In this paper, we present a model in which an up-type vector-like quark (VLQ) is charged under a new U (1) d gauge force which kinetically mixes with the SM hypercharge. The gauge boson of the U (1) d is the dark photon, γ d . Traditional searches for VLQs rely on decays into Standard Model electroweak bosons W, Z or Higgs. However, since no evidence for VLQs has been found at the Large Hadron Collider (LHC), it is imperative to search for other novel signatures of VLQs beyond their traditional decays. As we will show, if the dark photon is much less massive than the Standard Model electroweak sector, M γ d M Z , for the large majority of the allowed parameter space the VLQ predominately decays into the dark photon and the dark Higgs that breaks the U (1) d . That is, this VLQ is a "maverick top partner" with nontraditional decays.One of the appeals of this scenario is that pair production of the VLQ at the LHC occurs through the strong force and the rate is determined by the gauge structure. Hence, the production of the dark photon at the LHC only depends on the strong force and is largely independent of the small kinetic mixing with hypercharge. This scenario provides a robust framework to search for a light dark sector via searches for heavy colored particles at the LHC.Some of the most important searches for Beyond the Standard Model (BSM) physics at the Large Hadron Collider (LHC) are searches for new vector like quarks (VLQs). Up-type VLQs, so-called top partners T , are ubiquitous in composite [1][2][3][4][5][6][7] and Little Higgs [8][9][10][11][12][13][14][15] models where new fermionic top partners help solve the hierarchy problem. Traditionally, searches for VLQs rely on decays into the Standard Model (SM) electroweak (EW) bosons: W/Z/Higgs. However, there is a a class of "maverick top partners" with non-traditional decays into photons [16][17][18][19][20][21], gluons [16][17][18][19][20][21], new scalars [22][23][24][25], etc. These new decays can easily be dominant with minor tweaks to the simplest VLQ models. We consider a VLQ that is charged under both the SM and a new abelian gauge symmetry U (1) d , where the SM is neutral under the U (1) d . As we will show, for a very large range of parameter space, this opens new dominant decays of VLQs that have not yet been searched for.This new U (1) d can be motivated by noting that dark matter may very well have selfinteractions through this new force. The U (1) d gauge boson, the so-called dark photon, kinetically mixes with the SM hypercharge through a renormalizable interaction [26][27][28]. This kinetic mixing can be generated via new vector like fermions charged under both the SM and the new U (1) d [26,29,30], as considered here. In the limit that the dark photon is much less massive than the Z and the kinetic mixing is small, the dark photon inherits couplings to SM particles of the form ε J µ EM , where J µ EM is the electromagnetic current and ε is the kinetic mixing parameter. Hence, the name dark photon. Most of the searches for the dark photon...