Magnet lattice (in MAD-8 format) |
The VEPP-4 electron-positron collider with the maximal beam energy of 6 GeV has been commissioned in 1979. In 1979-1985, a range of high-energy physics experiments with the MD-1 detector has been performed, including ypsilon-meson study and two-photon physics. To increase the collider luminosity, a modernization has been done in 1986-1994. Principal modifications of the VEPP-4M against the VEPP-4:
The VEPP-4M layout in the PDF format is here.
|
Perimeter | 366.075 m |
Revolution frequency | 818.924 kHz |
Beam energy | 1.5-5.5 GeV |
Momentum compaction factor | 0.0168 |
Betatron tunes, horizontal/vertical | 8.54/7.58 |
Natural chromaticity, horizontal/vertical | -14.5/-20.3 |
Beta-function, maximum/minimum horizontal vertical |
132.25/0.70 m 122.20/0.05 m |
Horizontal dispersion, maximum/minimum | 1.99/-1.48 m |
Aperture in semi-rings | 60x30 mm2 |
Accelerating RF system | |
---|---|
Frequency | 181.10165 MHz |
Harmonic number | 222 |
Number of cavities | 5 |
Maximal amplitude voltage per cavity | 1000 kV |
Maximal RF generator power | 700 kW |
Design beam parameters (E = 1850 MeV) | |
Damping time of ver. betatron oscillation hor. betatron oscillation phase oscillation |
134 ms 139 ms 71 ms |
Horizontal emittance | 24.6 nm·rad |
Energy spread dE/E, r.m.s. | 3.22·10-4 |
Bunch length, r.m.s. | 3 см |
Energy loss per turn | 32 keV |
Synchrotron tune | 0.011 (9.26 kHz) |
At present, the main high-energy physics experiment at the VEPP-4M is precise measurement of the tau-lepton mass at its production threshold. Experiments for accuracy improvement of the measured masses of the psi(2s) and psi(3770) mesons are also continued (the beam energy range is 1840-1900 MeV). In the low energy range (1.5-3.0 GeV), peak luminosity of the collider is 2·1030cm-2s-1. Average rate of KEDR data collection is about 300 nb-1 per week.
Design luminosity at the 6 GeV energy is 4·1031cm-2s-1 with natural beam size; 7·1031см-2с-1 with superconducting damping wigglers; 1032см-2с-1 with additional superconducting RF cavity to decrease bunch length and beta-fuction at the interaction point.