Continued discussions with Alessandra Lombardi as new LCF380 study leader at CERN
Transition into organisation structure for LCF380 study is in preparation
TF Machine design, BDS, beam dynamics, global performance, S2E simulations
Setup lattice repository, incl. latest ILC & CLIC lattices for reference
CLIC lattice is available at CERN: https://gitlab.cern.ch/clic-simulations
Andrea makes united repository (CERN gitlab) with ILC TDR, ILC latest, CLIC latest, LCF
Re-assess (horizontal) emittance budget:
Natural emittance of DR => Yannis looks into first estimate based on https://bitbucket.org/whitegr/ilc-lattices/src/master
Emittance transport RTML, ML, BDS
Main linac x-ing angle:
Define constraints / boundary conditions from beam optics
Match with siting constraints (with TF CFS)
Fix value
2-BDS design and L*:
Does CLIC-like approach work for ILC-like beam parameters?
Conceptual design of switch yard
Longitudinal displacement required / possible? => LCVision document
Decide L* for the 2 IPs [detectors fine with ~4m (ILC-like) L*, larger no problem, i.e. can be any value between CLIC and ILC L* :) ]
IP cavern (with TF CFS):
1 or 2 caverns?
Longitudinal and transverse separation of IPs: minimum needed for 2 caverns / maximum possible for 1 cavern?
=> LCVision (Terunuma-san, page 78 of arXiv:2503.19983): 30m for transverse only, see also the two slide decks from Angeles & Rogelio linked under “discussion"
Extraction line incl dump locations
can this be re-used (with slight modifications?)?
Where to locate dumps for 2 BDS, need “3D approach” (with TF CFS)
Downstream instrumentation
Photon dump location for undulator source?
Design spin rotators for train-by-train adjustment of spin angle at 5 GeV such that Pz = max at either of the two IPs, for all final beam energies
Luminosity / polarisation risk assessment: S2E simulations, including tolerances, misalignments etc pp
Z pole:
Part of staging concept?