($\epsilon_\text{max} \gtrsim 10^{-4} \text{ GeV}$): Decays in this case occur at an indistinguishable distance from the collision point at an LHC detector.

The physics associated with non-prompt decays is mostly dependent on the mass of the squark (through its production) and its decay length (displaced vertices or collider stable squarks). Such probes would not be the ideal way of studying the specific branching ratios of the squarks predicted in the model under consideration. In addition such signals have already been analyzed in the references above. We therefore continue this paper considering prompt squark LSP decays only. As we shall see, this will intimately relate the neutrino sector to $R$-parity violation.

The existence of this relationship is already suggested by Eqs. (\[W.brpv\]) and (\[L.n\]). These RPV bilinear terms mix fields with different $R$-parity number but the same spin and SM quantum numbers. Specifically, the neutrinos now mix with the neutralinos, Eq. (\[neutralino\]), the charged leptons mix with the charginos, Eq. (\[chargino\]) and the Higgs fields mix with the sleptons. The neutrino/neutralino mixings are crucial because they generate tree-level Majorana neutrino masses through a seesaw mechanism. As a result of this, the bilinear $R$-parity violating terms cannot be too large. All $R$-parity 