Скачать презентацию Depolarisation Effects at the ILC Cockcroft Institute L Скачать презентацию Depolarisation Effects at the ILC Cockcroft Institute L

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Depolarisation Effects at the ILC Cockcroft Institute L I Malysheva, D P Barber, I Depolarisation Effects at the ILC Cockcroft Institute L I Malysheva, D P Barber, I R Bailey, J A Clarke, J B Dainton, G A Moortgat-Pick, D J Scott 2/10/06 The University of Liverpool/Cockcroft Institute L I Malysheva

Introduction n n International Linear Collider (ILC)----new life of an old idea. A high Introduction n n International Linear Collider (ILC)----new life of an old idea. A high intensity polarised e+ beam is essential for realising the total physics potential of the ILC (http: //www. ippp. dur. ac. uk/~gudrid/source/ to be published) in Physical Reports) n n Delivery of the beam polarisation to the interaction region must be robust and without loss of intensity Reliable software tools are required to optimise the machine for polarisation as well as luminosity 2/10/06 The University of Liverpool/Cockcroft Institute L I Malysheva

ILC layout (undulator positron source) polarised e-/(e+) beam Depolarisation? ? Misalignments, Synchrotron radiation, Spin ILC layout (undulator positron source) polarised e-/(e+) beam Depolarisation? ? Misalignments, Synchrotron radiation, Spin precession, Resonances, bunch- bunch effects … 2/10/06 The University of Liverpool/Cockcroft Institute L I Malysheva

Spin behaviour in guide fields SPIN PRECESSION ( THOMAS-BARGMANN-MICHEL-TELEGDI) n where Synchrotron Radiation 2/10/06 Spin behaviour in guide fields SPIN PRECESSION ( THOMAS-BARGMANN-MICHEL-TELEGDI) n where Synchrotron Radiation 2/10/06 SPIN DIFFUSION The University of Liverpool/Cockcroft Institute L I Malysheva

Damping rings for the ILC n n n In ideal Damping Ring depolarising effects Damping rings for the ILC n n n In ideal Damping Ring depolarising effects are expected to be negligible Enhancement of synchrotron radiation (wigglers) might lead to the depolarisation effects Two out of seven reference lattices were selected: OCS 6 km (circle) and TESLA 17 km (dogbone) 2/10/06 The University of Liverpool/Cockcroft Institute L I Malysheva

DAMPING RING damping time (msec) n S –T effect negligible n No equilibrium polarisation DAMPING RING damping time (msec) n S –T effect negligible n No equilibrium polarisation (evolution of spin distribution over a few damping times) n MERLIN and SLICKTRACK n STORAGE RING n storage time (hours) S –T effect significant Equilibrium polarisation (depolarisation rate can be “measured” ) n More then 10 different codes available n n (Handbook of Accelerator Physics and Engineering) 2/10/06 The University of Liverpool/Cockcroft Institute L I Malysheva

Computer Simulation n n Misalignments were introduced STEP 1 (SLICK): linearised orbital and spin Computer Simulation n n Misalignments were introduced STEP 1 (SLICK): linearised orbital and spin motion. Reference point as well as an energy scan STEP 2 (SLICKTRACK): Monte-Carlo simulation of the effects of synchrotron radiation, i. e. evolution of the spin distribution over a few damping times including full 3 -D spin motion NO significant depolarising effects have been detected confirming the earlier works 2/10/06 The University of Liverpool/Cockcroft Institute L I Malysheva

Spin-orbit resonances n n Spin tune on the closed orbit : First order resonances: Spin-orbit resonances n n Spin tune on the closed orbit : First order resonances: OCS ring depolarisation time with misalignments 2/10/06 The University of Liverpool/Cockcroft Institute L I Malysheva

Mean square angular deviation from the equilibrium direction mrad**2 OCS Spin Diffusion at 4. Mean square angular deviation from the equilibrium direction mrad**2 OCS Spin Diffusion at 4. 8 Ge. V turns 2/10/06 The University of Liverpool/Cockcroft Institute L I Malysheva

Mean square angular deviation from the equilibrium direction mrad**2 OCS Spin Diffusion at 5. Mean square angular deviation from the equilibrium direction mrad**2 OCS Spin Diffusion at 5. 066 Ge. V for spins initially at 100 mrad from turns 2/10/06 The University of Liverpool/Cockcroft Institute L I Malysheva

Beam Delivery System (BDS) n n Beam transport to the Interaction Region via bending Beam Delivery System (BDS) n n Beam transport to the Interaction Region via bending and focusing magnets. The 2 -mrad beam line selected (spin precession ) SLICKTRACK NO noticeable depolarisation (even with misalignments) 2/10/06 11 mrad NLC-style Big Bends IR 2 2 mrad IR 1 20 mrad Copy from BDS ILC@SLAC presentation The University of Liverpool/Cockcroft Institute L I Malysheva

Beam-Beam Interactions n n CAIN bunch-bunch depolarisation: survey of theoretical uncertainties complete. Studies of Beam-Beam Interactions n n CAIN bunch-bunch depolarisation: survey of theoretical uncertainties complete. Studies of possible ILC beam parameters: Theoretical work ongoing into n Validity of T-BMT equation in strong fields n validity of equivalent photon approximation (EPA) for incoherent pair production processes n higher-order processes n macro-particle dynamics Gudrid Moortgat [g. a. moortgat-pick@durham. ac. uk] 2/10/06 The University of Liverpool/Cockcroft Institute L I Malysheva

Conclusions n n n DR: New lattice design + NEW LAYOUT!! (under discussion) … Conclusions n n n DR: New lattice design + NEW LAYOUT!! (under discussion) … we will maintain a rolling study to include extra effects as necessary BDS: Include non-linear optics Beam-beam effects: CAIN code will be updated and a comparison with code GUINEA-PIG 2/10/06 The University of Liverpool/Cockcroft Institute L I Malysheva