Probing Nucleon Spin Structure with a Polarized Gamma Beam from Compton Backscattering at FCC-ee
arXiv:2606.04805
Abstract
We present the design of a high-energy polarized gamma-ray facility based on Compton backscattering (CBS) of laser pulses off the FCC-ee full-energy booster beams in the Z, WW, ZH and modes. Saturating the safe value of the kinematic parameter fixes the laser wavelength in each mode and yields backscattered photons up to GeV. The conversion point operates on the booster cycle structure: fully parasitically on the 0.1 s top-up flat-tops ( per bunch crossing, cumulative electron loss per cycle) or, as the baseline, in dedicated extended-flat-top fills inside the idle windows between top-up cycles (, beam loss below 1% per cycle). The collider luminosity is unaffected in both scenarios, and the operational laser pulse energies lie in the sub-millijoule to few-millijoule range. Photon selection is performed event-by-event with a pair spectrometer on the high-energy Compton edge; for the unpolarized booster beam the Compton polarization transfer limits the achievable band-averaged circular polarization, and the selection is set to . We project the sensitivity to the polarized gluon distribution via open-charm photoproduction on an NH dynamically polarized target, including NLO QCD corrections via K-factors and propagating polarized-PDF uncertainties through the 100 Monte Carlo replicas of NNPDFpol2.0. The projected total precision is -, a factor of 4-7 below the total uncertainty of the most precise existing direct measurement (HERMES), at four values of in the medium- region . The facility would set the dominant constraint on in this region, complementary to the low- reach of the Electron-Ion Collider.
18 pages, 8 figures, 8 tables. v2: numerical chain rebuilt on FCC FSR Vol. 2 booster parameters; two operating scenarios; polarization budget revised for the unpolarized booster beam (P_gamma = 0.90); conclusions unchanged