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08:20
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Participation of the FCC Physics Detector and Experiments to Snowmass.21
()
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08:25
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A framework and goals for FCC-hh physics studies at Snowmass 2021
()
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08:30
|
A selection of benchmark studies at FCC-ee
()
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08:35
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Physics at High Energy eh and hh Experiments
()
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08:40
|
Energy Frontier eh Scattering - LHeC and FCC-eh
()
|
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08:50
|
Contributions to the accelerator frontier
(until 09:58)
()
|
|
08:50
|
FCC-ee as Z, W and H factory
()
|
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08:51
|
FCC-ee upgrade to top factory
()
|
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08:52
|
Precision Energy Calibration for a Future Circular Electron-Positron Collider
()
|
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08:53
|
Monochromatized direct s-channel Higgs production in e+e- at sqrt(s)=125 GeV
()
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08:54
|
Elements for FCC electron and positron storage rings
()
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08:55
|
Superconducting RF for CW Synchrotrons and ERLs
()
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08:56
|
Higher Efficiency High Power RF Generation
()
|
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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
|
Contributions to the Energy Frontier
(until 09:22)
()
|
|
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
|
Contributions to the Energy Frontier
(until 09:55)
()
|
|
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
|
Contributions to the Instrumentation Frontier
(until 11:00)
()
|
|
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
|
Contributions to the Instrumentation Frontier
(until 12:00)
()
|
|
11:00
|
Detector solutions for Lepton-hadron Scattering based on the LHC and FCC
()
|
