Abstract
We investigate the projected sensitivity to effective dark matter (DM)–diboson interaction during the high luminosity Z-pole and 240 GeV runs at the proposed Circular Electron Positron Collider (CEPC). The proposed runs at the 91.2 GeV e^+e^- center of mass energy offers an interesting opportunity to probe effective dark matter couplings to the Z boson, which can be less stringently tested in non-collider searches. We investigate the prospective sensitivity for dimension 6 and dimension 7 effective diboson operators to scalar and fermion dark matter. These diboson operators can generate semi-visible Z boson decay, and high missing transverse momentum mono-photon signals that can be test efficiently at the CEPC, with a small and controllable Standard Model gamma bar{nu }nu background. Projected sensitivities for the effective gamma Z coupling efficient kappa _{gamma Z}< (1030,hbox {GeV})^{-3}, (1970,hbox {GeV})^{-3} for scalar DM, kappa _{gamma Z}< (360,text {GeV})^{-3}, (540,text {GeV})^{-3} for fermion DM are obtain for 25 hbox {fb}^{-1} and 2.5hbox {ab}^{-1}Z-pole luminosities assuming the optimal low dark matter mass range. We also compare the CEPC sensitivities to current direct and indirect search limits on these effective DM-diboson operators.
Highlights
At colliders, effective interactions allow dark matter (DM) particles to be produced as missing transverse energy (MET) by in association with a mono-jet [7,8,9,10,11,12] or single gauge boson [13,14,15,16,17] final states
photon transverse momentum (PT) (γ ) cut is at 35 (45) GeV for 91.2 (240) GeV runs for scalar DM, PT (γ ) cut is at 30 (35) GeV for 91.2 (240) GeV runs for fermion DM that optimizes the sensitivity for a low mφ,χ φ, χ φ, χ γ γ q q (a) Direct detection φ, χ γ φ∗, χγ (b) Indirect detection
With a focus on the Z -pole energy, the effective DM couplings to the Z boson can be accessed at large luminosity giga-Z and tera-Z runs
Summary
Effective interactions allow DM particles to be produced as missing transverse energy (MET) by in association with a mono-jet [7,8,9,10,11,12] or single gauge boson [13,14,15,16,17] final states. Effective DM–gauge boson operators couple the DM bilinears to one SM gauge boson field. Due to their lower dimensional dependence on the interaction scale, the constraints on single gauge boson–DM operators become increasingly stringent.
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