'2x10 10' presentation slideshows

Compton Scheme Overview Polarized e + Source for ILC

Compton Scheme Overview Polarized e + Source for ILC. Tsunehiko OMORI (KEK). Snowmass2005, Snowmass Colorado 18/Aug/2005. Why Compton Scheme?. i) Positron Polarization. ii) Full energy/intensity e - beam is NOT necessary to produce positrons. Therefore, Electron and positron

625 views • 47 slides

What IS Matter ?

431 views • 27 slides

What IS Matter ?

380 views • 27 slides

Polarized Positron Source using Backward Compton Scattering

Polarized Positron Source using Backward Compton Scattering. Tohru Takahashi Hiroshima University ???? ????. 2007/11/5. Why polarized positrons. electrons are polarized,,,,,, ? choose helicity of its counter part. if unpolarized e+. a half of the beam is thrown away.

434 views • 27 slides

Laser Based Polarized e + Source for ILC

Laser Based Polarized e + Source for ILC. Tsunehiko OMORI (KEK). 8th ACFA LCWS@ Daegu 11-14/Jul/2005. Why laser based?. i) Full energy/intensity e - beam is NOT necessary to produce positrons. Therefore, Electron and positron systems remain independent.

349 views • 26 slides

Lyman Break Galaxies as Markers for Large Scale Structure at z=5

Lyman Break Galaxies as Markers for Large Scale Structure at z=5. Elizabeth Stanway University of Bristol With Malcolm Bremer, Luke Davies, Matt Lehnert, Mark Birkinshaw, Chris Carilli, Alain Omont. The ESO Remote Galaxy Survey. Targets the 10 EDisCS Survey cluster fields (VRIJK)

330 views • 21 slides

Paperwork

240 views • 12 slides

Paperwork

449 views • 12 slides

Paperwork

212 views • 12 slides

V rf =2.55 MV

CLIC e+ damping ring. layout. performance with 0.5% coupling & wiggler period l w =10 cm. equilibrium emittances. V rf =3.03 MV. V rf =2.55 MV. beam-based tuning & tolerances being studied. M. Korostelev, CERN & U Lausanne. why is CLIC emittance smaller than NLC value?.

123 views • 3 slides