studied for quasiholes in the spin-polarized $\nu = 5/2$ quantum Hall state [@moore-read; @nayak-wilczek]. Therefore, if we want to obtain the same statistics for vortices in a spinful superconductor, the vortices should be HQVs so that there would be phase winding only for a single component.

However, while there are a number of candidate triplet superconductors such as the single layer ruthenate Sr$_2$RuO$4$ [@Maeno:1994fk; @RevModPhys.75.657], the cobaltate Na$_x$CoO$_2 \cdot y$H$_2$O [@Nature.Physics.1.91] and organic superconductors [@organic], HQV’s have never been observed in bulk systems, in line with the energetic stability issues raised by two of us in Ref. . It was pointed out in Ref.  due to the absence of screening for the spin supercurrent circulation required for HQV in triplet superconductors, HQV’s can be energetically unstable in bulk samples towards combining into full Abrikosov vortices despite their advantage in magnetic energy. Related considerations have appeared in the context of spin-triplet superconductivity in UPt$_3$ by Zhitomirsky [@Zhitomirskii_UPt3].

The main motivation of this work is to investigate the possibility of using high enough fields to generate a HQV lattice in triplet superconductors where the vortex lattice serves two purposes at once: 1) stabilizing HQV’s at finite separation 2) providing an unambiguous signature 