To correct more efficiently the arc dispersion, the exact antisymmetry of the LHC optics is now broken, except in the low-b triplets common to the two rings. A new quadrupole is added between the experimental insertions and the dispersion suppressors and several arc quadrupoles are complemented by a small trim quadrupole. The larger number of parameters gives flexibility to the lattice and allows a partial separation of the optical functions, with a decrease of the total number of quadrupole units. It is possible to change rather freely the phase advances of the arc cells. The nominal tunes are split by 4 units to reduce coupling. The bin boot tuning range in the experimental low-b is significantly increased, allowing e.g. a larger beam sep...
A strategy for optimizing the intersection region of LHC is presented. The quadrupole triplet is mov...
During injection at the LHC the dominant factor of the dynamic aperture comes from the non-linear er...
The geometrical acceptance in the interaction regions of the LHC must be large enough to accommodate...
To optimize the use of space, the LHC insertions combine dispersion matching (arc and ring separatio...
In version 6 of the LHC lattice the pairs of standard arc and additional trim quadrupoles in the dis...
In version 6 of the LHC lattice the pairs of standard arc and additional trim quadrupoles in the dis...
The variation in the field gradient of the LHC arc quadrupoles can not be corrected by the dedicated...
The LHC requires very precise matching of transfer line and LHC optics to minimise emittance blow-up...
Beam crossing schemes in the LHC interaction regions impose non-zero vertical closed orbit in the lo...
In view of the CERN Proton Synchrotron proposed replacement with a new ring (PS2), a detailed optics...
Abstract An excellent match between the SPS, the several kilometres long transfer lines and the LHC ...
In LHC the main contribution to the dynamic aperture is presently (September 1998) that of the ``sys...
Considering a generic double-ring collider, we discuss the matching from an antisymmetric optics in ...
The Large Hadron Collider Project LHC was approved by the CERN Council in December 1994. Commissioni...
The high nominal luminosity of the LHC requires a large number of bunches spaced by about 25 ns. To ...
A strategy for optimizing the intersection region of LHC is presented. The quadrupole triplet is mov...
During injection at the LHC the dominant factor of the dynamic aperture comes from the non-linear er...
The geometrical acceptance in the interaction regions of the LHC must be large enough to accommodate...
To optimize the use of space, the LHC insertions combine dispersion matching (arc and ring separatio...
In version 6 of the LHC lattice the pairs of standard arc and additional trim quadrupoles in the dis...
In version 6 of the LHC lattice the pairs of standard arc and additional trim quadrupoles in the dis...
The variation in the field gradient of the LHC arc quadrupoles can not be corrected by the dedicated...
The LHC requires very precise matching of transfer line and LHC optics to minimise emittance blow-up...
Beam crossing schemes in the LHC interaction regions impose non-zero vertical closed orbit in the lo...
In view of the CERN Proton Synchrotron proposed replacement with a new ring (PS2), a detailed optics...
Abstract An excellent match between the SPS, the several kilometres long transfer lines and the LHC ...
In LHC the main contribution to the dynamic aperture is presently (September 1998) that of the ``sys...
Considering a generic double-ring collider, we discuss the matching from an antisymmetric optics in ...
The Large Hadron Collider Project LHC was approved by the CERN Council in December 1994. Commissioni...
The high nominal luminosity of the LHC requires a large number of bunches spaced by about 25 ns. To ...
A strategy for optimizing the intersection region of LHC is presented. The quadrupole triplet is mov...
During injection at the LHC the dominant factor of the dynamic aperture comes from the non-linear er...
The geometrical acceptance in the interaction regions of the LHC must be large enough to accommodate...