Name: Repository for the FCC LOIs submitted to Snowmass
Start: 2020-09-02T08:20:00+02:00
End: 2020-09-02T14:01:00+02:00
Location: No location set

Repository for the FCC LOIs submitted to Snowmass

Wednesday 2 September 2020 - 08:20

Monday 31 August 2020
Tuesday 1 September 2020
Wednesday 2 September 2020

08:20 Participation of the FCC Physics Detector and Experiments to Snowmass.21
Participation of the FCC Physics Detector and Experiments to Snowmass.21
08:20 - 08:22

08:25 A framework and goals for FCC-hh physics studies at Snowmass 2021
A framework and goals for FCC-hh physics studies at Snowmass 2021
08:25 - 08:26

08:30 A selection of benchmark studies at FCC-ee
A selection of benchmark studies at FCC-ee
08:30 - 08:32

08:35 Physics at High Energy eh and hh Experiments
Physics at High Energy eh and hh Experiments
08:35 - 08:36

08:40 Energy Frontier eh Scattering - LHeC and FCC-eh
Energy Frontier eh Scattering - LHeC and FCC-eh
08:40 - 08:41
08:50 Contributions to the accelerator frontier
Contributions to the accelerator frontier
08:50 - 09:58
Contributions

08:50 FCC-ee as Z, W and H factory

08:51 FCC-ee upgrade to top factory

08:52 Precision Energy Calibration for a Future Circular Electron-Positron Collider

08:53 Monochromatized direct s-channel Higgs production in e+e- at sqrt(s)=125 GeV

08:54 Elements for FCC electron and positron storage rings

08:55 Superconducting RF for CW Synchrotrons and ERLs

08:56 Higher Efficiency High Power RF Generation

08:57 Optimizing the FCC-hh Hadron Collider

08:58 Ultra-radiation-transparent Superconducting Detector Magnets for High Energy Physics

08:59 PERLE a ‘Stepping Stone’ for the Next Generation ERLs
09:00 FCC-ee
FCC-ee
09:00 - 09:22
Contributions

09:00 Measurement of the Z lineshape at FCC-ee

09:01 Electroweak Heavy Flavour (bottom, charm,tau) at the FCC-ee

09:02 Searches for Long-Lived Particles at the FCC-ee

09:03 Charged Lepton Flavour Violation at the FCC-ee

09:04 Tau exclusive branching fractions and tau polarisation observables at the FCC-ee

09:05 Tau lepton properties and lepton universality measurements at the FCC-ee

09:06 Perspectives for high-precision αS(m2Z) determinations from future e+e− measurements at the FCC-ee

09:07 High-precision αS(m2Z) determinations from future FCC-ee e+e− → hadrons data below the Z peak

09:08 Measurement of the W mass and width at FCC-ee

09:09 Measurement of Higgs parameters at FCC-ee

09:10 Higgs boson coupling measurements to charm quarks at FCC-ee

09:11 Determination of the HZγ effective coupling at FCC-ee

09:12 The invisible Higgs branching fraction at FCC-ee

09:13 Top quark physics at FCC-ee

09:14 Search for new scalars at FCC-ee

09:15 The effective theory of the see-saw portal at future lepton colliders

09:16 Heavy-quark physics at FCC-ee: CP-violation

09:17 Heavy quark Physics at FCC-ee, rare decays
09:30 FCC-eh
FCC-eh
09:30 - 09:55
Contributions

09:30 Top-Quark and Electroweak Physics at LHeC and FCC-eh

09:31 LHeC and FCC-he: Dark Matter

09:32 LHeC and FCC-he: More general explorations

09:33 LHeC and FCC-he: Model specific explorations

09:34 LHeC and FCC-eh: Small-x Physics at Energy Frontier Electron-Proton and Electron-Nucleus Colliders

09:35 PDFs, alphas and Low-x Physics and at Future DIS Facilities
10:00 FCC-ee
FCC-ee
10:00 - 11:00
Contributions

10:00 IDEA detector Letter of Intent

10:01 The IDEA Drift Chamber for a Lepton Collider

10:02 μ-RWELL detector Letter of Intent

10:03 Dual-Readout Calorimetry

10:04 Detector optimisation and detector technology R&D for the CLIC detector and for the CLD detector of FCC-ee
11:00 FCC-eh
FCC-eh
11:00 - 12:00
Contributions

11:00 Detector solutions for Lepton-hadron Scattering based on the LHC and FCC
12:00 Contributions to the computing frontier
Contributions to the computing frontier
12:00 - 13:00
Contributions

12:00 Key4Hep
13:00 Contributions to the theory frontier
Contributions to the theory frontier
13:00 - 14:00
Contributions

13:00 Theory Needs for FCC-ee Part I: Towards high precision EWPO calculations

13:01 Theory Needs for FCC-ee Part II: New methods for SM calculations

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