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Wang, M.-H.

Paper Title Page
WE5RFP018 Reduction of Beam Emittance of PEP-X Using Quadruple Bend Achromat Cell 2306
 
  • M.-H. Wang, Y. Cai, R.O. Hettel, Y. Nosochkov
    SLAC, Menlo Park, California
 
 

Funding: Work supported by the U.S. Department of Energy under contract number DE-AC02-76SF00515


SLAC National Accelerator Laboratory is studying an option of building a high brightness synchrotron light source machine, PEP-X, in the existing PEP-II tunnel*,**. By replacing 6 arcs of FODO cells of PEPII High Energy Ring (HER) with two arcs of DBA and four arcs of TME and installation of 89.3 m long damping wiggler an ultra low beam emittance of 0.14 nm-rad (including intra-beam scattering) at 4.5 GeV is achieved. In this paper we study the possibility to further reduce the beam emittance by releasing the constraint of the dispersion free in the DBA straight. The QBA (Quadruple Bend Achromat) cell is used to replace the DBA. The ratio of outer and inner bending angle is optimized. The dispersion function in the non-dispersion straight is controlled to compromise with lower emittance and beam size at the dispersion straight. An undulator of period length 23 mm, maximum magnetic field of 1.053 T, and total periods of 150 is used to put in the 30 straights to simulate the effects of these IDs on the beam emittance and energy spread. The brightness including all the ID effects is calculated and compared to the original PEP-X design.


*R. Hettel et al., “Ideas for a Future PEP-X Light Source”, EPAC08, p.2031(2008).
**M-H Wang et al., “Lattice Design of PEP-X as a Light Source Machine at SLAC”, EPAC08, p.2127(2008).

 
WE5RFP015 Concepts for the PEP-X Light Source 2297
 
  • R.O. Hettel, K.L.F. Bane, K.J. Bertsche, Y. Cai, A. Chao, V.A. Dolgashev, J.D. Fox, X. Huang, Z. Huang, T. Mastorides, C.-K. Ng, Y. Nosochkov, A. Novokhatski, T. Rabedeau, C.H. Rivetta, J.A. Safranek, J. Seeman, J. Stohr, G.V. Stupakov, S.G. Tantawi, L. Wang, M.-H. Wang, U. Wienands, L. Xiao
    SLAC, Menlo Park, California
  • I. Lindau
    Stanford University, Stanford, California
  • C. Pellegrini
    UCLA, Los Angeles, California
 
 

Funding: This work was supported by the Director, Office of Science, Office of Basic Energy Sciences, of the U.S. Department of Energy under Contract No. DE-AC02-76SF00515.


SSRL and SLAC groups are developing a long-range plan to transfer its evolving scientific programs from the SPEAR3 light source to a much higher performing photon source that would be housed in the 2.2-km PEP-II tunnel. While various concepts for the PEP-X light source are under consideration, including ultimate storage ring and ERL configurations, the present baseline design is a very low-emittance storage ring. A hybrid lattice has DBA or QBA cells in two of the six arcs that provide a total ~30 straight sections for ID beam lines extending into two new experimental halls. The remaining arcs contain TME cells. Using ~100 m of damping wigglers the horizontal emittance at 4.5 GeV would be ~0.1 nm-rad with >1 A stored beam. PEP-X will produce photon beams having brightnesses near 1022 at 10 keV. Studies indicate that a ~100-m undulator could have FEL gain and brightness enhancement at soft x-ray wavelengths with the stored beam. Crab cavities or other beam manipulation systems could be used to reduce bunch length or otherwise enhance photon emission properties. The present status of the PEP-X lattice and beam line designs are presented and other implementation options are discussed.

 
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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