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Terunuma, N.

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MO6RFP065 Simulations of Mode Separated RF Photo Cathode Gun 515
 
  • A. Deshpande
    Sokendai, Ibaraki
  • S. Araki, M.K. Fukuda, N. Terunuma, J. Urakawa
    KEK, Ibaraki
  • K. Sakaue, M. Washio
    RISE, Tokyo
  • N. Sasao
    Kyoto University, Kyoto
 
 

At Accelerator Test Facility (ATF), we have developed and successfully used RF Photocathode gun as the source of electrons. We have also used a similar gun in the Laser Undulator Compact X-ray source facility (LUCX), KEK (High Energy Accelerator Research Organization) for performing experiments to generate X-rays by inverse Compton scattering. Both the existing guns have mode separation of 4 MHz. We designed a new RF Gun with high mode separation of around 9 MHz and high Q value to achieve a low emittance beam of good quality. We are also modifying the power delivery scheme to the accelerator at LUCX to achieve the acceleration of 200 nC in 100 bunches with low emittance. This will help to increase the intensity of X-rays by the inverse Compton scattering.

 
TU6RFP036 Beam Extraction Using Strip-Line Kicker at KEK-ATF 1620
 
  • T. Naito, H. Hayano, K. Kubo, S. Kuroda, T. Okugi, N. Terunuma, J. Urakawa
    KEK, Ibaraki
 
 

The kicker of the damping ring for the International linear collider(ILC) requires fast rise/fall times(3 or 6ns) and high repetition rate(3 MHz). A multiple strip-line kicker system is developing to realize the specification*. We present results of the beam test at KEK-ATF by the strip-line kicker**. The multi-bunch beam, which has 5.6ns bunch spacing in the damping ring, is extracted with 308ns duration. Two units of the strip-line electrodes are used to extract the beam. The scheme of the beam extraction is same as the kicker of the ILC. A bump orbit and an auxiliary septum magnet are used with the kicker to clear the geometrical restriction.


*T. Naito et. al., Proc. of PAC07, pp2772-2274
**T. Naito et. al., Proc. of EPAC08, pp601-603

 
WE3GRC04 3-Dimensional Beam Profile Monitor Based on a Pulse Storage in an Optical Cavity for Multi-Bunch Electron Beam 1925
 
  • K. Sakaue, M. Washio
    RISE, Tokyo
  • S. Araki, M.K. Fukuda, Y. Higashi, Y. Honda, T. Taniguchi, N. Terunuma, J. Urakawa
    KEK, Ibaraki
  • N. Sasao
    Kyoto University, Kyoto
 
 

Funding: Work supported by a Grant-In-Aid for Creative Scientific Research of JSPS (KAKENHI 17GS0210) and a Grant-In-Aid for JSPS Fellows (19-5789)


We have been developing a pulsed-laser storage technique in a super-cavity for compact X-ray sources. The pulsed-laser super-cavity enables to make high peak power and small waist laser at the collision point with the electron beam. Recently, using 357 MHz mode-locked Nd:VAN laser pulses which stacked in a super-cavity scattered off a multi-bunch electron beam, we obtained multi-pulse X-rays through laser-Compton scattering. Detecting an X-ray pulse-by-pulse using a high-speed detector makes it possible to measure the 3-dimensional beam size with bunch-by-bunch scanning the laserwire target position and pulse timing. This technique provides not only the non-destructive beam profile monitoring but also the measuring of bunch length and/or bunch spacing shifting. In our multi-bunch electron linac, the bunch spacing narrowing due to the electron velocity difference in the train at the output of rf-gun cavity was observed. The principle of the 3-dimensional laserwire monitor and the experimental results of multi-bunch electron beam measurements will be presented at the conference.

 

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MO6RFP102 Present Status of a Multi-Bunch Electron Beam Linac Based on Cs-Te Photo-Cathode RF-Gun at Waseda University 608
 
  • T. Suzuki, T. Fujino, Y. Kato, A. Masuda, A. Murata, K. Sakaue, M. Washio
    RISE, Tokyo
  • H. Hayano, T. Takatomi, N. Terunuma, J. Urakawa
    KEK, Ibaraki
  • S. Kashiwagi
    ISIR, Osaka
  • R. Kuroda
    AIST, Tsukuba, Ibaraki
 
 

At Waseda University, we have been developing a high quality electron source based on photo-cathode rf-gun and its application experiments. To produce a high current electron beam, we installed a Cs-Te cathode which has higher quantum efficiency and improved the structure of the rf cavity. By adopting a Cs-Te cathode, it is expected that the production of the higher charged single bunch electron beam with a low emittance can be achieved. Moreover, the generation of high quality multi-bunch electron beam is also expected to be possible due to the high quantum efficiency of Cs-Te. For understanding of a Cs-Te cathode and higher quantum efficiency operation, we have performed the fundamental studies by single bunch beam. On the other hand, we have also developed a multi-pulse UV laser for generating the multi-bunch electron beam. Our laser system is composed by all-solid-state Nd:YLF for the stable operation, and the specification of this laser is expected to generate a 100bunch/train with the bunch charge of 800pC/bunch. In this conference, the experimental results of Cs-Te and new laser system and the recent progress of multi-bunch electron beam generation will be reported.

 
WE6PFP024 ATF2 Ultra-Low IP Betas Proposal 2540
 
  • R. Tomás, H.-H. Braun, J.-P. Delahaye, A. Marin, D. Schulte, F. Zimmermann
    CERN, Geneva
  • D. Angal-Kalinin, J.K. Jones
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
  • S. Bai, J. Gao, X.W. Zhu
    IHEP Beijing, Beijing
  • P. Bambade, M. Renier
    LAL, Orsay
  • Y. Honda, S. Kuroda, T. Okugi, T. Tauchi, N. Terunuma, J. Urakawa
    KEK, Ibaraki
  • A. Scarfe
    UMAN, Manchester
  • A. Seryi, G.R. White, M. Woodley
    SLAC, Menlo Park, California
 
 

The CLIC Final Focus System has considerably larger chromaticity than those of ILC and its scaled test machine ATF2. We propose to reduce the IP betas of ATF2 to reach a CLIC-like chromaticity. This would also allow to study the FFS tuning difficulty as function of the IP beam spot size. Both the ILC and CLIC projects will largely benefit from the ATF2 experience at these ultra-low IP betas.

 
TH5RFP070 Nanometer Resolution Beam Position Monitor for the ATF2 Interaction Point Region 3603
 
  • A. Heo, E.-S. Kim, H.-S. Kim
    Kyungpook National University, Daegu
  • R. Ainsworth, S.T. Boogert, G.E. Boorman
    Royal Holloway, University of London, Surrey
  • Y. Honda, T. Tauchi, N. Terunuma
    KEK, Ibaraki
  • S.H. Kim, Y.J. Park
    PAL, Pohang, Kyungbuk
  • A. Lyapin, B. Maiheu, M. Wing
    UCL, London
  • J. May, D.J. McCormick, S. Molloy, J. Nelson, T.J. Smith, G.R. White
    SLAC, Menlo Park, California
  • S. Shin
    Fermilab, Batavia
  • D. Son
    CHEP, Daegu
  • D.R. Ward
    University of Cambridge, Cambridge
 
 

The ATF2 international collaboration is intending to demonstrate nanometer beam sizes required for the future Linear Colliders. The position of the electron beam focused down at the end of the ATF2 extraction line to a size as small as 35 nm has to be measured with nanometer resolution. For that purpose a special Interaction Point(IP) beam position monitor (BPM) was designed. In this paper we report on the features of the BPM and electronics design providing the required resolution. We also consider the results obtained with BPM triplet which was installed in the ATF beamline and the first data from ATF2 commissioning runs.

 
TH5RFP084 Nanometer Order of Stabilization for Precision Beam Size Monitor (Shintake Monitor) 3645
 
  • T. Kume, S. Araki, Y. Honda, T. Okugi, T. Tauchi, N. Terunuma, J. Urakawa
    KEK, Ibaraki
  • B. Bolzon, N. Geffroy, A. Jeremie
    IN2P3-LAPP, Annecy-le-Vieux
  • Y. Kamiya
    ICEPP, Tokyo
  • S. Komamiya, M. Oroku, T.S. Suehara, T. Yamanaka
    University of Tokyo, Tokyo
 
 

The ATF2, accelerator test facility has been developed confirming techniques for obtaining super low emittance beam for future particle accelerators. Here, the converged beam size is designed to be 37 nm, and a precision beam size monitor using interference fringes as a reference called Shintake monitor is used for measuring it. In order to measure the beam size with resolution of better than 10%, relative position between the beam and the interference fringes should be stabilized within few nanometers. Highly rigid tables and mounts for the Shintake monitor and final focusing magnets are adopted with highly rigid floor to ensure relative position stability. Then, the Shintake monitor can be stabilized against the beam, since the beam fluctuates coherently with the final focusing magnets. On the other hand the interference fringes are stabilized against the Shintake monitor with precise phase control system. As a result, relative position between the beam and the interference fringes is stabilized based on rigidity of tables, mounts, and floor between them. We will present our conception for stabilization and results of vibration measurements for the Shintake monitor.

 
TH6REP023 Micron Size Laser-Wire System at the ATF Extraction Line, Recent Results and ATF-II Upgrade 3997
 
  • A.S. Aryshev, V. Karataev
    JAI, Egham, Surrey
  • G.A. Blair, S.T. Boogert, G.E. Boorman, A. Bosco, L.C. Deacon
    Royal Holloway, University of London, Surrey
  • L. Corner, N. Delerue, B. Foster, F. Gannaway, D.F. Howell, L.J. Nevay, M. Newman, R. Senanayake, R. Walczak
    OXFORDphysics, Oxford, Oxon
  • H. Hayano, N. Terunuma, J. Urakawa
    KEK, Ibaraki
 
 

Funding: STFC LC-ABD Collaboration, Royal Society, Daiwa Foundation, Commission of European Communities under the 6th Framework Programme Structuring the European Research Area, contract number RIDS-011899


The KEK Accelerator Test Facility (ATF) extraction line laser-wire system has been upgraded, enabling the measurement of micron scale transverse size electron beams. The most recent measurements using the upgraded system are presented, including the major hardware upgrades to the laser transport, the laser beam diagnostics line, and the mechanical control systems.

 
TH6REP025 Development of the S-Band BPM System for ATF2 4003
 
  • A. Lyapin, B. Maiheu, M. Wing
    UCL, London
  • R. Ainsworth, A.S. Aryshev, S.T. Boogert, G.E. Boorman, S. Molloy
    Royal Holloway, University of London, Surrey
  • A. Heo, E.-S. Kim, H.-S. Kim
    Kyungpook National University, Daegu
  • Y. Honda, T. Tauchi, N. Terunuma
    KEK, Ibaraki
  • D.J. McCormick, J. Nelson, G.R. White
    SLAC, Menlo Park, California
  • S. Shin
    Fermilab, Batavia
  • D.R. Ward
    University of Cambridge, Cambridge
 
 

The ATF2 international collaboration is intending to demonstrate nanometre beam sizes required for the future Linear Colliders. An essential part of the beam diagnostics needed to achieve this goal is the high resolution cavity beam position monitors (BPMs). In this paper we report on the S-band system installed in the final focus region of the new ATF2 extraction beamline. It only includes 4 BPMs, but they are mounted on the most critical final focus magnets squeezing the beam down to 35 nm. We discuss both the design and the first operational experience with the system.

 
TH6REP028 Development of the C-Band BPM System for ATF2 4009
 
  • S. Molloy, R. Ainsworth, S.T. Boogert, G.E. Boorman
    Royal Holloway, University of London, Surrey
  • A. Heo, E.-S. Kim, H.-S. Kim
    Kyungpook National University, Daegu
  • Y. Honda, T. Tauchi, N. Terunuma
    KEK, Ibaraki
  • A. Lyapin, B. Maiheu, M. Wing
    UCL, London
  • D.J. McCormick, J. Nelson, G.R. White
    SLAC, Menlo Park, California
  • S. Shin
    Fermilab, Batavia
  • D.R. Ward
    University of Cambridge, Cambridge
 
 

The ATF2 international collaboration is intending to demonstrate nanometre beam sizes required for the future Linear Colliders. An essential part of the beam diagnostics needed to achieve that goal is the high resolution cavity beam position monitors (BPMs). In this paper we report on the C-band system consisting of 32 BPMs spread over the whole length of the new ATF2 extraction beamline. We discuss the design of the BPMs and electronics, main features of the DAQ system, and the first operational experience with these BPMs.

 
TH6REP062 Status of the First Commissioning of the Shintake Monitor for ATF2 4093
 
  • T. Yamanaka, S. Komamiya, M. Oroku, T.S. Suehara
    University of Tokyo, Tokyo
  • S. Araki, Y. Honda, T. Kume, T. Okugi, T. Tauchi, N. Terunuma, J. Urakawa
    KEK, Ibaraki
  • Y. Kamiya
    ICEPP, Tokyo
 
 

Commissioning of the ATF/ATF2 project will start in the winter of 2008 to 2009, with the aim of studying beam optics, diagnostic instrumentations, and tuning processes for around 35 nm beam size. The project is the realistic scaled down model of the ILC final focus system, and also, studies in the project offered important findings for future accelerator physics. In this presentation, we will present about the status of the first commissioning of the Shintake monitor for ATF2. The monitor is located at the virtual interaction point of the ATF2 (the focus point) to measure beam size. A measurable ranges as a design are from 6 micron down to 20 nm in vertical and down to several microns in horizontal. That wide range allows us to used the detector from the beginning of the beam tuning process. The monitor scheme was originally proposed by T. Shintake and verified using around 60 nm beam at FFTB project. We upgraded the detector system for ATF2 of smaller beam size and implemented a laser wire scheme for horizontal beam size measurement. These additional capabilities are also presented.

 
FR1RAI03 ATF2 Commissioning 4205
 
  • A. Seryi, J.W. Amann, P. Bellomo, B. Lam, D.J. McCormick, J. Nelson, J.M. Paterson, M.T.F. Pivi, T.O. Raubenheimer, C.M. Spencer, M.-H. Wang, G.R. White, W. Wittmer, M. Woodley, Y.T. Yan, F. Zhou
    SLAC, Menlo Park, California
  • D. Angal-Kalinin, J.K. Jones
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
  • R. Apsimon, B. Constance, C. Perry, J. Resta-López, C. Swinson
    JAI, Oxford
  • S. Araki, A.S. Aryshev, H. Hayano, Y. Honda, K. Kubo, T. Kume, S. Kuroda, M. Masuzawa, T. Naito, T. Okugi, R. Sugahara, T. Tauchi, N. Terunuma, J. Urakawa, K. Yokoya
    KEK, Ibaraki
  • S. Bai, J. Gao
    IHEP Beijing, Beijing
  • P. Bambade, Y. Renier, C. Rimbault
    LAL, Orsay
  • G.A. Blair, S.T. Boogert, V. Karataev, S. Molloy
    Royal Holloway, University of London, Surrey
  • B. Bolzon, N. Geffroy, A. Jeremie
    IN2P3-LAPP, Annecy-le-Vieux
  • P. Burrows
    OXFORDphysics, Oxford, Oxon
  • G.B. Christian
    ATOMKI, Debrecen
  • J.-P. Delahaye, D. Schulte, R. Tomás, F. Zimmermann
    CERN, Geneva
  • E. Elsen
    DESY, Hamburg
  • E. Gianfelice-Wendt, M.C. Ross, M. Wendt
    Fermilab, Batavia
  • A. Heo, E.-S. Kim, H.-S. Kim
    Kyungpook National University, Daegu
  • J.Y. Huang, W.H. Hwang, S.H. Kim, Y.J. Park
    PAL, Pohang, Kyungbuk
  • Y. Iwashita, T. Sugimoto
    Kyoto ICR, Uji, Kyoto
  • Y. Kamiya
    ICEPP, Tokyo
  • S. Komamiya, M. Oroku, T.S. Suehara, T. Yamanaka
    University of Tokyo, Tokyo
  • A. Lyapin
    UCL, London
  • B. Parker
    BNL, Upton, Long Island, New York
  • T. Sanuki
    Tohoku University, Graduate School of Science, Sendai
  • A. Scarfe
    UMAN, Manchester
  • T. Takahashi
    Hiroshima University, Graduate School of Science, Higashi-Hiroshima
  • A. Wolski
    Cockcroft Institute, Warrington, Cheshire
 
 

ATF2 is a final-focus test beam line that attempts to focus the low-emittance beam from the ATF damping ring to a beam size of about 37 nm, and at the same time to demonstrate nm beam stability, using numerous advanced beam diagnostics and feedback tools. The construction is well advanced and beam commissioning of ATF2 has started in the second half of 2008. ATF2 is constructed and commissioned by ATF international collaborations with strong US, Asian and European participation.

 

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