It is shown using dimensional analysis that the maximum current density JQCL transported on application of a voltage Vg across a gap of size D follows the relation JQCL ∼ 3−2α V α g /D 5−2α . The classical Child-Langmuir result is recovered at α = 3/2 on demanding that the scaling law be independent of . For a nanogap in the deep quantum regime, additional inputs in the form of appropriate boundary conditions and the behaviour of the exchange-correlation potential show that α = 5/14. This is verified numerically for several nanogaps. It is also argued that in this regime, the limiting mechanism is quantum reflection from a downhill potential due to a sharp change in slope seen by the electron on emerging through the barrier.