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FCC-hh parameter overview.
Hadron Collider (FCC-hh) Baseline V1.0 Parameters (30 June 2020)
This page contains the latest FCC-hh baseline parameters. Previous versions are linked at the bottom of the page.
FCC-hh Parameter |
Unit |
Initial |
Normal |
Main parameters and geometrical aspects |
c.m. Energy |
TeV |
100 |
Circumference C |
km |
97.75 |
Dipol field |
T |
<16 |
Arc filling factor |
|
0.8 |
Straight sections |
|
6 × 1400 m + 2 × 2800 m |
Number of IPs |
|
2+2 |
Injection energy |
TeV |
3.3 |
Physics performance and beam parameters |
Peak luminosity * |
1034 cm-2 s-1 |
5.0 |
<30.0 |
Optimum average integrated lumi/day* |
fb-1 |
2.2 |
8 |
Assumed turnaround time |
h |
5 |
4 |
Target turnaround time |
h |
2 |
2 |
Peak no. of inelastic events/crossing |
|
171 |
1026 |
Total/inelastic cross section σ proton |
mbarn |
153/108 |
Luminous region RMS length |
cm |
5.7 |
5.7 |
Distance IP to first quadrupole* |
m |
40 |
40 |
Beam parameters |
Number of bunches n |
|
10 400 |
Bunch spacing |
ns |
25 |
Bunch population N |
1011 |
1.0 |
Nominal transverse normalised emittance |
μm |
2.2 |
2.2 |
Number of IPs contributing to ∆Q |
|
2 + 2 |
2 |
Maximum total b-b tune shift ∆Q |
|
0.011 |
0.03 |
Beam current |
A |
0.5 |
RMS bunch length |
cm |
8 |
IP beta function |
m |
1.1 |
0.3 |
RMS IP spot size |
μm |
6.8 |
3.5 |
Full crossing angle |
μrad |
91 |
200** |
Other beam and machine parameters |
Stored energy per beam |
GJ |
8.4 |
SR power per ring |
MW |
2.4 |
Arc SR heat load |
W/m/aperture |
29 |
Energy loss per turn |
MeV |
4.67 |
Critical photon energy |
keV |
4.3 |
Longitudinal emittance damping time |
h |
0.5 |
Transverse emittance damping time |
h |
1.0 |
Dipole coil aperture |
mm |
50 |
Minimum arc beam half aperture |
mm |
13 |
Installed RF voltage (400.79 MHz) |
MV |
48 |
Harmonic number |
|
130 680 |
* For the nominal parameters, the peak luminosity is reached during the run.
The values refer to the baseline 25 ns bunch spacing option.
** The crossing angle will be compensated using the crab crossing scheme.
--
JohannesGutleber - 2021-01-12