In this paper, we consider the pseudo‐relativistic Hartree equation
i∂tψ=−△+m2ψ−1|x|∗|ψ|2ψonℝ3
and study travelling solitary waves of the form ψ(t, x) = eitμφ(x − v t) , where
v∈ℝ3 denotes travelling velocity. Fröhlich, Jonsson and Lenzmann in [Comm. Math. Phys. 2007, 274:1‐30] proved that for |v|<1 there exists a critical constant Nc(v), such that the travelling waves exist if and only if 0 < N < Nc(v), where N denotes particle number. In this paper, we consider
v=false(β,0,0false) with 0 < β < 1, and let
Ncfalse(βfalse)=Ncfalse(vfalse)false|v=false(β,0,0false). We find that Nc(β) is Lipschitz continuity with respect to β. Based on this fact, we then prove that the boosted ground states φβ with
false‖φβfalse‖L22=false(1−βfalse)Ncfalse(βfalse) satisfy
limβ→0+false‖φβfalse‖H1false/2→+∞. The explicit blow‐up profile and rate will be computed.