A merged quadrupole-calorimeter for CEPC
The luminosity [Formula: see text] of colliding beams in a storage ring such as CEPC depends strongly on [Formula: see text], the half-length of the free space centered on the intersection point (IP). [Formula: see text] is also the length from the IP to the front edges of the two near-in quadrupoles that are focusing the counter-circulating beams to the IP spot. The detector length cannot, therefore, exceed [Formula: see text]. Since [Formula: see text] increases strongly with decreasing [Formula: see text], there is incentive for reducing [Formula: see text]; but this requires the detector to be shorter than desirable. This paper proposes a method for integrating these adjacent quadrupoles into the particle detector to retain (admittedly degraded) active particle detection of those forward going particles that would otherwise be obscured by the quadrupole. A gently conical quadrupole shape is more natural for merging the quadrupole into the particle detector than is the analytically exact cylindrical shape. This is true whether or not the calorimeter is integrated. It will be the task of accelerator physicists to determine the extent to which deviation from the pure quadrupole field compromises (or improves) accelerator performance. Superficially, both the presence of strongest gradient close to the IP and largest aperture farther from the IP seem to be advantageous. A tentative design for this merged, quadrupole-calorimeter is given.