SuperB Accelerator Overview and Status

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Presentation transcript:

SuperB Accelerator Overview and Status John T. Seeman for the SuperB Accelerator Team 2nd IRC Meeting Rome April 29-30, 2008

Outline SuperB project Accelerator talks Luminosity and beam-beam Beam dynamics studies Conclusions

SuperB Project SuperB aims at the construction of a very high luminosity (1-4 x 1036 cm-2 s−1 ) asymmetric e+e− Flavour Factory, with possible location at the campus of the University of Rome Tor Vergata, near the INFN Frascati National Laboratory.

SuperB Accelerator Contributors M. E. Biagini, M. Boscolo, T. Demma, A. Drago, S. Guiducci, M. Preger, P. Raimondi, S. Tomassini, C. Vaccarezza, M. Zobov (INFN/LNF, Italy) Y. Cai, A. Fisher, S. Heifets, A. Novokhatski, M.T. Pivi, J. Seeman, M. Sullivan, U. Wienands, W. Wittmer (SLAC, US) T. Agoh, K. Ohmi, Y. Ohnishi (KEK, Japan) I. Koop, S. Nikitin, E. Levichev, P. Piminov, D. Shatilov (BINP, Russia) Wolski (Liverpool University, UK) M. Venturini (LBNL, US) S. Bettoni (CERN, Switzerland) A. Variola (LAL/Orsay, France) E. Paoloni, G. Marchiori (Pisa University, Italy)

SuperB footprint on Tor Vergata site SuperB Ring (about 1800m) SPARX Roman Villa 100m SuperB Injector (about 400m) SuperB Main Building

Super-B New Parameters Beam-beam transparency conditions in red

Comparison of SuperB to SuperKEKB Parameter SuperB Super- KEKB Energy GeV 4x7 3.5x8 Luminosity 1036 /cm2/s 1.0 to 2.0 0.4 to 0.8 Beam Currents Amps 1.9x1.9 10.0x4.0 by* mm 0.22 3.0 bx* cm 3.5x2.0 20. Crossing angle (full) mrad 48 30 RF power (AC line) MW 17 to 25 80 to 90 Tune shifts (x/y) 0.0004/0.2 0.4/0.8

The SuperB Process (M. Biagini) 9 11 3 4 6 9 11 12 5 5 7 7 9 11 12 2th Joint Japan-US SuperB-Factory Workshop, Hawaii, US International SuperB Steering Committee established 4th SuperB Workshop, Villa Mondragone, Italy Accelerator test started at DAFNE, LNF, Italy International SuperB Study Group formed 5th SuperB Workshop in Paris, France International Review Committee setup CDR presented to INFN Management Detector R&D workshop, SLAC,US ICFA08 Workshop at BINP, Russia CERN strategy group presentation Physics retreat at Valencia, Spain 2nd SuperB Workshop, LNF, Italy 3rd SuperB Workshop, SLAC, US 1st Accelerator retreat, SLAC, US 2th Accelerator retreat, SLAC, US 1st SuperB Workshop, LNF, Italy SuperB meeting, Daresbury,UK 2nd IRC meeting, Rome, Italy SuperB Meeting in Elba, Italy 1st IRC meeting, LNF, Italy Mini MAC, EPAC08, Italy 2nd Meeting with ECFA CDR presented to ECFA CDR writing started CDR published 9 11 3 4 6 9 11 12 5 5 7 7 9 11 12 1 2 3 4 4 6 6 .. Month 2005 2006 2007 2008

Topics presented at this IRC meeting Overview (J. Seeman) Daphne crab-waist studies (P. Raimondi) Lattice upgrades (M. Biagini) Beam dynamics and magnet tolerances (U. Wienands) Spin manipulation (U. Wienands) RF, injection, operations, vibration (J. Seeman)

Basic concepts B-Factories (PEP-II and KEKB) reached very high luminosity (>1034 s-1 cm-2 ), but to increase L of ~ two orders of magnitude bordeline parameters are needed, such as: Very high currents Smaller damping time Difficult and costly Shorter bunches operation Crab cavities for head-on collision Higher power SuperB exploits an alternative approach, with a new IP scheme: Small beams (ILC-DR like) Large Piwinski angle and “crab waist” Currents comparable to present Factories

Crab-waist Studies at DAFNE at INFN Frascati P. Raimondi et al: DAFNE upgrade with improved interaction region to focus tighter the beams at IP and have a “large” crossing angle  large Piwinski angle Features: Smaller collision area Lower b*y No parasitic crossings No synchro-betatron resonances due to the crossing angle “Crab Waist” sextupoles Results very encouraging so far with improved tunes shifts and higher luminosity with smaller currents.

DAFNE tests showing Enhanced beam-beam Tune shifts at lower Currents (Raimondi et al) (March 2008)

IP beam distributions for KEKB SuperB beams are focused in the y-plane 100 times more than in the present factories, thanks to: - small emittances - small beta functions larger crossing angle Tune shifts and longitudinal overlap are greatly reduced y(mm) x(mm) z(mm) KEKB SuperB I (A) 1.7 2. by* (mm) 6 0.22/0.39 bx* (mm) 300 22/39 sy* (mm) 3 0.039 sx* (mm) 80 10/6 sz (mm) 5 L (cm-2s-1) 1.7x1034 1.x1036 IP beam distributions for SuperB y(mm) x(mm) z(mm)

Beams distribution at IP E. Paoloni Crab sextupoles OFF Without Crab-sextupoles waist line is orthogonal to the axis of one bunch Crab sextupoles ON With Crab-sextupoles waist moves to the axis of other beam All particles from both beams collide in the minimum by region, with a net luminosity gain

SuperB transparency condition To have equal tune shifts with asymmetric energies in PEP-II and KEKB the “design” beam currents ratio is: I+/I- ~ E-/E+ Due to SuperB large crossing angle, new conditions are possible: LER and HER beams can have different emittances and b* and equal currents  Present B-factories SuperB

Beam-beam Luminosity Tune Plane Scan (crab=0.8/q, sz = 7 mm; 3x1010 particles) Lmax = 2.2x1036 cm-2 s-1 2D and 3D surface luminosity plots. The red color on the contour plot corresponds to the highest luminosity while the blue is the lowest. Each contour line corresponds to a 10% luminosity reduction. D. Shatilov, M. Zobov, IV SuperB Workshop

RF power estimate Including synchrotron radiation, HOMs and RF power with 50% klystron efficiency A. Novokhatski CDR parameters New parameters

Lattice overview LNF, BINP, KEK, LAL, CERN The SuperB lattice as described in the Conceptual Design Report is the result of an international collaboration between experts from BINP, Cockcroft Institute, INFN, KEKB, LAL/Orsay, SLAC Simulations were performed in many labs and with different codes: LNF, BINP, KEK, LAL, CERN The design is flexible but challenging and the synergy with the ILC Damping Rings which helped in focusing key issues, will be important for addressing some of the topics Further studies after the CDR completion led to an evolution of the lattice to fit the Tor Vergata Site and to include polarization manipulation hardware.

Arc cells layout M. Biagini LER HER Cell #1 Cell #1 Cell #2 Cell #2

Final Focus optical functions (Öb) Crab sextupoles LER: bx* = 35 mm, by* = 220 m HER: bx* = 20 mm, by* = 390 m M. Biagini

HER spin manipulation hardware Spin rotators in the HER Full HER lattice Wittmer, Wienands, Biagini

(M. Sullivan)

Lattice layout, PEP-II magnets reuse Lmag (m) 0.45 5.4 PEP HER - 194 PEP LER SBF HER 130 SBF LER 224 18 SBF Total 148 Needed 30 Total length 1800 m 280 m 20 m Dipoles Available Needed Quads Lmag (m) 0.56 0.73 0.43 0.7 0.4 PEP HER 202 82 - PEP LER 353 SBF HER 165 108 2 SBF LER 88 SBF Total 253 216 4 Needed 51* 134 Lmag (m) 0.25 0.5 PEP HER/LER 188 - SBF Total 372 4 Needed 184 Sexts All PEP-II magnets are reused. Dimensions and fields are properly sized.

Polarization Polarization of one beam is included in SuperB Either energy beam could be the polarized one The LER would be less expensive, the HER easier HER was chosen for now. Longitudinal polarization times and short beam lifetimes indicate a need to inject vertically polarized electrons. The plan is to use a polarized e- source similar to the SLAC SLC source. There are several possible IP spin rotators: Solenoids look better at present (vertical bends give unwanted vertical emittance growth) Expected longitudinal polarization at the IP of about 87%(inj) x 97%(ring)=85%(effective) Polarization section implementation in lattice: in progress with initial success

Example of spin rotators U. Wienands Proof-of-principle scheme No V-emittance growth. Maybe possible to incorporate into lattice using the Final Focus bends to provide the spin rotation. Work in progress

Accelerator & site cost estimate Note: site cost estimate not as detailed as other estimates.

Schedule Overall schedule dominated by: Site construction PEP-II/BaBar disassembly, transport, and reassembly The goal is to reach the commissioning phase after about 5 years from the start of the project.

Conclusions The initial SuperB design meets the goals requested by the experimenters. IR polarization rotators have now been added to the lattice. Beam dynamics issues are receiving a fresh look. The next phase for the accelerator group is to form a team to complete the Technical Design Report.