHTNESS ELECTRON SOURCES
HIGH CURRENT AND HIGH BRIGHTNESS ELECTRON SOURCES F. Loehl, I. Bazarov, S. Belomestnykh, M. Billing, E. Chojnacki, Z. Conway, J. Dobbins, B. Dunham, R. Ehrlich, M. Forster, S. M. Gruner, C. Gulliford,
More informationDESIGN AND CONSTRUCTION OF LOW ENERGY ELECTRON ACCELERATORS AT SINP MSU
DESIGN AND CONSTRUCTION OF LOW ENERGY ELECTRON ACCELERATORS AT SINP MSU V. Shvedunov Skobeltsyn Institute of Nuclear Physics Lomonosov Moscow State University 26 November 2013 Betatron 1959-1985 Low intensity
More informationInjector Linac and RF gun
Injector Linac and RF gun 1 Linac Overview Mission of electron/positron Injector in SuperKEKB u 40-times higher Luminosity v Twice larger storage beam à Higher beam current at Linac v 20-times higher collision
More informationDevelopment of Pulsed High Gradient Photoelectron Gun
Development of Pulsed High Gradient Photoelectron Gun Paul Scherrer Institut, 4MeV test stand Presented by Martin Paraliev Slide 1/25 Motivation X-ray Free Electron Lasers (XFEL) are important for future
More informationNovel, Hybrid RF Injector as a High-average. Dinh Nguyen. Lloyd Young
Novel, Hybrid RF Injector as a High-average average-current Electron Source Dinh Nguyen Los Alamos National Laboratory Lloyd Young TechSource Energy Recovery Linac Workshop Thomas Jefferson National Accelerator
More informationElectron Source. Contents
2 Electron Source Contents 2.1 Introduction..................................................... 25 2.2 PolarizedElectronGun.............................................. 28 2.2.1 Specifications...............................................
More informationAREAL. Test Facility for Advanced Accelerator and Radiation Sources Concepts. Part.1 Introduction. V. Tsakanov CANDLE SRI
AREAL Test Facility for Advanced Accelerator and Radiation Sources Concepts Part.1 Introduction V. Tsakanov CANDLE SRI 01 October 2015 2 nd European Advanced Accelerator Concepts 13-19 Sep 2015, Isola
More informationStudy on Bose-Einstein Condensation of Positronium
Study on Bose-Einstein Condensation of Positronium K. Shu 1, T. Murayoshi 1, X. Fan 1, A. Ishida 1, T. Yamazaki 1,T. Namba 1,S. Asai 1, K. Yoshioka 2, M. Kuwata-Gonokami 1, N. Oshima 3, B. E. O Rourke
More informationModeling of the secondary electron emission in rf photocathode guns
Modeling of the secondary electron emission in rf photocathode guns J.-H. Han, DESY Zeuthen 8 June 2004 Joint Uni. Hamburg and DESY Accelerator Physics Seminar Contents 1. Necessity of secondary electron
More informationA Polarized Electron PWT Photoinjector for the ILC
2005 ALCPG & ILC Workshops Snowmass, U.S.A. A Polarized Electron PWT Photoinjector for the ILC David Yu, Yan Luo, Alexei Smirnov, DULY Research Inc., Rancho Palos Verdes, CA 90275 Ivan Bazarov, Cornell
More informationEngineering Medical Optics BME136/251 Winter 2017
Engineering Medical Optics BME136/251 Winter 2017 Monday/Wednesday 2:00-3:20 p.m. Beckman Laser Institute Library, MSTB 214 (lab) Teaching Assistants (Office hours: Every Tuesday at 2pm outside of the
More informationSecond-Harmonic Generation Studies of Silicon Interfaces
Second-Harmonic Generation Studies of Silicon Interfaces Z. Marka 1, Y. D. Glinka 1, Y. Shirokaya 1, M. Barry 1, S. N. Rashkeev 1, W. Wang 1, R. D. Schrimpf 2,D. M. Fleetwood 2 and N. H. Tolk 1 1 Department
More informationStudies of the Spin Dynamics of Charge Carriers in Semiconductors and their Interfaces. S. K. Singh, T. V. Shahbazyan, I. E. Perakis and N. H.
Studies of the Spin Dynamics of Charge Carriers in Semiconductors and their Interfaces S. K. Singh, T. V. Shahbazyan, I. E. Perakis and N. H. Tolk Department of Physics and Astronomy Vanderbilt University,
More informationNeedle cathodes for high-brightness beams. Chase Boulware Jonathan Jarvis Heather Andrews Charlie Brau
Needle cathodes for high-brightness beams Chase Boulware Jonathan Jarvis Heather Andrews Charlie Brau Outline of the talk What is brightness? Definition Sources Why is brightness important? Light sources
More informationProton LINAC for the Frankfurt Neutron Source FRANZ
Proton LINAC for the Frankfurt Neutron Source FRANZ - IAEA - International Topical Meeting on Nuclear Research Applications and Utilization of Accelerators Oliver Meusel 4-8 May 2009 Vienna, Austria Motivation
More informationWorkshops on X-band and high gradients: collaboration and resource
Workshops on X-band and high gradients: collaboration and resource 25 October 2012 International workshop on breakdown science and high gradient technology 18-20 April 2012 in KEK 25 October 2012 International
More informationFree-electron laser SACLA and its basic. Yuji Otake, on behalf of the members of XFEL R&D division RIKEN SPring-8 Center
Free-electron laser SACLA and its basic Yuji Otake, on behalf of the members of XFEL R&D division RIKEN SPring-8 Center Light and Its Wavelength, Sizes of Material Virus Mosquito Protein Bacteria Atom
More informationD- Charge Exchange Ionizer for the JINR Polarized Ion Source POLARIS
D- Charge Exchange Ionizer for the JINR Polarized Ion Source POLARIS V.P. Ershov, V.V.Fimushkin, G.I.Gai, L.V.Kutuzova, Yu.K.Pilipenko, V.P.Vadeev, A.I.Valevich Λ and A.S. Belov Λ Joint Institute for Nuclear
More informationIntroduction. Thermoionic gun vs RF photo gun Magnetic compression vs Velocity bunching. Probe beam design options
Introduction Following the 19/05/04 meeting at CERN about the "CTF3 accelerated programme", a possible french contribution has been envisaged to the 200 MeV Probe Beam Linac Two machine options were suggested,
More informationDependency of Gabor Lens Focusing Characteristics on Nonneutral Plasma Properties
Dependency of Gabor Lens Focusing Characteristics on Nonneutral Plasma Properties Kathrin Schulte HIC for FAIR Workshop Riezlern, 14.03.2013 Outline 1. 2. 3. 4. 1. 1.1. Relevant to know about Gabor lenses...or
More informationSuperconducting RF Photoinjectors
Superconducting RF Photoinjectors Jacek Sekutowicz, DESY Introduction Projects; Specs and measured data Cathodes RF-performance of sc-cavities RF-focusing _ growth compensation with DC- and RF-magnetic
More informationUsing IMPACT T to perform an optimization of a DC gun system Including merger
Using IMPACT T to perform an optimization of a DC gun system Including merger Xiaowei Dong and Michael Borland Argonne National Laboratory Presented at ERL09 workshop June 10th, 2009 Introduction An energy
More informationNew Electron Source for Energy Recovery Linacs
New Electron Source for Energy Recovery Linacs Ivan Bazarov 20m Cornell s photoinjector: world s brightest electron source 1 Outline Uses of high brightness electron beams Physics of brightness High brightness
More informationMultivariate Optimization of High Brightness High Current DC Photoinjector. Ivan Bazarov
Multivariate Optimization of High Brightness High Current DC Photoinjector Ivan Bazarov Talk Outline: Motivation Evolutionary Algorithms Optimization Results 1 ERL Injector 750 kv DC Gun Goal: provide
More informationA Multi-beamlet Injector for Heavy Ion Fusion: Experiments and Modeling
A Multi-beamlet Injector for Heavy Ion Fusion: Experiments and Modeling G.A. Westenskow, D.P. Grote; LLNL J.W. Kwan, F. Bieniosek; LBNL PAC07 - FRYAB01 Albuquerque, New Mexico June 29, 2007 This work has
More informationEmission-related Activities at PITZ Proposals for the DFG-Networking "Hi 2 PE"
Emission-related Activities at PITZ Proposals for the DFG-Networking "Hi 2 PE" Ye Chen for the PITZ team 22.09.2017, Helmholtz-Zentrum Berlin, Germany Contents Photoemission (PE) Dark Current (DC) Other
More informationIntroduction to Nonlinear Optics
Introduction to Nonlinear Optics Prof. Cleber R. Mendonca http://www.fotonica.ifsc.usp.br Outline Linear optics Introduction to nonlinear optics Second order nonlinearities Third order nonlinearities Two-photon
More informationTime resolved optical spectroscopy methods for organic photovoltaics. Enrico Da Como. Department of Physics, University of Bath
Time resolved optical spectroscopy methods for organic photovoltaics Enrico Da Como Department of Physics, University of Bath Outline Introduction Why do we need time resolved spectroscopy in OPV? Short
More informationDevelopment status of non-destructive assay of nuclear material by using laser Compton scattered gamma-rays
Development status of non-destructive assay of nuclear material by using laser Compton scattered gamma-rays Ryoichi Hajima Japan Atomic Energy Agency IZEST Tokyo 2013 Nov. 18, 2013 Collaborators Quantum
More informationHighly-Polarized Electron Emission from Strain-Compensated Superlattices and Superlattices with High-Valence-Band Splitting
SLAC-PUB-375 PPRC-TN-- March Highly-Polarized Electron Emission from Strain-Compensated Superlattices and Superlattices with High-Valence-Band Splitting A. V. Rochansky Stanford Linear Accelerator Center,
More informationModeling Electron Emission From Diamond-Amplified Cathodes
Modeling Electron Emission From Diamond-Amplified Cathodes D. A. Dimitrov Tech-X Corporation, Boulder, CO I. Ben-Zvi, T. Rao, J. Smedley, E. Wang, X. Chang Brookhaven National Lab, NY This work is funded
More informationSLS at the Paul Scherrer Institute (PSI), Villigen, Switzerland
SLS at the Paul Scherrer Institute (PSI), Villigen, Switzerland Michael Böge 1 SLS Team at PSI Michael Böge 2 Layout of the SLS Linac, Transferlines Booster Storage Ring (SR) Beamlines and Insertion Devices
More informationPhotoinjector design for the LCLS
SLAC-PUB-8962 LCLS-TN-01-05 Revised November 2001 Photoinjector design for the LCLS P.R. Bolton a, J.E. Clendenin a, D.H. Dowell a, M. Ferrario b, A.S. Fisher a, S.M. Gierman a, R.E. Kirby a, P. Krejcik
More informationThe ISIS Penning H - SPS and Diagnostic Developments at RAL
The ISIS Penning H - SPS and Diagnostic Developments at RAL D.C. Faircloth 1, A.P. Letchford 1, J. Pozimski 1+2, M.O. Whitehead 1, T. Wood 1, S. Jolly 2, P. Savage 2, M. Haigh 3, J. Morrison 3, I. Yew
More informationIonization Detectors
Ionization Detectors Basic operation Charged particle passes through a gas (argon, air, ) and ionizes it Electrons and ions are collected by the detector anode and cathode Often there is secondary ionization
More informationUltrafast nanophotonics - optical control of coherent electron -
ICTP 18.2.8 Ultrafast nanophotonics - optical control of coherent electron - Hirofumi Yanagisawa LMU, MPQ Hirofumi Yanagisawa Japan (Tokyo) Switzerland (Zurich) Germany (Munich) http://roundtripticket.me/world-map-labled.html/best-image-of-diagram-world-map-and-labeled-for-labled
More informationBALKAN PHYSICS LETTERS Bogazici University Press 15 November 2016 BPL, 24, , pp , (2016)
139 BALKAN PHYSICS LETTERS Bogazici University Press 15 November 2016 BPL, 24, 241016, pp. 139 145, (2016) VACUUM STUDIES ON ELECTRON GUN AND INJECTOR LINE OF TARLA FACILITY E. COŞGUN, E.P. DEMİRCİ, Ö.
More informationStatus of the EBIT in the ReA3 reaccelerator at NSCL
Status of the EBIT in the ReA3 reaccelerator at NSCL ReA3 concept and overview: - Gas stopping EBIT RFQ LINAC EBIT commissioning National Science Foundation Michigan State University S. Schwarz, TCP-2010,
More informationHigh average current photo injector (PHIN) for the CLIC Test Facility at CERN
High average current photo injector (PHIN) for the CLIC Test Facility at CERN CLIC and CTF3 motivation Photo injectors, PHIN Emittance measurements Long pulse operation, time resolved measurements Cathode
More informationPlasma Chemistry Study in an Inductively Coupled Dielectric Etcher
Plasma Chemistry Study in an Inductively Coupled Dielectric Etcher Chunshi Cui, John Trow, Ken Collins, Betty Tang, Luke Zhang, Steve Shannon, and Yan Ye Applied Materials, Inc. October 26, 2000 10/28/2008
More informationGEM: A new concept for electron amplification in gas detectors
GEM: A new concept for electron amplification in gas detectors F. Sauli, Nucl. Instr. & Methods in Physics Research A 386 (1997) 531-534 Contents 1. Introduction 2. Two-step amplification: MWPC combined
More informationElectron beam scanning
Electron beam scanning The Electron beam scanning operates through an electro-optical system which has the task of deflecting the beam Synchronously with cathode ray tube which create the image, beam moves
More informationLaser Heater Integration into XFEL. Update. Yauhen Kot XFEL Beam Dynamics Meeting
Laser Heater Integration into XFEL. Update. Yauhen Kot XFEL Beam Dynamics Meeting 5..8 Outline Overview about the main components and space margins Optics at the laser heater and diagnostics - FODO + parabola-like
More informationNova 600 NanoLab Dual beam Focused Ion Beam IITKanpur
Nova 600 NanoLab Dual beam Focused Ion Beam system @ IITKanpur Dual Beam Nova 600 Nano Lab From FEI company (Dual Beam = SEM + FIB) SEM: The Electron Beam for SEM Field Emission Electron Gun Energy : 500
More informationInjector Experimental Progress
Injector Experimental Progress LCLS TAC Meeting December 10-11 2001 John Schmerge for the GTF Team GTF Group John Schmerge Paul Bolton Steve Gierman Cecile Limborg Brendan Murphy Dave Dowell Leader Laser
More informationAn Overview of the Activities of ICS Sources in China
An Overview of the Activities of ICS Sources in China Chuanxiang Tang *, Yingchao Du, Wenhui Huang * tang.xuh@tsinghua.edu.cn Department of Engineering physics, Tsinghua University, Beijing 100084, China
More informationBeam dynamics studies of H-beam chopping in a LEBT for project X
Beam dynamics studies of H-beam chopping in a LEBT for project X Qing Ji, David Grote, John Staples, Thomas Schenkel, Andrew Lambert, and Derun Li Lawrence Berkeley National Laboratory, 1 Cyclotron Road,
More informationVolume Production of D - Negative Ions in Low-Pressure D 2 Plasmas - Negative Ion Densities versus Plasma Parameters -
Volume Production of D - Negative Ions in Low-Pressure D 2 Plasmas - Negative Ion Densities versus Plasma Parameters - Osamu Fukumasa and Shigefumi Mori Department of Electrical and Electronic Engineering,
More informationReduction of thermal emittance of rf guns *
SLAC-PUB-884 LCLS TN 99-8 October 1999 Reduction of thermal emittance of rf guns * J. E. Clendenin, T. Kotseroglou, G. A. Mulhollan, D. T. Palmer, and J. F. Schmerge Stanford Linear Accelerator Center,
More informationSRF-Seminars Jacek Sekutowicz
SRF-Seminars Jacek Sekutowicz 1/32 5. SUPERCONDUCTING PHOTO-INJECTORS 2/32 SRF Photo-Injectors; Topics 1. Introduction 2. Projects; Specs and measured data 3. Cathodes 4. RF-performance of sc-cavities
More informationChemistry Instrumental Analysis Lecture 34. Chem 4631
Chemistry 4631 Instrumental Analysis Lecture 34 From molecular to elemental analysis there are three major techniques used for elemental analysis: Optical spectrometry Mass spectrometry X-ray spectrometry
More informationWG2 on ERL light sources CHESS & LEPP
Charge: WG2 on ERL light sources Address and try to answer a list of critical questions for ERL light sources. Session leaders can approach each question by means of (a) (Very) short presentations (b)
More informationDesign and numerical simulation of thermionic electron gun
Design and numerical simulation of thermionic electron gun M.Hoseinzade 1;1), A.Sadighzadeh 1) Plasma Physics and Nuclear Fusion Research School, Nuclear Science and Technology Research Institute, AEOI,
More informationR&D experiments at BNL to address the associated issues in the Cascading HGHG scheme
R&D experiments at BNL to address the associated issues in the Cascading HGHG scheme Li Hua Yu for DUV-FEL Team National Synchrotron Light Source Brookhaven National Laboratory FEL2004 Outline The DUVFEL
More informationLow Energy RHIC electron Cooling (LEReC)
Low Energy RHIC electron Cooling (LEReC) LEReC overview: project goal and cooling approach Alexei Fedotov MEIC Collaboration Meeting 30 31 LEReC Project Mission/Purpose The purpose of the LEReC is to provide
More informationDevelopment of a table top TW laser accelerator for medical imaging isotope production
Development of a table top TW laser accelerator for medical imaging isotope production R U I Z, A L E X A N D R O 1 ; L E R A, R O B E R T O 1 ; T O R R E S - P E I R Ó, S A LVA D O R 1 ; B E L L I D O,
More informationTime of Flight measurements with MCP-PMT
International Symposium on the Development of Detectors, 2006/4 at SLAC Time of Flight measurements with MCP-PMT - Very high resolution TOF counter - Lifetime of MCP-PMTs T.Ohshima, K.Inami, N.Kishimoto,
More informationHigh quantum efficiency S-20 photocathodes for photon counting applications
High quantum efficiency S-20 photocathodes for photon counting applications D. A. Orlov a,*, J. DeFazio b, S. Duarte Pinto a, R. Glazenborg a and E. Kernen a a PHOTONIS Netherlands BV, Dwazziewegen 2,
More informationPhotoemission Properties of and Under Various Temperature and Incident Photon Energy Conditions
Photoemission Properties of and Under Various Temperature and Incident Photon Energy Conditions Kenichi Morita, Heishun Zen, Kai Masuda, Konstantin Torgasin, Tsubasa Katsurayama, Tomoya Murata, Sikharin
More information